TW202242518A - Electrochromic devices, the precursor thereof, and method and apparatus of fabricating the same - Google Patents

Electrochromic devices, the precursor thereof, and method and apparatus of fabricating the same Download PDF

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TW202242518A
TW202242518A TW111125592A TW111125592A TW202242518A TW 202242518 A TW202242518 A TW 202242518A TW 111125592 A TW111125592 A TW 111125592A TW 111125592 A TW111125592 A TW 111125592A TW 202242518 A TW202242518 A TW 202242518A
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layer
electrochromic
counter electrode
lithium
electrically insulating
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王仲春
安殊 普拉達
羅伯特 羅茲畢基
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美商唯景公司
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Priority claimed from US12/772,055 external-priority patent/US8300298B2/en
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    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/15Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect
    • G02F1/153Constructional details
    • G02F1/155Electrodes
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/15Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect
    • G02F1/1514Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material
    • G02F1/1523Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material comprising inorganic material
    • G02F1/1525Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material comprising inorganic material characterised by a particular ion transporting layer, e.g. electrolyte
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/15Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect
    • G02F1/1514Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material
    • G02F1/1523Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on an electrochromic effect characterised by the electrochromic material, e.g. by the electrodeposited material comprising inorganic material
    • G02F1/1524Transition metal compounds

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  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Electrochemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Electrochromic Elements, Electrophoresis, Or Variable Reflection Or Absorption Elements (AREA)

Abstract

Conventional electrochromic devices frequently suffer from poor reliability and poor performance. Improvements are made using entirely solid and inorganic materials. Electrochromic devices are fabricated by forming an ion conducting electronically insulating interfacial region that serves as an IC layer. In some methods, the interfacial region is formed afterformation of an electrochromic and a counter electrode layer. The interfacial region contains an ion conducting electronically insulating material along with components of the electrochromic and/or the counter electrode layer. Materials and microstructure of the electrochromic devices provide improvements in performance and reliability over conventional devices.

Description

電致變色裝置,其前驅物及製造其之方法及設備Electrochromic device, its precursor and method and equipment for its manufacture

本發明係關於一種電致變色裝置、一種電致變色裝置前驅物,及一種用於製造電致變色裝置之方法及設備。The present invention relates to an electrochromic device, a precursor of the electrochromic device, and a method and equipment for manufacturing the electrochromic device.

電致變色為一種現象,其中材料在處於不同電子能態下(通常藉由經受電壓變化)時展現光學性質上的可逆之以電化學為媒介之變化。光學性質通常為色彩、透射率、吸光度及反射率中之一或多者。舉例而言,一種熟知電致變色材料為氧化鎢(WO 3)。氧化鎢為陰極電致變色材料,其中藉由電化學還原而發生著色過渡(藍色可透過)。 電致變色材料可併入至(例如)窗及鏡子中。此等窗及鏡子之色彩、透射率、吸光度及/或反射率可藉由誘發電致變色材料之變化來改變。舉例而言,電致變色材料之一個熟知應用為一些汽車中之後視鏡。在此等電致變色後視鏡中,鏡子之反射率在夜間改變,使得其他車輛之前照燈不分散駕駛者之注意力。 儘管電致變色係在1960年代發現,但遺憾地,電致變色裝置仍遭受各種問題且尚未開始實現其全部商業潛能。需要電致變色技術、設備及製造及/或使用該等設備之相關方法之進步。 Electrochromism is a phenomenon in which a material exhibits a reversible, electrochemically mediated change in optical properties when placed in a different electronic energy state, usually by being subjected to a voltage change. Optical properties are typically one or more of color, transmittance, absorbance, and reflectance. For example, one well-known electrochromic material is tungsten oxide (WO 3 ). Tungsten oxide is a cathodic electrochromic material in which the color transition (blue transmission) occurs by electrochemical reduction. Electrochromic materials can be incorporated into, for example, windows and mirrors. The tint, transmittance, absorbance and/or reflectance of these windows and mirrors can be changed by inducing changes in the electrochromic material. For example, one well-known application of electrochromic materials is in some automobile mid-view mirrors. In these electrochromic rearview mirrors, the reflectivity of the mirror changes at night so that the headlights of other vehicles do not distract the driver. Despite the discovery of the electrochromic system in the 1960's, unfortunately, electrochromic devices still suffer from various problems and have not yet begun to realize their full commercial potential. There is a need for advances in electrochromic technology, devices, and related methods of making and/or using such devices.

典型電致變色裝置包括由對離子高度傳導且對電子高度抵抗之離子傳導(「IC」)層分離的電致變色(「EC」)電極層及對向電極(「CE」)層。換言之,該離子傳導層准許離子之輸送,但阻斷電流。如通常所理解,該離子傳導層因此防止該電致變色層與該對向電極層之間的短路。該離子傳導層允許電致變色電極及對向電極保持電荷,且藉此維持其褪色狀態或著色狀態。在習知電致變色裝置中,該等組件形成堆疊,其中該離子傳導層夾在該電致變色電極與該對向電極之間。此等三個堆疊組件之間的邊界由組成及/或微結構之突然變化界定。因此,該等裝置具有具兩個突變界面之三個相異層。 相當令人吃驚地,發明者已發現,可在不沈積離子傳導電絕緣層之情況下製造高品質電致變色裝置。根據特定實施例,對向電極及電致變色電極係在不分離地沈積離子傳導層之情況下彼此緊接鄰近地形成(常常直接接觸)。咸信,各種製造程序及/或物理或化學機制在接觸之電致變色層與對向電極層之間產生界面區,且此界面區起到習知裝置中之離子傳導電絕緣層的至少一些功能。下文描述可能為形成界面區之關鍵之特定機制。 該界面區通常(儘管不必)具有包括由不同相及/或組成表示之至少兩種離散組份之異質結構。此外,該界面區可包括此等兩種或兩種以上離散組份中之梯度。該梯度可提供(例如)可變之組成、微結構、電阻率、摻雜劑濃度(例如,氧濃度)及/或化學計量。 除了以上發現之外,發明者還觀察到,為了改良裝置可靠性,可製造電致變色裝置之兩個層(電致變色(EC)層及對向電極(CE)層)以使其各自包括已定義量之鋰。另外,電致變色裝置之一些組件之材料及形態及/或微結構之小心選擇提供效能及可靠性之改良。在一些實施例中,裝置之所有層全部為固體且無機的。 與以上觀察及發現一致,發明者已發現,EC-IC-CE堆疊之形成無需以習知序列(EC→IC→CE或CE→IC→EC)進行,而可在電致變色層及對向電極層之形成之後形成充當IC層的離子傳導電絕緣區。亦即,首先形成EC-CE(或CE-EC)堆疊,接著在EC層及CE層之界面處使用該等層中之一者或兩者之組份在EC層與CE層之間形成起到IC層之一些用途之界面區。本發明之方法不僅藉由消除一或多個處理步驟而減少製造複雜性及費用,且提供展示改良之效能特性之裝置。 因此,本發明之一態樣為一種製造電致變色裝置之方法,該方法包括:形成包括電致變色材料之電致變色層;形成與該電致變色層接觸之對向電極層,而並不首先在該電致變色層與該對向電極層之間提供離子傳導電絕緣層;及在該電致變色層與該對向電極層之間形成界面區,其中該界面區為實質上離子傳導且實質上電絕緣的。該電致變色層及該對向電極層通常(但不必)由比該界面區導電性更強但可能具有一定抗電子特性之一或多種材料製成。該界面區可含有該EC層及/或該CE層之組份材料,且在一些實施例中,該EC層及該CE層含有該界面區之組份材料。在一實施例中,該電致變色層包括WO 3。在一些實施例中,該EC層包括WO 3,該CE層包括氧化鎳鎢(NiWO),且該IC層包括鎢酸鋰(Li 2WO 4)。 可在該電致變色層之至少一部分之沈積期間應用加熱。在一實施例中,在該EC層包括WO 3之情況下,在經由濺鍍進行之一系列沈積中之每一者之後應用加熱以便形成具有實質上多晶微結構之EC層。在一實施例中,該電致變色層之厚度在約300 nm與約600 nm之間,但該厚度可取決於預期在沈積該EC-CE堆疊之後形成該界面區之所要結果而改變。在一些實施例中,WO 3為實質上多晶的。在一些實施例中,可使用WO 3之富氧層作為該界面區之前驅物。在其他實施例中,該WO 3層為層中具有變化之氧濃度之分級層。在一些實施例中,鋰為用於驅動電致變色過渡之較佳離子種類,且描述了堆疊或層鋰化方案。形成參數及層特性之詳細內容將在下文予以更詳細地描述。 本發明之另一態樣為一種製造電致變色裝置之方法,該方法包括:(a)形成包括電致變色材料之電致變色層或包括對向電極材料之對向電極層;(b)在該電致變色層或該對向電極層上方形成中間層,其中該中間層包括該電致變色材料、該對向電極材料及額外材料中之至少一者之富氧形式,其中該額外材料包括相異之電致變色材料及/或對向電極材料,該中間層不為實質上電絕緣的;(c)形成該電致變色層及該對向電極層中之另一者;及(d)允許該中間層之至少一部分變得實質上電絕緣及實質上離子傳導。用於此方法之形成參數及層特性之詳細內容亦將在下文予以更詳細地描述。 本發明之另一態樣為一種用於製造電致變色裝置之設備,其包括:整合式沈積系統,其包括:(i)含有材料源之第一沈積台,其經配置以沈積包括電致變色材料之電致變色層;及(ii)第二沈積台,其經配置以沈積包括對向電極材料之對向電極層;及控制器,其含有用於以在基板上順序地沈積堆疊之方式傳遞該基板經過該第一沈積台及該第二沈積台之程式指令,該堆疊具有夾在該電致變色層與該對向電極層之間的中間層;其中該第一沈積台及該第二沈積台中之任一者或兩者亦經配置以在該電致變色層或該對向電極層上方沈積該中間層,且其中該中間層包括該電致變色材料或該對向電極材料之富氧形式,且其中該第一沈積台及該第二沈積台串聯互連且可操作以將基板自一個台傳遞至下一個台而不將該基板曝露於外部環境。在一實施例中,本發明之設備可操作以將該基板自一個台傳遞至下一個台而不破壞真空,且可包括可操作以將來自含鋰材料源之鋰沈積在該電致變色裝置之一或多個層上之一或多個鋰化台。在一實施例中,本發明之設備可操作以在建築玻璃基板上沈積該電致變色堆疊。本發明之設備無需具有用於製造離子傳導層之單獨標靶。 本發明之另一態樣為一種電致變色裝置,其包括:(a)包括電致變色材料之電致變色層;(b)包括對向電極材料之對向電極層;及(c)在該電致變色層與該對向電極層之間的界面區,其中該界面區包括電絕緣離子傳導材料及該電致變色材料、該對向電極材料及額外材料中之至少一者,其中該額外材料包括相異之電致變色材料及/或對向電極材料。在一些實施例中,未包括該額外材料;在此等實施例中,該界面區包括該電致變色材料及該對向電極材料中之至少一者。該界面區之組成及形態及/或微結構之變化將在本文中予以更詳細地描述。本文中所描述之電致變色裝置可併入至窗(在一實施例中,建築玻璃鱗片窗(glass scale window))中。 本發明之此等及其他特徵及優點將參看相關聯圖式在下文予以更詳細地描述。 A typical electrochromic device includes an electrochromic ("EC") electrode layer and a counter electrode ("CE") layer separated by an ion-conducting ("IC") layer that is highly conductive to ions and highly resistant to electrons. In other words, the ionically conductive layer permits transport of ions but blocks electrical current. As generally understood, the ion-conducting layer thus prevents short circuits between the electrochromic layer and the counter electrode layer. The ion-conducting layer allows the electrochromic electrode and counter electrode to retain charge, and thereby maintain their faded or colored state. In conventional electrochromic devices, the components form a stack with the ion-conducting layer sandwiched between the electrochromic electrode and the counter electrode. The boundaries between these three stacked components are defined by abrupt changes in composition and/or microstructure. Thus, the devices have three distinct layers with two abrupt interfaces. Quite surprisingly, the inventors have discovered that high quality electrochromic devices can be fabricated without depositing an ion-conducting electrically insulating layer. According to a particular embodiment, the counter electrode and the electrochromic electrode are formed in close proximity to each other (often in direct contact) without separately depositing the ion-conducting layer. It is believed that various fabrication procedures and/or physical or chemical mechanisms create an interfacial region between the contacting electrochromic layer and the counter electrode layer, and that this interfacial region acts as at least some of the ion-conducting electrically insulating layers in conventional devices Function. Specific mechanisms that may be key to the formation of the interfacial region are described below. The interfacial region typically, though not necessarily, has a heterostructure comprising at least two discrete components represented by different phases and/or compositions. Additionally, the interfacial region may include gradients among these two or more discrete components. The gradient can provide, for example, variable composition, microstructure, resistivity, dopant concentration (eg, oxygen concentration), and/or stoichiometry. In addition to the above findings, the inventors have also observed that in order to improve device reliability, the two layers of an electrochromic device (the electrochromic (EC) layer and the counter electrode (CE) layer) can be fabricated so that each includes Lithium in defined quantities. Additionally, careful selection of materials and morphology and/or microstructure of some components of an electrochromic device provides improvements in performance and reliability. In some embodiments, all layers of the device are solid and inorganic. Consistent with the above observations and findings, the inventors have discovered that the formation of the EC-IC-CE stack does not need to proceed in the conventional sequence (EC→IC→CE or CE→IC→EC), but can be done in the electrochromic layer and the opposite Formation of the electrode layer is followed by the formation of an ionically conductive electrically insulating region that acts as the IC layer. That is, first an EC-CE (or CE-EC) stack is formed, then a stack is formed between the EC layer and the CE layer at the interface of the EC layer and the CE layer using components of either or both of these layers. To the interface area of IC layer for some purposes. The method of the present invention not only reduces manufacturing complexity and cost by eliminating one or more processing steps, but also provides devices exhibiting improved performance characteristics. Therefore, one aspect of the present invention is a method of manufacturing an electrochromic device, the method comprising: forming an electrochromic layer including an electrochromic material; forming a counter electrode layer in contact with the electrochromic layer, and without first providing an ionically conductive electrically insulating layer between the electrochromic layer and the counter electrode layer; and forming an interface region between the electrochromic layer and the counter electrode layer, wherein the interface region is substantially ionic Conductive and substantially electrically insulating. The electrochromic layer and the counter electrode layer are typically (but not necessarily) made of one or more materials that are more conductive than the interfacial region but may have some electron-resistant properties. The interfacial region can contain constituent materials of the EC layer and/or the CE layer, and in some embodiments, the EC layer and the CE layer contain constituent materials of the interfacial region. In one embodiment, the electrochromic layer includes WO 3 . In some embodiments, the EC layer includes WO 3 , the CE layer includes nickel tungsten oxide (NiWO), and the IC layer includes lithium tungstate (Li 2 WO 4 ). Heating may be applied during deposition of at least a portion of the electrochromic layer. In one embodiment, where the EC layer comprises WO 3 , heating is applied after each of a series of depositions by sputtering in order to form an EC layer with a substantially polycrystalline microstructure. In one embodiment, the thickness of the electrochromic layer is between about 300 nm and about 600 nm, but the thickness can vary depending on the desired result of forming the interfacial region expected after depositing the EC-CE stack. In some embodiments, WO 3 is substantially polycrystalline. In some embodiments, an oxygen-rich layer of WO 3 may be used as a precursor to the interfacial region. In other embodiments, the WO 3 layer is a graded layer with varying oxygen concentration in the layer. In some embodiments, lithium is the preferred ion species for driving the electrochromic transition, and a stack or layer lithiation scheme is described. Details of the formation parameters and layer properties are described in more detail below. Another aspect of the present invention is a method of manufacturing an electrochromic device, the method comprising: (a) forming an electrochromic layer comprising an electrochromic material or a counter electrode layer comprising a counter electrode material; (b) An intermediate layer is formed over the electrochromic layer or the counter electrode layer, wherein the intermediate layer includes an oxygen-enriched form of at least one of the electrochromic material, the counter electrode material, and an additional material, wherein the additional material comprising a dissimilar electrochromic material and/or counter electrode material, the intermediate layer is not substantially electrically insulating; (c) forming the other of the electrochromic layer and the counter electrode layer; and ( d) allowing at least a portion of the intermediate layer to become substantially electrically insulating and substantially ionically conductive. Details of the formation parameters and layer characteristics used in this method will also be described in more detail below. Another aspect of the present invention is an apparatus for fabricating an electrochromic device comprising: an integrated deposition system comprising: (i) a first deposition station containing a source of material configured to deposit materials including electrochromic an electrochromic layer of a color-changing material; and (ii) a second deposition station configured to deposit a counter electrode layer comprising a counter electrode material; and a controller containing a transfer the substrate through the program instructions of the first deposition station and the second deposition station, the stack has an intermediate layer sandwiched between the electrochromic layer and the counter electrode layer; wherein the first deposition station and the Either or both of the second deposition stations are also configured to deposit the intermediate layer over the electrochromic layer or the counter electrode layer, and wherein the intermediate layer includes the electrochromic material or the counter electrode material and wherein the first deposition station and the second deposition station are interconnected in series and are operable to transfer a substrate from one station to the next without exposing the substrate to the external environment. In one embodiment, the apparatus of the present invention is operable to transfer the substrate from one station to the next without breaking vacuum, and may include operable to deposit lithium from a source of lithium-containing material on the electrochromic device. One or more lithiation sites on one or more layers. In one embodiment, the apparatus of the present invention is operable to deposit the electrochromic stack on an architectural glass substrate. The apparatus of the present invention need not have a separate target for making the ion-conducting layer. Another aspect of the present invention is an electrochromic device comprising: (a) an electrochromic layer comprising an electrochromic material; (b) a counter electrode layer comprising a counter electrode material; and (c) an electrochromic layer comprising an electrochromic material; The interface region between the electrochromic layer and the counter electrode layer, wherein the interface region includes an electrically insulating ion-conducting material and at least one of the electrochromic material, the counter electrode material, and an additional material, wherein the Additional materials include dissimilar electrochromic materials and/or counter electrode materials. In some embodiments, the additional material is not included; in these embodiments, the interface region includes at least one of the electrochromic material and the counter electrode material. Variations in the composition and morphology and/or microstructure of the interfacial region are described in more detail herein. The electrochromic devices described herein can be incorporated into windows (in one embodiment, architectural glass scale windows). These and other features and advantages of the present invention will be described in more detail below with reference to the associated drawings.

本發明主張各自於2010年4月30日申請且題為「電致變色裝置(Electrochromic Devices)」之美國申請案第12/772,055號及第12/772,075號之權利及優先權,該等申請案中之每一者係以全文引用方式併入。 以下詳細描述可在結合圖式考慮時得到更全面理解。 圖1A為描繪習知電致變色裝置堆疊100之示意性橫截面。電致變色裝置100包括基板102、導電層(CL)104、電致變色(EC)層106、離子傳導(IC)層108、對向電極(CE)層110及導電層(CL)112。將元件104、106、108、110及112共同稱為電致變色堆疊114。通常,該等CL層係由透明導電氧化物製成,且通常被稱為「TCO」層。由於TCO層為透明的,故EC-IC-CE堆疊之著色行為可(例如)經由TCO層觀測,從而允許在窗上使用此等裝置以獲得可逆遮光。可操作以跨電致變色堆疊114施加電位之電壓源116實現電致變色裝置自(例如)褪色狀態(亦即,透明)至著色狀態之過渡。該等層之次序相對於基板可顛倒。亦即,該等層可處於以下次序:基板、透明導電層、對向電極層、離子傳導層、電致變色材料層及(另一)透明導電層。 再次參看圖1A,在製造電致變色堆疊之習知方法中,個別層係以如圖1A之左側之示意圖中所描繪之順序格式沈積在另一層之上。亦即,TCO層104沈積在基板102上。接著,EC層106沈積在TCO 104上。接著,IC層108沈積在EC層106上,繼之以CE層110沈積在IC層108上,且最後TCO層112沈積在CE層110上以形成電致變色裝置100。當然,步驟之次序可顛倒以形成「反向」堆疊,但要點在於,在習知方法中,IC層必須沈積在EC層上、繼之以CE層沈積在IC層上,或IC層沈積在CE層上、繼之以EC層沈積在IC層上。堆疊中之材料層之間的過渡為突然的。 以上程序之一顯著挑戰為形成IC層所需之處理。在一些先前方法中,IC層係藉由難以併入至用以形成EC層及CE層之CVD或PVD製程中之溶膠凝膠製程形成。此外,藉由溶膠凝膠及其他基於液體之製程產生之IC層易於具有降低裝置之品質且可能需要藉由(例如)雕刻移除之缺陷。在其他方法中,IC層係藉由PVD自可能難以製造及使用之陶瓷標靶沈積。 圖1B為描繪材料%組成對圖1A之電致變色堆疊中之位置(即層106、108及110,亦即,EC層、IC層及CE層)的曲線圖。如所提及,在習知電致變色堆疊中,堆疊中之材料層之間的過渡為突然的。舉例而言,EC材料106經沈積為相異層而很少或沒有至鄰近IC層之組合物滲流。類似地,IC材料108及CE材料110在組成上相異而很少或沒有至鄰近層之滲流。因此,該等材料為實質上均質的(下文所描述之CE材料之特定組合物除外)且具有突變界面。習知思想為該三個層中之每一者應作為相異之均勻沈積且平滑之層而敷設以形成堆疊。每一層之間的界面應為「清楚的」,其中界面處存在來自每一層之材料之很少互混。 一般熟習此項技術者可認識到,圖1B為理想化描繪,且在實踐意義上,層界面處存在一定程度上不可避免的材料混合。要點在於,在習知製造方法中,任何此混合為非故意且最少的。發明者已發現,可形成充當IC層之界面區,其中界面區有意包括大量的一或多種電致變色材料及/或對向電極材料。此為自習知製造方法之根本偏離。 如上文所提及,發明者已發現,EC-IC-CE堆疊之形成不必以習知序列(EC→IC→CE或CE→IC→EC)進行,而是可在電致變色層及對向電極層之沈積之後形成充當離子傳導層之界面區域。亦即,首先形成EC-CE(或CE-EC)堆疊,接著,在該等層之界面處使用該等層(在一些實施例中,及/或另一電致變色材料或對向電極材料)中之一者或兩者之組份在EC層與CE層之間形成界面區(其可擁有IC層之至少一些功能)。該界面區起到習知IC層之至少一些功能,此係因為該界面區為實質上離子傳導且實質上電絕緣的。然而,應注意,如所描述之界面區可具有高於習知所接受之漏電流的漏電流,但儘管如此,該等裝置展示良好效能。 在一實施例中,電致變色層經形成而具有富氧區,該富氧區在沈積對向電極層之後在後續處理時轉換成充當IC層之界面區或層。在一些實施例中,使用包括電致變色材料之富氧型式之相異層來(最終)在EC層與CE層之間形成充當IC層之界面層。在其他實施例中,使用包括對向電極材料之富氧型式之相異層來(最終)在EC層與CE層之間形成充當IC層之界面區。該富氧CE層之全部或一部分經轉換成界面區。在其他實施例中,使用包括對向電極材料之富氧型式及電致變色材料之富氧形式之相異層來(最終)在EC層與CE層之間形成充當IC層之界面區。換言之,富氧材料之一些或全部充當該充當IC層之界面區之前驅物。本發明之方法不僅可減少處理步驟,而且產生展示改良之效能特性之電致變色裝置。 如所提及,咸信,界面區中之EC層及/或CE層之一些經轉換成提供IC層之一或多個功能(特別是對離子之高傳導性及對電子之高電阻率)之材料。界面區中之IC功能性材料可為(例如)導電陽離子之鹽;例如,鋰鹽。 圖2A、圖2B及圖2C展示電致變色裝置堆疊(各自含有EC層、CE層及充當IC層之界面區)之三個可能實例之組成曲線圖,其中EC材料為氧化鎢(此處表示為WO 3,但意欲包括WO x ,其中 x在約2.7與約3.5之間,在一實施例中, x在約2.7與約2.9之間),CE材料為氧化鎳鎢(NiWO),且界面區主要包含鎢酸鋰(此處表示為Li 2WO 4,在另一實施例中,界面區為在約0.5%與約50(原子)%之間的Li 2O、在約5%與約95%之間的Li 2WO 4及約5%與約70%之間的WO 3之奈米複合材料)及某一量之EC材料及/或CE材料。更一般言之,界面區通常(但不必)具有包括由不同相及/或組成表示之至少兩個離散組份之異質結構,該等相或組成之濃度在界面區之寬度上變化。由於此原因,本文中有時將充當IC層之界面區稱為「梯度區」、「異質IC層」或「分散式IC層」。雖然關於特定材料加以描述,但圖2A、圖2B及圖2C中之說明更一般地表示用於本發明之電致變色裝置之任何合適材料之組成變化。 圖2A描繪本發明之電致變色堆疊,其中EC材料為充當IC層之界面區之重要組份,而CE材料並非重要組份。參看圖2A,自原點開始且沿著 x軸自左向右移動,吾人可看到,一部分EC材料WO 3(其實質上全部為氧化鎢)充當EC層。存在至界面區中之過渡,其中存在逐漸減少之氧化鎢及對應地逐漸增加之鎢酸鋰,直至且包括靠近界面區之末端,在該末端處,存在具有某一最小量之氧化鎢之實質上全部為鎢酸鋰之部分。雖然自EC層至界面區之過渡以實質上全部氧化鎢及最小量之鎢酸鋰之組合物來區分,但顯而易見,該過渡不像習知裝置中一樣突然。在此實例中,實際上,該過渡在該組合物具有足夠量之鎢酸鋰之情況下開始發生以使該材料能夠起到IC層之至少一些功能,例如,離子傳導及電絕緣。無疑,更接近CE層之組合物(其中該組合物實質上為鎢酸鋰)起到IC層之功能,此係因為已知鎢酸鋰展現此等性質。但在界面區之其他部分中亦存在一定IC層功能。發明者已發現,與具有突然過渡之習知裝置相比,此等「異質IC層」改良電致變色裝置之切換特性及可能之熱循環穩定性。此實例中之CE層主要含有氧化鎳鎢作為活性材料,且具有至界面區之邊緣處之氧化鎳鎢組合物的相對突然過渡。用於製造具有此等界面區之堆疊之方法將在下文予以更詳細描述。 應注意,例如,圖2A中之氧化鎳鎢CE層經描繪為具有約20%之鎢酸鋰。不希望受理論限制,咸信,氧化鎳鎢CE層作為由鎢酸鋰之外殼或基質環繞之氧化鎳核心或粒子(其將相當良好之離子傳導率賦予CE層)而存在,且藉此在電致變色堆疊之操作期間幫助CE層之電致變色過渡。CE層中之鎢酸鋰之確切化學計量可在實施例之間顯著改變。在一些實施例中,CE層中亦可能存在一些氧化鎢。又,因為鋰離子經由充當IC層之界面區而至及自EC層及CE層行進,所以EC層中可能存在大量鎢酸鋰,例如,如圖2A中所描繪。 圖2B描繪本發明之電致變色堆疊,其中CE材料為充當IC層之界面區之重要組份,而EC材料並非重要組份。參看圖2B,自原點開始且沿著 x軸自左向右移動,吾人可看到,在此情況下,實質上全部為氧化鎢之EC材料充當EC層。存在至界面區中之突然過渡,該界面區中存在很少(若存在)氧化鎢,但存在大量鎢酸鋰及至少一些氧化鎳鎢(CE材料)。該界面區之組合物沿著 x軸以逐漸減少之鎢酸鋰及對應之逐漸增多之氧化鎳鎢變化。自界面區至CE層之過渡以約80%之氧化鎳鎢及約20%之鎢酸鋰之組合物任意地區分,但此僅為過渡以分級組合物發生之情況之一實例。當在對堆疊進行進一步處理時無或很少有組合物之額外變化發生時,界面區可視為終止。另外,過渡實際上在組合物具有足夠量之氧化鎳鎢之情況下終止,以使得該材料不再起到相異IC層可起到之至少某一功能。無疑,更接近CE層之組合物(如所區分)(其中組合物為80%之氧化鎳鎢)起到CE層之功能。同樣地,更接近EC層之界面區之組合物(其中鎢酸鋰為實質組份)充當離子傳導電絕緣材料。 圖2C描繪本發明之電致變色堆疊,其中EC材料及CE材料均為充當IC層之界面區的重要組份。參看圖2C,自原點開始且沿著 x軸自左向右移動,吾人可看到,一部分EC材料WO 3(其實質上全部為氧化鎢)充當EC層。存在至界面區中之過渡,其中存在逐漸減少之氧化鎢及對應地逐漸增多之鎢酸鋰。在此實例中,在通過區分為界面區之部分之路途的三分之一附近,亦存在增長量之氧化鎳鎢對向電極材料。在通過區分為界面區之部分的約中間位置處,存在各自約10%之氧化鎢及氧化鎳鎢及80%之鎢酸鋰。在此實例中,EC層與IC層之間或IC層與CE層之間不存在突然過渡,而是存在具有CE材料及EC材料兩者之連續分級組合物之界面區。在此實例中,鎢酸鋰組份在通過界面區之約中間處出現峰值,且因此,此區很可能為界面區之最強電絕緣部分。 如以上[發明內容]中所提及,EC層及CE層可包括將某一電阻率賦予EC層及CE層之材料組份;圖2A至圖2C中所描述之至少以某一量跨越所有三個區之鎢酸鋰為將電阻率賦予EC層及CE層之此等材料之一實例。 圖2A至圖2C僅表示本發明之電致變色裝置中之充當IC層之界面區之分級組合物的三個非限制性實例。一般熟習此項技術者將瞭解,在不脫離本發明之範疇的情況下,許多變化係可能的。在圖2A至圖2C中之實例之每一者中,存在至少一層,其中僅存在兩種材料組份且該等組份中之一者為最少的。本發明不限於此方式。因此,本發明之一實施例為一種電致變色裝置,其包括電致變色層、充當IC層之界面區,及對向電極層,其中該裝置之前述兩個層及一個區中之每一者之至少一材料組份以如下量存在於該電致變色層、該界面區及該對向電極層中之每一者中:至少約25重量%,在另一實施例中,至少約15重量%,在另一實施例中,至少約10重量%,在另一實施例中,至少約5重量%,在又一實施例中,至少約2重量%。 界面區中之電致變色材料及/或對向電極材料之量可為顯著的,在一實施例中,多達界面區之50重量%。然而,在許多實施例中,離子傳導電絕緣材料通常為多數組份,而界面區之剩餘部分為電致變色材料及/或對向電極材料。在一實施例中,界面區包括在約60重量%與約95重量%之間的離子傳導電絕緣材料,而界面區之剩餘部分為電致變色材料及/或對向電極材料。在一實施例中,界面區包括在約70重量%與約95重量%之間的離子傳導電絕緣材料,而界面區之剩餘部分為電致變色材料及/或對向電極材料。在一實施例中,界面區包括在約80重量%與約95重量%之間的離子傳導電絕緣材料,而界面區之剩餘部分為電致變色材料及/或對向電極材料。 在一些實施例中,本文中所描述之裝置中之界面區可為相對相異的,亦即,當(例如)藉由顯微鏡分析時,鄰接層處存在相對可區別之邊界,即使界面區含有某一量之電致變色材料及/或對向電極材料亦如此。在此等實施例中,可量測界面區之厚度。在界面區係由EC層及/或CE層之富氧(超化學計量)區形成之實施例中,界面區之厚度與形成界面區之該層或該等層之比為用於特性化界面區之一量度。舉例而言,電致變色層經沈積具有富氧上層。EC層可包括單一金屬氧化物或在層或更多擴散區中均質或異質地混合之兩種或兩種以上金屬氧化物。EC層為550 nm厚,其包括富氧層(或區)。若EC層之約150 nm經轉換成界面區,則EC之約27%經轉換成界面區,亦即,150 nm除以550 nm。在另一實例中,EC層包括第一金屬氧化物區(或層)及富氧之第二金屬氧化物層(或區)。若富氧金屬氧化物層之全部或一部分經轉換成界面區,則界面區之厚度除以該第一金屬氧化物層及該第二金屬氧化物層之總厚度(在形成界面區之前)為界面區之量度。在一實施例中,界面區包括以厚度計約0.5%與約50%之間的用以形成界面區之前驅物區(EC及/或CE,包括富氧部分),在另一實施例中在約1%與約30%之間,在又一實施例中在約2%與約10%之間,且在另一實施例中在約3%與約7%之間。 發明者已發現,分級組合物充當IC層具有許多益處。儘管不希望受理論限制,但咸信,藉由具有此等分級區,電致變色過渡之效率得到大大改良。如下文將更詳細描述,存在其他益處。 儘管不希望束縛於理論,但咸信,以下機制中之一或多者可實現EC及/或CE材料至界面區中之IC功能性材料之轉化。然而,本發明之執行或應用並不限於此等機制中之任一者。此等機制中之每一者與在堆疊之製造期間絕不沈積IC層材料之製程一致。如本文中其他處清楚表示,本發明之設備無需具有包含用於IC層之材料之單獨標靶。 在第一機制中,電致變色材料或對向電極材料之直接鋰化產生界面區中之IC材料(例如,鎢酸鋰)。如下文將更充分解釋,各種實施例在EC層及CE層之形成之間的製造程序中之某時刻使用該等作用層中之一者之直接鋰化。此操作涉及EC層或CE層(首先形成者)於鋰之曝露。根據此機制,通過EC或CE層之鋰之通量產生離子傳導之抵抗電子之材料,諸如,鋰鹽。可施加熱或其他能量以驅動鋰之此通量。所描述之此機制在形成第二層(CE或EC層)之前轉換首先形成之層(EC或CE層)之頂部或曝露部分。 在第二機制中,自EC或CE中之一者擴散至另一層之鋰在兩個層皆已形成之後及/或在經鋰化之第一層上形成第二層期間導致EC及/或CE中之一者之部分在其界面處轉換至具有IC功能材料之界面區。該鋰擴散可在整個該第二層已形成之後或在該第二層之僅某一部分已形成之後發生。此外,鋰之擴散及至IC功能性材料之後續轉換在該第一或該第二沈積層中及在EC或CE層中發生。在一實例中,首先形成EC層,且接著鋰化該EC層。當隨後將CE層沈積在EC層之上時,一些鋰自下伏EC層朝著CE層擴散及/或擴散至CE層中,從而導致轉化成含有IC功能性材料之界面區。在另一實例中,首先形成EC層(視情況具有富氧上部區),接著,形成CE層且鋰化該CE層。隨後,來自CE層之一些鋰擴散至EC層中,在此處其形成具有IC功能性材料之界面區。在又一實例中,首先沈積EC層,且接著鋰化該EC層以根據上述之該第一機制產生某一IC功能性材料。接著,當形成CE層時,一些鋰自下伏EC層朝著CE層擴散以在CE層之界面區中產生某一IC材料。以此方式,IC功能性材料名義上緊接CE層與EC層之界面駐留於CE層及EC層兩者中。 在第三機制中,形成EC層及CE層至完成(或至少到達第二形成之層部分完成之時刻)。接著,加熱裝置結構,且該加熱將界面區中之材料之至少一些轉換成IC功能性材料(例如,鋰鹽)。加熱(例如,作為本文中進一步描述之多步驟熱化學調節(MTCC)之部分)可在沈積期間或在沈積完成之後執行。在一實施例中,在於堆疊上形成透明導電氧化物之後執行加熱。在另一實施例中,在該第二層部分或完全完成之後,但在將透明導電氧化物塗覆至該第二層之前應用加熱。在一些情況下,加熱直接且主要負責轉化。在其他情況下,加熱主要促進鋰離子之擴散或流動,如該第二機制中所描述,此建立IC功能性材料區。 最後,在第四機制中,在EC層與CE層之間流動之電流驅動電致變色材料及對向電極材料中之至少一者轉化為界面區中之IC功能性材料。此轉化可能發生,此係因為(例如)與流動電流相關聯之離子通量很大,以致其驅動EC及/或CE材料至界面區中之IC材料之化學轉化。舉例而言,如下文將解釋,穿過EC層中之氧化鎢之大的鋰通量可產生鎢酸鋰,其充當IC材料。鋰通量可(例如)在新形成之裝置之初始活化循環期間引入。然而,情況不必如此,此係因為用於驅動高離子通量之其他機會對實現該轉換而言可能更適當。本發明之方法可由一般熟習此項技術者在不採用以上機制中之任何一或多者之情況下執行。 圖3A為根據本發明之方法之程序流程300。具體言之,參見305,(在例如TCO之CL上)沈積EC層。接著,參見310,沈積CE層。在沈積EC層及CE層之後,接著,參見315,在EC層與CE層之間形成充當IC層之界面區。本發明之一實施例為步驟305與310顛倒之類似方法(未描繪)。該方法之要點在於,充當IC層之界面區係在EC層及CE層之後形成(在一些實施例中,使用EC層及CE層中之一者之至少部分形成界面區)。為此,有時將以此方式形成之界面區稱為「本質」IC層。在其他實施例中,例如使用EC材料或CE材料之富氧型式在EC層與CE層之間形成相異層,其中該層再次在形成EC層及CE層之後被完全或部分轉換成界面區。用以在形成EC-CE堆疊之後形成界面區之各種方法將在下文予以描述。 因此,如所提及,本發明之一態樣為一種製造電致變色裝置之方法,該方法包括:形成包括電致變色材料之電致變色層;形成與該電致變色層接觸之對向電極層,而並不首先在該電致變色層與該對向電極層之間提供離子傳導電絕緣層,其中該對向電極層包括對向電極材料;及在該電致變色層與該對向電極層之間形成界面區,其中該界面區為實質上離子傳導且實質上電絕緣的。該界面區可含有EC層、CE層或兩者之組份材料。如下文將更詳細描述,該界面區可以許多方式形成。 圖3B為展示根據關於圖3A所描述之方法之程序流程(詳言之,用於沈積EC層、接著沈積CE層且最終在該等層之間形成充當IC層之界面區之程序流程)的程序流程320。更特定言之,在此實施例中,EC層包括具有各種量之氧(詳言之,組合物及配置)之WO 3;CE層包括NiWO,界面區包括Li 2WO 4,且使用諸如氧化銦錫及經氟化之氧化錫之TCO材料。應注意,將在下文關於固態材料來描述電致變色裝置之層。固態材料由於可靠性、一致特性及程序參數及裝置效能而為所需的。例示性固態電致變色裝置、方法及用於製造其之設備以及用此等裝置製造電致變色窗之方法描述於Kozlowski等人之題為「Fabrication of Low Defectivity Electrochromic Devices」之美國非臨時專利申請案第12/645,111號及Wang等人之題為「Electrochromic Devices」之美國非臨時專利申請案第12/645,159號中,該兩專利申請案出於所有目的而以引用方式併入本文中。在特定實施例中,本發明之電致變色裝置全部為固態的且係在允許在受控周圍環境中沈積堆疊之一或多個層之設備中製造。亦即,在係在不離開設備且(例如)不破壞沈積步驟之間的真空之情況下沈積該等層之設備中,藉此減少污染物且最終改善裝置效能。在特定實施例中,本發明之設備不需要習知設備中所需之用於沈積IC層之單獨標靶。如一般熟習此項技術者將瞭解,本發明並不限於此等材料及方法,然而,在特定實施例中,組成電致變色堆疊及前驅物堆疊(如下文所描述)之材料全部為無機、固體(亦即,為固態)或無機且固體的。 因為有機材料傾向於隨時間推移而降級,例如當曝露於與窗應用相關聯之紫外光及熱時,所以無機材料提供可工作達長時間段之可靠電致變色堆疊之優點。固態材料亦提供不具有液態材料常常具有的污染物及洩漏問題之優點。應理解,堆疊中之該等層中之任何一或多者可含有某一量之有機材料,但在許多實施中,該等層中之一或多者含有很少或不含有有機物質。對於可能以小量存在於一或多個層中之液體而言可同樣如此。亦應理解,固態材料可藉由使用液體組份之製程(諸如,使用溶膠-凝膠或化學氣相沈積之特定製程)沈積或以其他方式形成。 再次參看圖3B,參見325,首先沈積WO 3之EC層。圖4A至圖4C為描繪根據本發明之特定方法及設備且具體言之根據程序流程320形成電致變色裝置之示意性橫截面。具體言之,圖4A至圖4C用以展示包括WO 3之EC層可如何形成為堆疊之部分之三個非限制性實例,其中充當IC層之界面區係在沈積該堆疊之其他層之後形成。在圖4A至圖4C中之每一者中,基板402、第一TCO層404、CE層410及第二TCO層412基本上相同。又,在該三個實施例中之每一者,形成不具有IC層之堆疊,且接著進一步處理該堆疊以便在該堆疊內形成充當IC層之界面區,其在EC層與CE層之間。 參看圖4A至圖4C中之每一者,分別描繪了分層結構400、403及409。此等分層結構中之每一者包括為(例如)玻璃之基板402。可使用具有合適光學、電、熱及機械性質之任何材料作為基板402。此等基板包括(例如)玻璃、塑膠及鏡材料。合適塑膠基板包括(例如)丙烯酸、聚苯乙烯、聚碳酸酯、烯丙基二乙二醇碳酸酯、SAN(styrene acrylonitrile copolymer,苯乙烯丙烯腈共聚物)、聚(4-甲基-1-戊烯)、聚酯、聚醯胺等,且較佳地,塑膠應能夠耐受高溫處理條件。若使用塑膠基板,則其較佳使用(例如)類鑽石保護塗層、矽石/聚矽氧耐磨塗層或其類似者(諸如,塑膠上光技術中所熟知之塗層)之硬塗層來加以障壁保護及磨損保護。合適玻璃包括透明或有色鹼石灰玻璃,包括鹼石灰漂浮玻璃。玻璃可為經回火或未經回火的。在一些實施例中,諸如玻璃基板之市售基板含有透明導電層塗層。此等玻璃之實例包括以商標TEC Glass™(Pilkington of Toledo, Ohio)及SUNGATE™ 300及SUNGATE™ 500 (PPG Industries of Pittsburgh, Pennsylvania)銷售的塗有導電層之玻璃。TEC Glass™為塗有經氟化之氧化錫導電層之玻璃。 在一些實施例中,基板402之光學透射率(亦即,透過之輻射或光譜對入射之輻射或光譜之比)為約90%至95%,例如,約90%至92%。基板可具有任何厚度,只要其具有合適機械性質以支撐電致變色裝置即可。雖然基板402可具有任何大小,但在一些實施例中,其為約0.01 mm至10 mm厚,較佳約3 mm至9 mm厚。 在本發明之一些實施例中,基板為建築玻璃。建築玻璃為用作建築材料之玻璃。建築玻璃通常用於商業建築中,但亦可用於居住建築中,且通常(但不必)分離室內環境與室外環境。在特定實施例中,建築玻璃為至少20吋乘以20吋,且可以更大,例如,大達約72吋乘以120吋。建築玻璃通常為至少約2 mm厚。小於約3.2 mm厚之建築玻璃不可回火。在以建築玻璃作為基板之本發明之一些實施例中,即使在已在基板上製造電致變色堆疊之後,基板仍可經回火。在以建築玻璃為基板之一些實施例中,基板為來自錫浮法生產線(tin float line)之鹼石灰玻璃。建築玻璃基板之可見光譜上之透射百分率(亦即,跨越可見光譜之整體透射)一般比中性基板大80%,但其可能低於著色基板之透射百分率。較佳地,基板在可見光譜上之透射百分率為至少約90%(例如,約90%至92%)。可見光譜為典型人眼會回應之光譜,一般為約380 nm(紫色)至約780 nm(紅色)。在一些情況下,玻璃具有在約10 nm與約30 nm之間的表面粗糙度。在一實施例中,基板402為具有鈉擴散障壁(未圖示)以防止鈉離子擴散至電致變色裝置中之鈉玻璃。為此描述之目的,將此配置稱為「基板402」。 再次參看分層結構400、403及409,(例如)由經氟化之氧化錫或其他合適材料(其尤其為導電且透明的)製成之第一TCO層404沈積在基板402之上。透明導電氧化物包括金屬氧化物及摻雜一或多種金屬之金屬氧化物。此等金屬氧化物及經摻雜之金屬氧化物之實例包括氧化銦、氧化銦錫、經摻雜之氧化銦、氧化錫、經摻雜之氧化錫、氧化鋅、氧化鋁鋅、經摻雜之氧化鋅、氧化釕、經摻雜之氧化釕及其類似者。在一實施例中,此第二TCO層之厚度在約20 nm與約1200 nm之間,在另一實施例中在約100 nm與約600 nm之間,在另一實施例中,約350 nm厚。TCO層由於該等層所跨越之相對較大區域而應具有適當之薄層電阻(R s)。在一些實施例中,TCO層之薄層電阻在每平方約5歐姆與約30歐姆之間。在一些實施例中,TCO層之薄層電阻為每平方約15歐姆。一般而言,希望兩個導電層中之每一者之薄層電阻大致相同。在一實施例中,兩個層(例如,404及412)各自具有約每平方10-15歐姆之薄層電阻。 分層結構400、403及409中之每一者分別包括堆疊414a、414b及414c,該等堆疊中之每一者包括在基板402之上之第一TCO層404、CE層410及第二TCO層412。分層結構400、403及409中之每一者之差異在於EC層係如何形成的,在每一情形下,此又影響所得界面區之形態。 與圖3B之程序流程320一致,堆疊414a、414b及414c中之每一者包括沈積在第一TCO層404之上之電致變色層。該電致變色層可含有包括金屬氧化物之許多不同電致變色材料中之任何一或多者。此等金屬氧化物包括氧化鎢(WO 3)、氧化鉬(MoO 3)、氧化鈮(Nb 2O 5)、氧化鈦(TiO 2)、氧化銅(CuO)、氧化銥(Ir 2O 3)、氧化鉻(Cr 2O 3)、氧化錳(Mn 2O 3)、氧化釩(V 2O 5)、氧化鎳(Ni 2O 3)、氧化鈷(Co 2O 3)及其類似者。在一些實施例中,金屬氧化物摻雜有一或多種摻雜劑,諸如鋰、鈉、鉀、鉬、鈮、釩、鈦及/或其他合適金屬或含有金屬之化合物。混合氧化物(例如,W-Mo氧化物、W-V氧化物)亦可在特定實施例中使用,亦即,電致變色層包括上述金屬氧化物中之兩者或兩者以上。包括金屬氧化物之電致變色層能夠接收自對向電極層轉移之離子。 在一些實施例中,將氧化鎢或經摻雜之氧化鎢用於電致變色層。在本發明之一實施例中,電致變色層實質上由WO x 製成,其中「 x」指代電致變色層中之氧與鎢之原子比,且 x在約2.7與3.5之間。已提出僅低於化學計量之氧化鎢展現電致變色;亦即,化學計量之氧化鎢(WO 3)不展現電致變色。在一更特定實施例中,將WO x (其中 x小於3.0且為至少約2.7)用於電致變色層。在另一實施例中,電致變色層為WO x ,其中 x在約2.7與約2.9之間。諸如拉塞福背向散射光譜測定法(RBS,Rutherford Backscattering Spectroscopy)之技術可識別包括鍵結至鎢之氧原子及未鍵結至鎢之氧原子之氧原子之總數。在一些例子中,氧化鎢層(其中 x為3或更大)展現電致變色,其可能係歸因於未結合之過量氧以及低於化學計量之氧化鎢。在另一實施例中,氧化鎢層具有化學計量或更多之氧,其中 x為3.0至約3.5。在本發明之一些實施例中,EC層之至少一部分具有過量之氧。將EC層之此更高度氧化之區用作形成充當IC層之離子傳導電絕緣區之前驅物。在其他實施例中,高度氧化之EC材料之相異層形成於EC層與CE層之間以用於至少部分地至離子傳導電絕緣界面區之最終轉換。 在特定實施例中,氧化鎢為晶形、奈米晶形或非晶形的。在一些實施例中,氧化鎢為實質上奈米晶形的,且具有平均約5 nm至50 nm(或約5 nm至20 nm)之晶粒大小,以透射電子顯微學(TEM)為特性。氧化鎢形態或微結構亦可使用x光繞射(XRD)及/或電子繞射(諸如,選定區域電子繞射(SAED))特性化為奈米晶形的。舉例而言,奈米晶形電致變色氧化鎢之特性可能在於以下XRD特徵:約10至100 nm(例如,約55 nm)之晶體大小。此外,奈米晶形氧化鎢可展現有限之長程有序性,例如,約若干(約5至20個)氧化鎢單位晶胞。 因此,為便利起見,圖3B中之程序流程320之剩餘部分將關於第一實施例(包括圖4A中所表示之EC層406之形成)予以進一步描述。接著,將在下文描述圖4B及圖4C中分別表示之第二實施例及第三實施例,其尤其著重於其各別EC層之形成及形態及/或微結構。 如參看圖3B所提及,參見325,沈積EC層。在第一實施例(圖4A中所表示)中,實質上均質之EC層406(包括WO 3)經形成作為堆疊414a之部分,其中該EC層與CE層410直接接觸。在一實施例中,如上所述,該EC層包括WO 3。在一實施例中,在沈積WO 3之至少一部分期間應用加熱。在一特定實施例中,經過濺鍍標靶若干遍,其中在每一遍經過時沈積WO 3之一部分,且在每一遍沈積之後將加熱應用於(例如)基板402以在沈積層406之WO 3之下一部分之前調節WO 3。在其他實施例中,可在沈積期間連續加熱WO 3層,且可以連續方式進行沈積,而非經過濺鍍標靶若干遍。在一實施例中,該EC層之厚度在約300 nm與約600 nm之間。如所提及,該EC層之厚度取決於所要結果及形成IC層之方法。 在關於圖4A所描述之實施例中,EC層為厚度在約500 nm與約600 nm之間的使用鎢標靶及包括約40%與約80%之間的O 2及約20%與約60%之間的Ar之濺鍍氣體濺鍍之WO 3,且其中沈積有WO 3之基板在形成EC層期間被至少間歇性地加熱至約150℃與約450℃之間。在一特定實施例中,EC層為約550 nm厚之使用鎢標靶濺鍍之WO 3,其中該濺鍍氣體包括約50%至約60%之O 2及約40%至約50%之Ar,且沈積有WO 3之基板在形成該電致變色層期間被至少間歇性地加熱至約250℃與約350℃之間。在此等實施例中,WO 3層為實質上均質的。在一實施例中,WO 3為實質上多晶的。咸信,在沈積期間至少間歇性地加熱WO 3幫助多晶形式之WO 3之形成。 如所提及,許多材料適合於EC層。一般而言,在電致變色材料中,電致變色材料之著色(或任何光學性質,例如,吸光度、反射率及透射率之變化)係藉由至材料中之可逆離子插入(例如,夾插)及電荷平衡電子之對應注入引起。通常,負責光學過渡之離子之某一小部分在電致變色材料中不可逆地結合在一起。如本文中所描述,不可逆地結合之離子之一些或全部用以補償材料中之「盲電荷(blind charge)」。在大部分電致變色材料中,合適離子包括鋰離子(Li +)及氫離子(H +)(亦即,質子)。然而,在一些情況下,其他離子將為合適的。此等離子包括(例如)氘離子(D +)、鈉離子(Na +)、鉀離子(K +)、鈣離子(Ca ++)、鋇離子(Ba ++)、鍶離子(Sr ++)及鎂離子(Mg ++)。在本文中所描述之各種實施例中,鋰離子用以產生電致變色現象。鋰離子至氧化鎢(WO 3-y(0<y≤~0.3))中之夾插使氧化鎢自透明(褪色狀態)改變為藍色(著色狀態)。在EC層包括或為氧化鎢之典型製程中,鋰係(例如)經由濺鍍沈積在EC層406上以滿足盲電荷(如下文參看圖6及圖7將更詳細論述),參見圖3B中之程序流程之330。在一實施例中,鋰化係在整合式沈積系統(其中真空在沈積步驟之間未被破壞)中執行。應注意,在一些實施例中,鋰並不在此階段添加,而是可在沈積對向電極層之後添加,或在其他實施例中,鋰係在沈積TCO之後添加。 再次參看圖4A,接下來,在EC層406上沈積CE層410。在一些實施例中,對向電極層410為無機及/或固體。該對向電極層可包括在電致變色裝置處於褪色狀態下時能夠充當離子之儲集器之許多不同材料中之一或多者。在藉由(例如)施加適當電位起始之電致變色過渡期間,對向電極層將其保持之離子中之一些或全部轉移至電致變色層,從而使電致變色層改變為著色狀態。同時,在NiO及/或NiWO之情況下,對向電極層由於離子之損失而著色。 在一些實施例中,用於對向電極之合適材料包括氧化鎳(NiO)、氧化鎳鎢(NiWO)、氧化鎳釩、氧化鎳鉻、氧化鎳鋁、氧化鎳錳、氧化鎳鎂、氧化鉻(Cr 2O 3)、氧化錳(MnO 2)及普魯士藍(Prussian blue)。光學被動對向電極包括氧化鈰鈦(CeO 2-TiO 2)、氧化鈰鋯(CeO 2-ZrO 2)、氧化鎳(NiO)、氧化鎳鎢(NiWO)、氧化釩(V 2O 5)及氧化物之混合物(例如,Ni 2O 3與WO 3之混合物)。亦可使用此等氧化物之摻雜調配物,其中摻雜劑包括(例如)鉭及鎢。因為對向電極層410含有用以在電致變色材料處於褪色狀態下時在電致變色材料中產生電致變色現象之離子,所以對向電極在其保持顯著量之此等離子時較佳具有高透射率及中性色彩。對向電極形態可為晶形、奈米晶形或非晶形。 在一些實施例中,在對向電極層為氧化鎳鎢之情況下,對向電極材料為非晶形或實質上非晶形的。與實質上非晶形之氧化鎳鎢對向電極之晶形對應物相比,已發現該等實質上非晶形之氧化鎳鎢對向電極在一些條件下較佳地執行。如下文所描述,可藉由使用特定處理條件獲得氧化鎳鎢之非晶形狀態。儘管不希望束縛於任何理論或機制,但咸信,非晶形氧化鎳鎢係藉由濺鍍製程中之相對較高能量之原子產生。較高能量之原子係(例如)在具有較高標靶功率、較低腔室壓力(亦即,較高真空)及較小的源至基板之距離之濺鍍製程中獲得。在所描述之處理條件下,產生在UV/熱曝露下具有更佳穩定性之較高密度薄膜。 在特定實施例中,存在於氧化鎳鎢中之鎳的量可高達氧化鎳鎢之約90重量%。在一特定實施例中,氧化鎳鎢中之鎳與鎢之質量比在約4:6與6:4之間,在一實例中為約1:1。在一實施例中,NiWO包含約15%(原子)與約60%之間的Ni,及在約10%與約40%之間的W。在另一實施例中,NiWO包含約30%(原子)與約45%之間的Ni,及在約15%與約35%之間的W。在另一實施例中,NiWO包含在約30%(原子)與約45%之間的Ni,及在約20%與約30%之間的W。在一實施例中,NiWO包含約42%(原子)之Ni及約14%之W。 在一實施例中,如上所述,參見圖3B之335,CE層410為NiWO。在一實施例中,CE層之厚度在約150 nm與約300 nm之間,在另一實施例中在約200 nm與約250 nm之間,在另一實施例中為約230 nm。 在典型製程中,亦將鋰塗覆至CE層,直至CE層褪色。應理解,對著色狀態與褪色狀態之間的過渡之述及為非限制性的且暗示可能實施之電致變色過渡之許多實例中之僅一個實例。除非本文中另有說明,否則無論何時述及褪色-著色過渡,對應之裝置或製程涵蓋諸如非反射-反射、透明-不透明等之其他光學狀態過渡。此外,術語「褪色」指代光學中性狀態,例如未著色、透明或半透明。更進一步,除非本文中另有說明,否則電致變色過渡之「色彩」不限於任何特定波長或波長範圍。如一般熟習此項技術者所理解,適當電致變色材料及對向電極材料之選擇控管相關光學過渡。 在一特定實施例中,參見圖3B之340,鋰(例如,經由濺鍍)添加至NiWO CE層。在一特定實施例中,參見圖3B之345,在已引入足夠鋰以使NiWO完全褪色之後添加額外量之鋰(此程序為可選的,且在一實施例中,在程序之此階段不添加過量鋰)。在一實施例中,此額外量在基於使該對向電極層褪色所需之量過量約5%與約15%之間。在另一實施例中,添加至CE層之過量鋰為基於使該對向電極層褪色所需之量過量約10%。在沈積CE層410、以鋰使其褪色及添加額外鋰之後,參見圖3B之350,在對向電極層之上沈積第二TCO層412。在一實施例中,透明導電氧化物包括氧化銦錫,在另一實施例中,TCO層為氧化銦錫。在一實施例中,此第二TCO層之厚度在約20 nm與約1200 nm之間,在另一實施例中在約100 nm與約600 nm之間,在另一實施例中為約350 nm。 再次參看圖4A,一旦完成分層結構400,則使其經受將堆疊414a之至少一部分轉換成IC層之熱化學調節(若其歸因於鋰擴散或其他機制而未經轉換)。堆疊414a為前驅物而非電致變色裝置,此係因為該堆疊在EC層406與CE層410之間尚未具有離子傳導/電絕緣層(或區)。在此特定實施例中,在兩步驟之程序中,EC層406之部分經轉換成IC層408以形成功能性電致變色裝置401。參看圖3B,參見355,分層結構400經受MTCC。在一實施例中,該堆疊首先在惰性氛圍(例如,氬氣)下在約150℃與約450℃之間經受加熱歷時約10分鐘與約30分鐘之間,且接著在O 2下加熱歷時約1分鐘與約15分鐘之間。在另一實施例中,該堆疊在約250℃下在惰性氛圍下加熱歷時約15分鐘,且接著在O 2下加熱約5分鐘。接下來,分層結構400在空氣中經受加熱。在一實施例中,該堆疊在空氣中在約250℃與約350℃之間加熱歷時約20分鐘與約40分鐘之間,在另一實施例中,該堆疊在空氣中在約300℃下加熱歷時約30分鐘。實施MTCC所需之能量不必為輻射熱能。舉例而言,在一實施例中,使用紫外輻射來實施MTCC。在不脫離本發明之範疇的情況下亦可使用其他能量源。 在多步驟熱化學調節之後,程序流程320完成,且建立功能性電致變色裝置。如所提及,且儘管不希望受理論限制,但咸信,堆疊414a中之鋰與EC層406及/或CE層410之一部分一起組合以形成充當IC層之界面區408。咸信界面區408主要為鎢酸鋰(Li 2WO 4),已知其相對於傳統IC層材料具有良好的離子傳導及電絕緣性質。如上文所論述,尚不明確知曉此現象如何發生。存在在多步驟熱化學調節期間必須發生以在EC層與CE層之間形成離子傳導電絕緣區408之化學反應,但亦認為,行進穿過堆疊之鋰之初始通量(例如,由如上所述之添加至CE層之過量鋰提供)在IC層408之形成中起作用。離子傳導電絕緣區之厚度可取決於所使用之材料及用於形成該層之處理條件而改變。在一些實施例中,界面區408之厚度在約10 nm與約150 nm之間,在另一實施例中在約20 nm與約100 nm之間,且在其他實施例中在約30 nm與約50 nm之間。 如上文所提及,存在用於形成EC層之許多合適材料。因而,在上述方法中使用(例如)鋰或其他合適離子,吾人可自富氧EC材料開始製成充當IC層之其他界面區。用於此用途之合適EC材料包括(但不限於)SiO 2、Nb 2O 5、Ta 2O 5、TiO 2、ZrO 2及CeO 2。在使用鋰離子之特定實施例中,離子傳導材料(諸如,但不限於,矽酸鋰、矽酸鋰鋁、硼酸鋰鋁、氟化鋰鋁、硼酸鋰、氮化鋰、矽酸鋰鋯、鈮酸鋰、硼矽酸鋰、磷矽酸鋰及其他此等基於鋰之陶瓷材料、矽石或氧化矽(包括氧化鋰矽))可製成為充當IC層之界面區。 如所提及,在一實施例中,離子傳導區之前驅物為經由本文中所描述之鋰化及MTCC轉化成離子傳導/電絕緣區之富氧(超化學計量之)層。儘管不希望束縛於理論,但咸信,在鋰化後,過量氧形成氧化鋰,其進一步形成鋰鹽(亦即,鋰電解質),諸如,鎢酸鋰(Li 2WO 4)、鉬酸鋰(Li 2MoO 4)、鈮酸鋰(LiNbO 3)、鉭酸鋰(LiTaO 3)、鈦酸鋰(Li 2TiO 3)、鋯酸鋰(Li 2ZrO 3)及其類似物。在一實施例中,界面區包含下列各者中之至少一者:氧化鎢(WO 3+x,0≤x≤1.5)、氧化鉬(MoO 3+x,0≤x≤1.5)、氧化鈮(Nb 2O 5+x,0≤x≤2)、氧化鈦(TiO 2+x,0≤x≤1.5)、氧化鉭(Ta 2O 5+x,0≤x≤2)、氧化鋯(ZrO 2+x,0≤x≤1.5)及氧化鈰(CeO 2+x,0≤x≤1.5)。 然而,任何材料可用於離子傳導界面區,只要該材料可經製造而具有低缺陷度且其在實質上阻止電子通過的同時允許離子在對向電極層410與電致變色層406之間通過即可。該材料可以實質上傳導離子且實質上抵抗電子為特性。在一實施例中,該離子導體材料具有介於約10 -10西門子/公分(Siemens/cm)(或ohm -1cm -1)與約10 -3西門子/公分之間的離子電導率及大於10 5歐姆-公分之電阻率。在另一實施例中,該離子導體材料具有介於約10 -8西門子/公分與約10 -3西門子/公分之間的離子電導率及大於10 10歐姆-公分之電阻率。雖然離子傳導層應大體上抗漏電流(例如,提供不大於約15 μA/cm 2之漏電流),但已發現,如本文中所描述而製造之一些裝置具有驚人的高之漏電流(例如,在約40 μA/cm與約150 μA/cm之間),但仍提供跨越裝置之良好色彩變化且有效地操作。 如上文所提及,存在在形成堆疊之後,於EC層與CE層之間建立離子傳導電絕緣區之至少兩種其他方式。此等額外實施例將在下文參考將氧化鎢用於IC層之特定實例予以描述。又,如上文所提及,當(例如)鋰擴散或熱將EC及/或CE層之一些轉換成界面區時,具有IC性質之界面區可在製造堆疊期間在原位形成。 通常,在製程中稍後建立離子傳導區存在特定益處。首先,可保護離子傳導材料不受在EC層及CE層之沈積及鋰化期間發生的苛刻處理中之一些影響。舉例而言,藉由電漿製程沈積此等層常常伴隨著緊接堆疊之大的電壓降,常在15-20伏特上下。此等大電壓可損害敏感離子傳導材料或造成敏感離子傳導材料之分解。藉由將IC材料形成移至製程中稍後階段,該材料即不曝露於潛在之損害電壓極值。其次,藉由在製程中稍後形成IC材料,吾人可更佳地控制在完成EC層及CE層兩者之前所不可能的一些處理條件。此等條件包括鋰擴散及電極之間的電流。在製程中後期控制此等及其他條件提供額外靈活性以使IC材料之物理性質及化學性質適合特定應用。因此,並非本發明之所有益處皆歸因於充當IC層之獨特界面區,亦即,亦存在製造及其他益處。 已觀測到,與使用用於形成IC層之習知技術(例如,自IC材料標靶之PVD)製造之裝置相比,根據本文中所描述之實施例中之一些形成之離子傳導材料具有優異效能。舉例而言,已發現,與傳統裝置之20-25分鐘或以上相比,裝置切換速度非常快(例如,小於10分鐘,在一實例中為約8分鐘)以達成約80%之最終狀態。在一些例子中,本文中所描述之裝置具有優於習知裝置之切換速度數量級。此可能可歸因於較大量的安置在界面區及/或分級界面中之可容易地轉移(例如,在EC與界面區之間及/或在CE與界面區之間)之鋰。此等鋰可處於與存在於界面區中之IC相互混之EC及/或CE相中。其亦可能歸因於存在於界面區中之IC材料之相對較薄層或網路。為支持此觀點,已觀測到,根據本文中之教示製造之一些裝置具有高漏電流,但仍驚人地展現良好色彩變化及良好效率。在一些情況下,已發現穩健執行之裝置之漏電流密度為至少約100 μA/cm。 現參看圖4B,在第二實施例中,堆疊414b之最初敷設之EC材料實際上為兩個層:第一WO 3層406,其類似於圖4A中之層406,但厚度在約350 nm與約450 nm之間,該第一層係使用鎢標靶及包括約40%與約80%之間的O 2及約20%與約60%之間的Ar之第一濺鍍氣體濺鍍;及第二WO 3層405,其厚度在約100 nm與約200 nm之間,該第二層係使用鎢標靶及包括約70%與100%之間的O 2及0%與約30%之間的Ar之第二濺鍍氣體濺鍍。在此實施例中,藉由在第一WO 3層406之沈積期間將基板402至少間歇性地加熱至約150℃與約450℃之間而施加熱,但在第二WO 3層405之沈積期間不加熱或實質上不加熱。在一更特定實施例中,層406為約400 nm厚,且該第一濺鍍氣體包括約50%與約60%之間的O 2及約40%與約50%之間的Ar;第二WO 3層405為約150 nm厚,且該第二濺鍍氣體實質上為純O 2。在此實施例中,在第一WO 3層406之形成期間至少間歇性地施加熱至約200℃與約350℃之間,但在第二WO 3層405之形成期間不加熱或實質上不加熱。以此方式,該第一WO 3層為實質上多晶的,而該第二WO 3層不必如此。 再次參看圖4B,如上文關於圖3B及圖4A所描述,藉由以下操作來完成堆疊:鋰化EC層406及405以大致或實質上滿足盲電荷、沈積CE層410、將CE層鋰化至褪色狀態、添加額外鋰及沈積第二TCO層412以完成分層堆疊403。對分層堆疊403執行類似熱化學調節以提供分層堆疊407、包括離子傳導電絕緣區408a之功能性電致變色裝置。儘管不希望束縛於理論,但在此實例中,咸信WO 3之富氧層405主要充當前驅物材料之源以形成界面區408a。在此實例中,整個富氧WO 3層經描繪為轉換成界面區408a,然而,已發現,情況並不始終如此。在一些實施例中,富氧層之僅一部分經轉換而形成起到IC層之功能之界面區。 現參看圖4C,在第三實施例中,分層堆疊409包括EC層406a(其具有WO 3之分級組合物( graded composition)且形成為堆疊414c之部分),其中該分級組合物包括變化含量之氧。在一非限制性實例中,在EC-CE層(410)界面處存在比TCO層404與EC層406a之界面處高的EC層406a中之氧濃度。 在一實施例中,EC層406a為厚度在約500 nm與約600 nm之間的使用鎢標靶及濺鍍氣體濺鍍之分級組合物WO 3層,其中該濺鍍氣體在濺鍍電致變色層開始時包括約40%與約80%之間的O 2及約20%與約60%之間的Ar,且該濺鍍氣體在濺鍍該電致變色層結束時包括約70%與100%之間的O 2及0%與約30%之間的Ar,且其中在EC層406a之形成之開始期間至少間歇性地施加熱至(例如)基板402至約150℃與約450℃之間,但不或實質上不在EC層406a之至少一最後部分之沈積期間施加熱。在一更特定實施例中,分級組合物WO 3層為約550 nm厚;該濺鍍氣體在濺鍍該電致變色層開始時包括約50%與約60%之間的O 2及40%與約50%之間的Ar,且該濺鍍氣體在濺鍍該電致變色層結束時為實質上純O 2;且其中在電致變色層之形成之開始期間至少間歇性地施加熱至(例如)基板402至約200℃與約350℃之間,但不或實質上不在電致變色層之至少一最後部分之沈積期間施加熱。在一實施例中,在沈積開始時在所述溫度範圍下施加熱,且逐漸減小至在沈積了約一半之EC層時不施加熱,而濺鍍氣體組合物在EC層之沈積期間沿著實質上線性之速率自約50%與約60%之間的O 2及約40%與約50%之間的Ar調整至實質上純O 2。 更一般地,該界面區通常(但不必)具有包括由不同相及/或組成表示之至少兩個離散組份之異質結構。此外,該界面區在此等兩個或兩個以上離散組份(諸如,離子傳導材料及電致變色材料(例如,鎢酸鋰與氧化鎢之混合物))中可包括梯度。該梯度可提供(例如)可變之組合物、微結構、電阻率、摻雜劑濃度(例如,氧濃度)、化學計量、密度及/或晶粒大小範圍。該梯度可具有許多不同形式之過渡,包括線性過渡、S型過渡、高斯過渡等。在一實例中,電致變色層包括過渡至超化學計量氧化鎢區中之氧化鎢區。該超化學計量氧化物區之部分或全部經轉換成界面區。在最後結構中,氧化鎢區為實質上多晶的,且微結構在界面區處過渡至實質上非晶形的。在另一實例中,電致變色層包括過渡至(超化學計量之)氧化鈮區中之氧化鎢區。該氧化鈮區之部分或全部經轉換成界面區。在最後結構中,氧化鎢區為實質上多晶的,且微結構在界面區處過渡至實質上非晶形的。 再次參看圖4C,如上文關於圖3B及圖4A所描述,藉由以下操作來完成堆疊: 鋰化EC層406a以大致或實質上滿足盲電荷、沈積CE層410、鋰化CE層至褪色狀態、添加額外鋰及沈積第二TCO層412以完成分層堆疊409。對分層堆疊409執行類似之多步驟熱化學調節以提供分層堆疊411、包括離子傳導電絕緣區408b及原始分層EC層406a之至少一部分(其在功能性電致變色裝置411中充當EC層)之功能性電致變色裝置。儘管不希望束縛於理論,但在此實例中,咸信,WO 3之分級層之最上層富氧部分主要形成分級界面區408b。儘管不希望束縛於理論,但存在如下可能性:界面區之形成為受自身限制的且取決於堆疊中之氧、鋰、電致變色材料及/或對向電極材料之相對量。 在本文中所描述之各種實施例中,電致變色堆疊經描述為在特定處理階段期間不或實質上不加熱。在一實施例中,在加熱步驟之後,主動或被動地(例如,使用散熱片)冷卻堆疊。本發明之設備包括主動及被動冷卻組件,例如,主動冷卻可包括經由流體循環、曝露於冷(例如,經由膨脹)氣體之冷卻、致冷單元及其類似者而冷卻之壓板。被動冷卻組件可包括散熱片,諸如金屬塊及其類似者,或僅自於熱之曝露移除基板。 本發明之另一態樣為一種製造電致變色裝置之方法,該方法包括:(a)形成包括電致變色材料之電致變色層或包括對向電極材料之對向電極層;(b)在該電致變色層或該對向電極層上方形成中間層,其中該中間層包括該電致變色材料、該對向電極材料及額外材料中之至少一者之富氧形式,其中該額外材料包括相異之電致變色材料或對向電極材料,其中該中間層不為實質上電絕緣的;(c)形成該電致變色層及該對向電極層中之另一者;及(d)允許該中間層之至少一部分變得實質上電絕緣。在一實施例中,該電致變色材料為WO 3。在另一實施例中,(a)包括使用鎢標靶及包括約40%與約80%之間的O 2及約20%與約60%之間的Ar之第一濺鍍氣體濺鍍WO 3以達到在約350 nm與約450 nm之間的厚度,及在該電致變色層之形成期間至少間歇性地加熱至約150℃與約450℃之間。在另一實施例中,(b)包括在不加熱的情況下使用鎢標靶及包括約70%與100%之間的O 2及0%與約30%之間的Ar之第二濺鍍氣體濺鍍WO 3以達到在約100 nm與約200 nm之間的厚度。在又一實施例中,該方法進一步包括將鋰濺鍍至該中間層上,直至盲電荷大致或實質上得到滿足。在一實施例中,該對向電極層包括厚度在約150 nm與約300 nm之間的NiWO。在另一實施例中,將鋰濺鍍至對向電極層上,直至該對向電極層褪色。在另一實施例中,將基於使該對向電極層褪色所需之量過量約5%與約15%之間的額外量之鋰濺鍍至該對向電極層上。在另一實施例中,在該對向電極層之上沈積透明導電氧化物層。在一實施例中,該透明導電氧化物包括氧化銦錫,在另一實施例中,該透明導電氧化物為氧化銦錫。在另一實施例中,將根據以上實施例形成之堆疊在Ar下在約150℃與約450℃之間加熱歷時約10分鐘與約30分鐘之間,且接著在O 2下加熱歷時約1分鐘與約15分鐘之間,且接著在空氣中在約250℃與約350℃之間加熱歷時約20分鐘與約40分鐘之間。 在另一實施例中,(a)包括濺鍍式MO x 之第一電致變色材料,其中M為金屬或非金屬元素,且 x指示化學計量之氧與M之比,且(b)包括濺鍍式NO y 之第二電致變色材料以作為中間層,其中N為相同或不同之金屬或非金屬元素,且 y指示超化學計量量之氧與N之比。在一實施例中,M為鎢,且N為鎢。在另一實施例中,M為鎢,且N係選自由鈮、矽、鉭、鈦、鋯及鈰組成之群組。 本發明之另一實施例為一種電致變色裝置,其包括:(a)包括電致變色材料之電致變色層;(b)包括對向電極材料之對向電極層;及(c)在該電致變色層與該對向電極層之間的界面區,其中該界面區包括電絕緣離子傳導材料及該電致變色材料、該對向電極材料及額外材料中之至少一者,其中該額外材料包括相異之電致變色材料或對向電極材料。 在一實施例中,該電絕緣離子傳導材料及該電致變色材料、該對向電極材料及該額外材料中之至少一者實質上均勻地分佈於該界面區內。在另一實施例中,該電絕緣離子傳導材料及該電致變色材料、該對向電極材料及該額外材料中之至少一者包括在垂直於該等層之方向上之組成梯度。在另一實施例中,與兩個前述實施例中之任一者一致,該電絕緣離子傳導材料包括鎢酸鋰,該電致變色材料包括氧化鎢,且該對向電極材料包括氧化鎳鎢。在前述實施例之一特定實施中,不存在額外材料。在一實施例中,該電致變色層之厚度在約300 nm與約500 nm之間,該界面區之厚度在約10 nm與約150 nm之間,且該對向電極層之厚度在約150 nm與約300 nm之間。在另一實施例中,該電致變色層之厚度在約400 nm與約500 nm之間;該界面區之厚度在約20 nm與約100 nm之間,且該對向電極層之厚度在約150 nm與約250 nm之間。在又一實施例中,該電致變色層之厚度在約400 nm與約450 nm之間;該界面區之厚度在約30 nm與約50 nm之間,且該對向電極層之厚度在約200 nm與約250 nm之間。 另一實施例為一種製造電致變色裝置之方法,該方法包括: 藉由用包含約40%與約80%之間的O 2及約20%與約60%之間的Ar之濺鍍氣體濺鍍鎢標靶以產生WO 3至在約500 nm與約600 nm之間的厚度來沈積電致變色層,其中沈積有該WO 3之基板在該電致變色層之形成期間被至少間歇性地加熱至約150℃與約450℃之間; 將鋰濺鍍至該電致變色層上,直至盲電荷得到滿足; 在該電致變色層上沈積對向電極層,而並不首先在該電致變色層與該對向電極層之間提供離子傳導電絕緣層,其中該對向電極層包括NiWO; 將鋰濺鍍至該對向電極層上,直至該對向電極層實質上褪色;及 在該電致變色層與該對向電極層之間形成界面區,其中該界面區為實質上離子傳導且實質上電絕緣的。在一實施例中,形成該界面區包括該堆疊單獨或與基板、導電層及/或囊封層一起之MTCC。 本發明之電致變色裝置可包括諸如一或多個被動層之一或多個額外層(未圖示)(例如)以改良特定光學性質(提供防潮或抗刮擦性)以氣密式地密封該電致變色裝置及其類似物。通常(但不必),罩蓋層沈積於該電致變色堆疊上。在一些實施例中,該罩蓋層為SiAlO。在一些實施例中,該罩蓋層係藉由濺鍍沈積。在一實施例中,罩蓋層之厚度在約30 nm與約100 nm之間。 自上文之論述應瞭解,本發明之電致變色裝置可在單一腔室設備(例如,具有(例如)鎢標靶、鎳標靶及鋰標靶以及氧氣及氬氣濺鍍氣體之濺鍍工具)中製造。如所提及,歸因於經形成以起到習知相異IC層之用途的界面區之性質,用於濺鍍IC層之單獨標靶並非必需的。發明者特別感興趣的是(例如)以高產量方式製造本發明之電致變色裝置,因此,需要具有可在基板通過整合式沈積系統時順序地製造本發明之電致變色裝置之設備。舉例而言,發明者對在窗、特別是建築玻璃鱗片窗(上述)上製造電致變色裝置特別感興趣。 因此,本發明之另一態樣為一種用於製造電致變色裝置之設備,其包括:整合式沈積系統,其包括:(i)含有材料源之第一沈積台,其經配置以沈積包括電致變色材料之電致變色層;及(ii)第二沈積台,其經配置以沈積包括對向電極材料之對向電極層;及控制器,其含有用於以在該基板上順序地沈積堆疊之方式傳遞該基板經過該第一沈積台及該第二沈積台之程式指令,該堆疊具有夾在該電致變色層與該對向電極層之間的中間層;其中該第一沈積台及該第二沈積台中之任一者或兩者亦經配置以在該電致變色層或該對向電極層上方沈積該中間層,且其中該中間層包括該電致變色材料或該對向電極材料之富氧形式,且其中該第一沈積台及該第二沈積台串聯互連且可操作以將基板自一個台傳遞至下一個台而不將該基板曝露於外部環境。在一實施例中,本發明之設備可操作以將該基板自一個台傳遞至下一個台而不破壞真空,且可包括可操作以將來自含鋰材料源之鋰沈積在該電致變色裝置之一或多個層上之一或多個鋰化台。在一實施例中,本發明之設備可操作以在建築玻璃基板上沈積該電致變色堆疊。 在一實施例中,該設備可操作以將該基板自一個台傳遞至下一個台而不破壞真空。在另一實施例中,該整合式沈積系統進一步包括可操作以在該電致變色層、該中間層及該對向電極層中之至少一者上沈積來自含鋰材料源之鋰之一或多個鋰化台。在又一實施例中,該整合式沈積系統可操作以在建築玻璃基板上沈積該堆疊。在另一實施例中,該整合式沈積系統進一步包括可操作以在使該建築玻璃基板通過該整合式沈積系統時將該建築玻璃基板固持在垂直定向上之基板固持器及輸送機構。在另一實施例中,該設備進一步包括用於在外部環境與該整合式沈積系統之間傳遞該基板之一或多個真空預抽室(load lock)。在另一實施例中,該設備進一步包括至少一狹縫閥門,該至少一狹縫閥門可操作以准許該一或多個鋰沈積台與該第一沈積台及該第二沈積台中之至少一者隔離。在一實施例中,該整合式沈積系統包括經配置以加熱該基板之一或多個加熱器。 圖5以透視圖描繪整合式沈積系統500之簡化表示且更詳細地包括內部之剖視圖。在此實例中,系統500為模組,其中入口真空預抽室502及出口真空預抽室504連接至沈積模組506。存在用於裝載(例如)建築玻璃基板525之入口埠510(真空預抽室504具有對應出口埠)。基板525由沿著軌道515行進之集裝架520支撐。在此實例中,集裝架520係經由懸掛而由軌道515支撐,但集裝架520亦可支撐在靠近設備500之底部定位之軌道或(例如)在設備500之頂部與底部中間的軌道之頂上。集裝架520可在系統500中向前及/或向後平移(如雙頭箭頭所指示)。舉例而言,在鋰沈積期間,基板可在鋰標靶530前面向前及向後移動,從而產生多次通過以便達成所要鋰化。然而,此功能不限於鋰標靶,例如,鎢標靶可通過基板多次,或該基板可在該鎢標靶前面經由向前/向後運動路徑通過以沈積(例如)電致變色層。集裝架520及基板525處於實質上垂直之定向上。實質上垂直之定向並非限制性的,但其可幫助防止缺陷,此係因為可能(例如)自來自濺鍍之原子之聚結產生之顆粒物質將傾向於受到重力且因此不沈積在基板525上。又,因為建築玻璃基板傾向於為大的,所以基板之垂直定向在其橫越該整合式沈積系統之該等台時實現較薄玻璃基板之塗佈,此係因為對關於較厚熱玻璃發生之下垂之擔憂較少。 標靶530(在此情況下為圓柱形標靶)係經定向而實質上平行於將發生沈積之基板表面且在該基板表面前面(為便利起見,此處未描繪其他濺鍍手段)。基板525在沈積期間可平移通過標靶530,及/或標靶530可在基板525前面移動。標靶530之移動路徑不限於沿著基板525之路徑平移。標靶530可沿著通過其長度之軸線旋轉、沿著基板之路徑(向前及/或向後)平移、沿著垂直於基板之路徑之路徑平移、在平行於基板525之平面中以圓形路徑移動等。標靶530不必為圓柱形的,其可為平坦的或沈積具有所要性質之所要層所需之任何形狀。又,在每一沈積台中可能存在一個以上之標靶,及/或標靶可取決於所要製程而在台之間移動。本發明之整合式沈積系統之各種台可為模組,但其一旦連接即形成連續系統,其中建立且維持受控周圍環境以便在系統內之各種台處處理基板。 如何使用整合式沈積系統500沈積電致變色材料之更詳細態樣描述於前述之美國非臨時專利申請案第12/645,111號及第12/645,159號中。 整合式沈積系統500亦具有建立且維持系統內之受控周圍環境之各種真空泵、氣體入口、壓力感測器及其類似者。此等組件並未展示,而是可為一般熟習此項技術者所瞭解。系統500(例如)係經由圖5中由LCD及鍵盤535所表示之電腦系統或其他控制器控制。一般熟習此項技術者將瞭解,本發明之實施例可使用涉及儲存於一或多個電腦系統或經由一或多個電腦系統傳送之資料之各種製程。本發明之實施例亦係關於用於執行此等操作之設備、此等電腦及微控制器。此等設備及製程可用以沈積本發明之方法及經設計以實施該等方法之設備之電致變色材料。本發明之控制設備可經特殊建構以用於所需目的,或該控制設備可為通用電腦,其藉由儲存於該電腦中之電腦程式及/或資料結構而選擇性地啟動或重配置。本文中所呈現之該等程序並不固有地與任何特定電腦或其他設備相關。詳言之,各種通用機器可與根據本文中之教示撰寫之程式一起使用,或其對建構更特定設備以執行及/或控制所需方法及程序而言可能更便利。 自以上(特別是圖3A至圖3B之)描述可見,利用本發明之方法,吾人不僅可製造電致變色裝置,而且可預先製造分層堆疊(例如,400、403及409),其在一些情況下可經由例如本文中所描述之後續處理轉換成電致變色裝置。儘管由於在EC層與CE層之間不具有離子傳導且電絕緣之區而並非功能性電致變色裝置,但此等「電致變色裝置前驅物」可具有特別價值。在裝置前驅物係以高純度在如本文中所描述之整合式處理設備中製造之情況下尤其如此,其中材料層全部在(例如)真空始終未被破壞之受控周圍環境下沈積。以此方式,高純度之低缺陷材料經堆疊且基本上(例如)在離開整合式系統之前由最後TCO層及/或罩蓋層「密封」。 與上述之本發明之電致變色裝置一樣,電致變色裝置前驅物亦可包括諸如一或多個被動層之一或多個額外層(未圖示)(例如)以改良特定光學性質(提供防潮或抗刮性)以氣密式地密封該裝置前驅物及其類似物。在一實施例中,罩蓋層沈積於該前驅物堆疊之TCO層上。在一些實施例中,該罩蓋層為SiAlO。在一些實施例中,該罩蓋層係藉由濺鍍沈積。在一實施例中,罩蓋層之厚度在約30 nm與約100 nm之間。對處於適當位置之頂蓋層之後續處理形成IC層而無來自環境之污染,亦即,具有罩蓋層之額外保護。 至功能性電致變色裝置之轉換必要時可在該整合式系統之外發生,此係因為內部堆疊結構受保護而不受外部環境影響,且稍微較低嚴格純度之條件係用以將前驅物堆疊轉換成功能性裝置之最末調節步驟所必需的。此等堆疊之電致變色裝置前驅物可具有優點,例如,歸因於僅在需要時轉換至電致變色裝置之較長壽命、由具有(例如)可儲存且在轉換參數取決於最後產品之需要及必須滿足之品質標準而改良或饋送至不同轉換腔室及/或消費點以用於轉換時使用之單一前驅物堆疊導致之靈活性。又,此等前驅物堆疊可用於測試目的,例如,品質控制或研究努力。 因此,本發明之一實施例為一種電致變色裝置前驅物,其包括:(a)基板;(b)該基板上之第一透明導電氧化物層;(c)該第一透明導電氧化物層上之堆疊,該堆疊包括:(i)包括電致變色材料之電致變色層,及(ii)包括對向電極材料之對向電極層;其中該堆疊不包括介於該電致變色層與該對向電極層之間的離子傳導且電絕緣之區;及(d)在該堆疊之上之第二透明導電氧化物層。在一實施例中,該電致變色層包括氧化鎢,且該對向電極層包含氧化鎳鎢。在一實施例中,該堆疊及該電致變色層中之至少一者含有鋰。在另一實施例中,該電致變色層為至少在與該對向電極層之界面處具有超化學計量之含氧量之氧化鎢。在另一實施例中,該堆疊包括在該對向電極層與該電致變色層之間的IC前驅物層,該IC前驅物層包括具有比該電致變色層之含氧量高的含氧量之氧化鎢。在一實施例中,在於EC層與CE層之間不存在IC前驅物層之情況下,該電致變色層之厚度在約500 nm與約600 nm之間,且該對向電極層之厚度在約150 nm與約300 nm之間。在另一實施例中,在於EC層與CE層之間存在IC前驅物層之情況下,該電致變色層之厚度在約350 nm與約400 nm之間,該IC前驅物層之厚度在約20 nm與約100 nm之間,且該對向電極層之厚度在約150 nm與約300 nm之間。在一實施例中,本文中所描述之前驅物裝置曝露於加熱以將該等裝置轉換成功能性電致變色裝置。在一實施例中,加熱為MTCC之部分。 另一實施例為一種電致變色裝置,其包括:(a)包括電致變色材料之電致變色層;及(b)包括對向電極材料之對向電極層,其中該裝置不含有在該電致變色層與該對向電極之間的電絕緣離子傳導材料之組成上均質之層。在一實施例中,該電致變色材料為氧化鎢,該對向電極材料為氧化鎳鎢,且介於該電致變色層與該對向電極層之間的為包括鎢酸鋰與氧化鎢及氧化鎳鎢中之至少一者之混合物之界面區。在另一實施例中,該電致變色層之厚度在約300 nm與約500 nm之間;該界面區之厚度在約10 nm與約150 nm之間,且該對向電極層之厚度在約150 nm與約300 nm之間。 實例圖6為用作用於製造本發明之電致變色裝置之方案之程序流程之曲線圖。 y軸單位為光學密度,且 x軸單位為時間/程序流程。在此實例中,製造類似於關於圖4A所描述之電致變色裝置之電致變色裝置,其中基板為以經氟化之氧化錫作為第一TCO之玻璃,EC層為基質中具有過量氧之WO 3(例如,使用鎢標靶濺鍍,其中濺鍍氣體為約60%之O 2及約40%之Ar),CE層形成於EC層之上且由NiWO製成,且第二TCO為氧化銦錫(ITO)。將鋰用作用於電致變色過渡之離子源。 光學密度用以在電致變色裝置之製造期間判定終點。自曲線圖之原點開始,隨著EC層(WO 3)沈積在基板(玻璃+ TCO)上,量測光學密度。玻璃基板之光學密度具有為約0.07(吸光度單位)之基線值光學密度。隨著EC層建置,光學密度自該點增加,因為氧化鎢(雖然實質上透明)吸收一些可見光。針對約550 nm厚之氧化鎢層之所要厚度,如上所述,光學密度上升至約0.2。在沈積氧化鎢EC層之後,在EC層上濺鍍鋰,如「Li」指示之第一時間週期所指示。在此週期期間,光學密度沿著曲線進一步增加至0.4,其指示氧化鎢之盲電荷已得到滿足,此係因為氧化鎢隨著鋰添加而著色。「NiWO」指示之時間週期指示NiWO層之沈積,光學密度在此期間增加,此係因為NiWO經著色。由於約230 nm厚之NiWO層之添加,光學密度在NiWO沈積期間自約0.4進一步增加至約0.9。請注意,隨著NiWO沈積,一些鋰可自EC層擴散至CE層。此用來在NiWO沈積期間或至少在沈積之初始階段期間將光學密度維持在相對較低值。 「Li」指示之第二時間週期指示鋰至NiWO EC層之添加。光學密度在此階段期間自約0.9減小至約0.4,此係因為NiWO之鋰化使NiWO褪色。進行鋰化,直至NiWO褪色(包括約0.4光學密度之局部最小值)。光學密度在約0.4開始回升,此係因為WO 3層仍被鋰化且影響光學密度。接下來,如時間週期「額外Li」所指示,將額外鋰濺鍍至NiWO層上,在此實例中,與添加至NiWO之鋰相比約10%之額外鋰使NiWO層褪色。在此階段期間,光學密度稍微增加。接下來,添加氧化銦錫TCO,如曲線圖中「ITO」所指示。再次,光學密度在氧化銦錫層之形成期間繼續稍微上升至約0.6。接下來,如「MSTCC」指示之時間週期所指示,在Ar下將裝置加熱至約250℃歷時約15分鐘,且接著在O 2下加熱約5分鐘。接著,在空氣中在約300℃下將裝置退火歷時約30分鐘。在此時間期間,光學密度減小至約0.4。因此,光學密度為用於製造本發明之裝置(例如,用於基於所沈積之材料及形態判定層厚度,且尤其用於將鋰滴定至各種層上以用於滿足盲電荷及/或達到褪色狀態)之有用工具。 與關於圖6所描述之方案一致,圖7展示使用本發明之方法製造的電致變色裝置700之橫截面TEM。裝置700具有玻璃基板702,電致變色堆疊714形成於該玻璃基板上。基板702具有充當第一TCO之ITO層704。氧化鎢EC層706沈積於TCO 704上。層706以約550 nm之厚度形成(亦即,利用氧氣及氬氣經由濺鍍鎢形成之WO 3),如上文關於圖6所描述。將鋰添加至EC層。接著,添加約230 nm厚之NiWO CE層710,繼而添加鋰以褪色且接著添加約10%過量之鋰。最後,沈積氧化銦錫層712,且使堆疊經受多步驟熱化學調節,如上文關於圖4A所描述。在MSTCC之後,進行此TEM。如所見,形成離子傳導電絕緣之新區708。 圖7亦展示各種層之五個選定區域電子繞射(SAED)圖案。首先,704a指示ITO層為高度晶形的。圖案706a展示EC層為多晶的。圖案708a展示IC層為實質上非晶形的。圖案710a展示CE層為多晶的。最後,圖案712a展示氧化銦錫TCO層為高度晶形的。 圖8為藉由掃描透射電子顯微鏡(STEM)分析的本發明之裝置800之橫截面。在此實例中,與關於圖4B描述之方案一致,裝置800係使用本發明之方法製造。裝置800為形成於玻璃基板(未標記)上之電致變色堆疊。在該玻璃基板上的是經氟化之氧化錫層804,其充當第一TCO(對透明電子導體而言,該層有時被稱為「TEC」層)。氧化鎢EC層806沈積於TCO 804上。在此實例中,層806以約400 nm之厚度形成(亦即,利用氧氣及氬氣經由濺鍍鎢形成之WO 3,如上文關於圖6所描述),接著沈積富氧前驅物層805至約150 nm之厚度。將鋰添加至層805。接著,添加約230 nm厚之NiWO CE層810,繼而添加鋰以褪色且接著添加約10%過量之鋰。最後,沈積氧化銦錫層812且使堆疊經受多步驟熱化學調節,如上文關於圖4B所描述。在MSTCC之後,進行此STEM。如所見,形成離子傳導電絕緣之新區808。此實例與關於圖4B所描述之實施例之間的差異在於,不同於圖4B中之類似層405,富氧層805僅部分地轉換成界面區808。在此情況下,150 nm之富氧前驅物層405中僅約40 nm轉換成充當離子傳導層之區。 圖8B及圖8C展示本發明之裝置800(圖8C)與如STEM所分析的在多步驟熱化學調節之前的裝置前驅物(圖8B)之「前後」比較。在此實例中,僅描繪層804-810(EC至CE)。該等層與圖8A中相同地編號,但有些例外。圖8B中之點線用以大致地區分EC層806與富氧層805之界面(此在圖8C中更清楚)。再次參看圖8B,看起來至少存在集中在富氧層805與CE層810之界面處之鋰(大致10-15 nm厚之區),如808a所指示。在MTCC之後(圖8C),很明顯,界面區808已形成。 雖然已稍微詳細地描述前述發明以促進理解,但所描述之實施例應視為說明性而非限制性的。一般熟習此項技術者將顯而易見,在附加申請專利範圍之範疇內,可實踐特定變化及修改。 This application claims the benefit and priority of U.S. Application Nos. 12/772,055 and 12/772,075, each filed April 30, 2010, and entitled "Electrochromic Devices," which applications Each of which is incorporated by reference in its entirety. The following detailed description can be more fully understood when considered in conjunction with the accompanying drawings. FIG. 1A is a schematic cross-section depicting a conventional electrochromic device stack 100 . The electrochromic device 100 includes a substrate 102 , a conductive layer (CL) 104 , an electrochromic (EC) layer 106 , an ion conducting (IC) layer 108 , a counter electrode (CE) layer 110 and a conductive layer (CL) 112 . Elements 104 , 106 , 108 , 110 , and 112 are collectively referred to as electrochromic stack 114 . Typically, these CL layers are made of transparent conductive oxides and are often referred to as "TCO" layers. Since the TCO layer is transparent, the coloring behavior of the EC-IC-CE stack can be observed, for example, through the TCO layer, allowing the use of these devices on windows for reversible shading. A voltage source 116 operable to apply a potential across the electrochromic stack 114 effects the transition of the electrochromic device from, for example, a faded state (ie, transparent) to a colored state. The order of the layers can be reversed with respect to the substrate. That is, the layers may be in the following order: substrate, transparent conductive layer, counter electrode layer, ion-conducting layer, electrochromic material layer and (another) transparent conductive layer. Referring again to FIG. 1A , in a conventional method of fabricating an electrochromic stack, individual layers are deposited on top of one another in a sequential format as depicted in the schematic diagram on the left side of FIG. 1A . That is, the TCO layer 104 is deposited on the substrate 102 . Next, an EC layer 106 is deposited on the TCO 104 . Next, an IC layer 108 is deposited on the EC layer 106 , followed by a CE layer 110 deposited on the IC layer 108 , and finally a TCO layer 112 deposited on the CE layer 110 to form the electrochromic device 100 . Of course, the order of the steps can be reversed to form a "reverse" stack, but the point is that in conventional methods, the IC layer must be deposited on the EC layer followed by the CE layer deposited on the IC layer, or the IC layer deposited on the On the CE layer, followed by the EC layer is deposited on the IC layer. The transitions between layers of material in the stack are abrupt. One of the significant challenges of the above process is the processing required to form the IC layer. In some previous approaches, the IC layer was formed by a sol-gel process that was difficult to incorporate into the CVD or PVD processes used to form the EC and CE layers. Furthermore, IC layers produced by sol-gel and other liquid-based processes are prone to have defects that degrade the quality of the device and may need to be removed by, for example, engraving. In other approaches, IC layers are deposited by PVD from ceramic targets which can be difficult to manufacture and use. 1B is a graph depicting material % composition versus position in the electrochromic stack of FIG. 1A (ie, layers 106, 108, and 110, ie, the EC layer, the IC layer, and the CE layer). As mentioned, in conventional electrochromic stacks, the transitions between material layers in the stack are abrupt. For example, EC material 106 is deposited as a distinct layer with little or no composition bleed to adjacent IC layers. Similarly, IC material 108 and CE material 110 are compositionally distinct with little or no percolation to adjacent layers. Thus, these materials are substantially homogeneous (except for certain compositions of CE materials described below) and have abrupt interfaces. The conventional thinking is that each of the three layers should be laid down as distinct uniformly deposited and smooth layers to form a stack. The interface between each layer should be "clear" where there is little intermingling of materials from each layer at the interface. Those of ordinary skill in the art will recognize that FIG. 1B is an idealized depiction and that, in a practical sense, there is a certain degree of unavoidable mixing of materials at the layer interfaces. The point is that any such mixing is unintentional and minimal in conventional manufacturing methods. The inventors have discovered that an interfacial region can be formed that acts as an IC layer, wherein the interfacial region intentionally includes a substantial amount of one or more electrochromic materials and/or counter electrode materials. This is a fundamental departure from known manufacturing methods. As mentioned above, the inventors have discovered that the formation of the EC-IC-CE stack does not have to be done in the conventional sequence (EC→IC→CE or CE→IC→EC), but can be done between the electrochromic layer and the opposing Deposition of the electrode layers is followed by the formation of an interfacial region that acts as an ion-conducting layer. That is, the EC-CE (or CE-EC) stack is formed first, then the layers (and/or another electrochromic material or counter electrode material in some embodiments) are applied at the interface of the layers ) form an interfacial region (which may possess at least some of the functions of the IC layer) between the EC layer and the CE layer. The interfacial region serves at least some of the functions of conventional IC layers in that the interfacial region is substantially ionically conductive and substantially electrically insulating. It should be noted, however, that the interfacial region as described may have leakage currents higher than conventionally accepted leakage currents, but nevertheless these devices show good performance. In one embodiment, the electrochromic layer is formed with an oxygen-rich region that, after deposition of the counter electrode layer, is converted to act as an interfacial region or layer of the IC layer in subsequent processing. In some embodiments, a dissimilar layer comprising an oxygen-rich version of the electrochromic material is used to (eventually) form an interface layer between the EC layer and the CE layer that acts as the IC layer. In other embodiments, a dissimilar layer comprising an oxygen-rich version of the counter electrode material is used to (eventually) form an interfacial region between the EC layer and the CE layer that acts as the IC layer. All or part of the oxygen-enriched CE layer is converted into an interfacial region. In other embodiments, a distinct layer comprising an oxygen-enriched version of the counter electrode material and an oxygen-enriched version of the electrochromic material is used to (eventually) form an interfacial region between the EC layer and the CE layer that acts as the IC layer. In other words, some or all of the oxygen-rich material acts as a precursor to the interfacial region of the IC layer. The method of the present invention not only reduces processing steps, but also results in electrochromic devices exhibiting improved performance characteristics. As mentioned, it is believed that some of the EC layer and/or CE layer in the interfacial region is converted to provide one or more functions of the IC layer (in particular high conductivity for ions and high resistivity for electrons) The material. The IC functional material in the interfacial region can be, for example, a salt of a conductive cation; for example, a lithium salt. 2A, 2B, and 2C show compositional graphs for three possible examples of electrochromic device stacks (each containing an EC layer, a CE layer, and an interfacial region serving as an IC layer), where the EC material is tungsten oxide (here denoted is WO 3 , but is intended to include WO x , where x is between about 2.7 and about 3.5, and in one embodiment, x is between about 2.7 and about 2.9), the CE material is nickel tungsten oxide (NiWO), and the interface The region mainly comprises lithium tungstate (represented here as Li 2 WO 4 , in another embodiment, the interfacial region is between about 0.5% and about 50 (atomic) % Li 2 O, between about 5% and about A nanocomposite of between 95% Li2W04 and between about 5 % and about 70% WO3) and some amount of EC material and/or CE material. More generally, an interfacial region typically, but not necessarily, has a heterostructure comprising at least two discrete components represented by distinct phases and/or compositions whose concentrations vary across the width of the interfacial region. For this reason, the interfacial region serving as the IC layer is sometimes referred to herein as a "gradient region," a "heterogeneous IC layer," or a "distributed IC layer." Although described with respect to specific materials, the illustrations in Figures 2A, 2B, and 2C more generally represent variations in the composition of any suitable material for electrochromic devices of the present invention. Figure 2A depicts an electrochromic stack of the present invention where the EC material is an important component serving as the interfacial region of the IC layer and the CE material is not. Referring to FIG. 2A , starting from the origin and moving from left to right along the x -axis, one can see that a portion of the EC material WO 3 , which is substantially all tungsten oxide, acts as the EC layer. There is a transition into the interfacial region where there is progressively less tungsten oxide and correspondingly more lithium tungstate up to and including near the end of the interfacial region where there is a substantial amount of tungsten oxide with some minimum amount All of the above are parts of lithium tungstate. Although the transition from the EC layer to the interfacial region is distinguished by a composition of substantially all tungsten oxide and a minimal amount of lithium tungstate, it is apparent that the transition is not as abrupt as in conventional devices. In this example, in fact, the transition begins with the composition having a sufficient amount of lithium tungstate to enable the material to perform at least some of the functions of the IC layer, such as ion conduction and electrical insulation. Undoubtedly, compositions closer to the CE layer, where the composition is essentially lithium tungstate, function as the IC layer, since lithium tungstate is known to exhibit such properties. But there is also some IC layer function in other parts of the interface region. The inventors have found that such "heterogeneous IC layers" improve the switching characteristics and possibly thermal cycling stability of electrochromic devices compared to conventional devices with abrupt transitions. The CE layer in this example mainly contains nickel-tungsten oxide as the active material, with a relatively abrupt transition to the nickel-tungsten oxide composition at the edge of the interfacial region. Methods for fabricating stacks with such interfacial regions are described in more detail below. It should be noted, for example, that the nickel tungsten oxide CE layer in FIG. 2A is depicted as having about 20% lithium tungstate. Without wishing to be bound by theory, it is believed that the nickel tungsten oxide CE layer exists as nickel oxide cores or particles (which impart fairly good ionic conductivity to the CE layer) surrounded by a shell or matrix of lithium tungstate, and thereby in The electrochromic transition of the CE layer is aided during operation of the electrochromic stack. The exact stoichiometry of lithium tungstate in the CE layer can vary significantly between embodiments. In some embodiments, some tungsten oxide may also be present in the CE layer. Also, because lithium ions travel to and from the EC and CE layers through the interfacial region that acts as the IC layer, there may be a significant amount of lithium tungstate in the EC layer, eg, as depicted in Figure 2A. Figure 2B depicts the electrochromic stack of the present invention, where the CE material is an important component serving as the interfacial region of the IC layer, while the EC material is not. Referring to Figure 2B, starting from the origin and moving from left to right along the x -axis, one can see that in this case the EC material, substantially all tungsten oxide, serves as the EC layer. There is an abrupt transition into the interfacial region where there is little, if any, tungsten oxide but a lot of lithium tungstate and at least some nickel tungsten oxide (CE material). The composition of the interfacial region varies along the x -axis with decreasing amounts of lithium tungstate and corresponding increasing amounts of nickel tungsten oxide. The transition from the interfacial region to the CE layer is arbitrarily distinguished by a composition of about 80% nickel tungsten oxide and about 20% lithium tungstate, but this is only one example where the transition occurs with a graded composition. The interfacial region can be considered terminated when no or little additional change in composition occurs upon further processing of the stack. Additionally, the transition actually ends where the composition has a sufficient amount of nickel tungsten oxide such that the material no longer serves at least some of the functions that a dissimilar IC layer could. Undoubtedly, the composition (as distinguished) closer to the CE layer, where the composition is 80% nickel tungsten oxide, functions as the CE layer. Likewise, the composition closer to the interfacial region of the EC layer, in which lithium tungstate is a substantial component, acts as an ionically conductive electrically insulating material. Figure 2C depicts the electrochromic stack of the present invention, where both the EC material and the CE material are important components serving as the interfacial region of the IC layer. Referring to FIG. 2C , starting from the origin and moving from left to right along the x -axis, one can see that a portion of the EC material WO 3 , which is essentially all tungsten oxide, acts as the EC layer. There is a transition into the interfacial region where there is progressively less tungsten oxide and correspondingly more lithium tungstate. In this example, there is also an increased amount of nickel-tungsten oxide counter electrode material approximately one-third of the way through the portion of the zone that divides into the interfacial region. At approximately midway through the portion divided into the interfacial region, there are approximately 10% each of tungsten oxide and nickel tungsten oxide and 80% lithium tungstate. In this example, there is no abrupt transition between the EC layer and the IC layer or between the IC layer and the CE layer, but rather an interfacial region with a continuous graded composition of both CE material and EC material. In this example, the lithium tungstate component peaks about halfway through the interfacial region, and thus, this region is likely to be the most electrically insulating portion of the interfacial region. As mentioned in [Summary of the Invention] above, the EC layer and the CE layer may include material components that impart a certain resistivity to the EC layer and the CE layer; Lithium tungstate of the three regions is one example of such a material that imparts resistivity to the EC and CE layers. Figures 2A-2C represent only three non-limiting examples of graded compositions serving as interfacial regions of the IC layer in electrochromic devices of the present invention. Those of ordinary skill in the art will appreciate that many variations are possible without departing from the scope of the invention. In each of the examples in Figures 2A-2C, there is at least one layer in which there are only two material components and one of those components is a minimum. The present invention is not limited in this way. Accordingly, one embodiment of the invention is an electrochromic device comprising an electrochromic layer, an interfacial region serving as an IC layer, and a counter electrode layer, wherein each of the aforementioned two layers and one region of the device At least one material component thereof is present in each of the electrochromic layer, the interfacial region, and the counter electrode layer in an amount of at least about 25% by weight, and in another embodiment, at least about 15% by weight. % by weight, in another embodiment, at least about 10% by weight, in another embodiment, at least about 5% by weight, in yet another embodiment, at least about 2% by weight. The amount of electrochromic material and/or counter electrode material in the interface region can be significant, in one embodiment, as much as 50% by weight of the interface region. In many embodiments, however, the ionically conductive electrically insulating material is typically the majority component, while the remainder of the interfacial region is the electrochromic material and/or the counter electrode material. In one embodiment, the interfacial region includes between about 60% and about 95% by weight ionically conductive electrically insulating material, while the remainder of the interfacial region is electrochromic material and/or counter electrode material. In one embodiment, the interfacial region includes between about 70% and about 95% by weight ionically conductive electrically insulating material, while the remainder of the interfacial region is electrochromic material and/or counter electrode material. In one embodiment, the interfacial region includes between about 80% and about 95% by weight ionically conductive electrically insulating material, while the remainder of the interfacial region is electrochromic material and/or counter electrode material. In some embodiments, the interfacial regions in the devices described herein may be relatively distinct, that is, there are relatively distinguishable boundaries at adjacent layers when analyzed, for example, by microscopy, even if the interfacial region contains The same is true for a certain amount of electrochromic material and/or counter electrode material. In these embodiments, the thickness of the interface region can be measured. In embodiments where the interface region is formed by an oxygen-rich (superstoichiometric) region of the EC layer and/or CE layer, the ratio of the thickness of the interface region to the layer or layers forming the interface region is used to characterize the interface A measure of the area. For example, an electrochromic layer is deposited with an oxygen-rich upper layer. The EC layer may comprise a single metal oxide or two or more metal oxides mixed homogeneously or heterogeneously in the layer or more diffusion regions. The EC layer is 550 nm thick and includes an oxygen-rich layer (or region). If about 150 nm of the EC layer is converted to the interfacial region, then about 27% of the EC is converted to the interfacial region, ie, 150 nm divided by 550 nm. In another example, the EC layer includes a first metal oxide region (or layer) and an oxygen-enriched second metal oxide layer (or region). If all or a portion of the oxygen-rich metal oxide layer is converted into an interfacial region, the thickness of the interfacial region divided by the total thickness of the first metal oxide layer and the second metal oxide layer (before forming the interfacial region) is Measurement of interface area. In one embodiment, the interfacial region comprises between about 0.5% and about 50% by thickness of precursor regions (EC and/or CE, including oxygen-enriched portions) used to form the interfacial region, in another embodiment Between about 1% and about 30%, in yet another embodiment between about 2% and about 10%, and in another embodiment between about 3% and about 7%. The inventors have discovered that there are a number of benefits to a graded composition acting as an IC layer. While not wishing to be bound by theory, it is believed that by having such graded regions, the efficiency of the electrochromic transition is greatly improved. There are other benefits, as will be described in more detail below. While not wishing to be bound by theory, it is believed that one or more of the following mechanisms may effect the conversion of EC and/or CE materials to IC functional materials in the interfacial region. However, the implementation or application of the invention is not limited to any of these mechanisms. Each of these mechanisms is consistent with a process that never deposits IC layer material during fabrication of the stack. As is clear elsewhere herein, devices of the present invention need not have separate targets comprising materials for the IC layers. In the first mechanism, direct lithiation of the electrochromic material or the counter electrode material results in IC material (eg, lithium tungstate) in the interfacial region. As will be explained more fully below, various embodiments use direct lithiation of one of the active layers at some point in the fabrication process between the formation of the EC and CE layers. This operation involves exposure of the EC layer or the CE layer (whichever is formed first) to lithium. According to this mechanism, the flux of lithium through the EC or CE layer creates ion-conducting electron-resistant materials, such as lithium salts. Heat or other energy can be applied to drive this flux of lithium. This described mechanism converts the top or exposed portion of the first formed layer (EC or CE layer) before forming the second layer (CE or EC layer). In the second mechanism, lithium diffusing from one of EC or CE to the other layer results in EC and/or Part of one of the CEs is converted at its interface to an interface region with IC functional material. The lithium diffusion can occur after the entire second layer has been formed or after only a portion of the second layer has been formed. Furthermore, diffusion of lithium and subsequent conversion to IC functional material takes place in the first or the second deposited layer and in the EC or CE layer. In one example, an EC layer is formed first, and then the EC layer is lithiated. When the CE layer is subsequently deposited over the EC layer, some lithium diffuses from the underlying EC layer toward and/or into the CE layer, resulting in conversion to an interfacial region containing the IC functional material. In another example, the EC layer is formed first (optionally with an oxygen-rich upper region), then the CE layer is formed and lithiated. Subsequently, some of the lithium from the CE layer diffuses into the EC layer where it forms an interfacial region with IC functional material. In yet another example, an EC layer is deposited first, and then the EC layer is lithiated to produce an IC functional material according to the first mechanism described above. Then, when the CE layer is formed, some lithium diffuses from the underlying EC layer towards the CE layer to create some IC material in the interface region of the CE layer. In this way, the IC functional material resides nominally in both the CE layer and the EC layer next to the interface of the CE layer and the EC layer. In a third mechanism, the EC and CE layers are formed to completion (or at least to the point where the second formed layer is partially completed). Next, the device structure is heated, and the heating converts at least some of the material in the interfacial region into an IC functional material (eg, a lithium salt). Heating (eg, as part of multi-step thermochemical conditioning (MTCC) described further herein) can be performed during deposition or after deposition is complete. In one embodiment, heating is performed after forming the transparent conductive oxide on the stack. In another embodiment, heating is applied after the second layer is partially or fully completed, but before the transparent conductive oxide is applied to the second layer. In some cases, heating is directly and primarily responsible for the transformation. In other cases, heating primarily promotes the diffusion or flow of lithium ions, which creates regions of IC functional material as described in this second mechanism. Finally, in a fourth mechanism, current flowing between the EC layer and the CE layer drives conversion of at least one of the electrochromic material and the counter electrode material into an IC functional material in the interface region. This conversion may occur because, for example, the ion flux associated with the flowing current is so large that it drives the chemical conversion of the EC and/or CE material to the IC material in the interface region. For example, as will be explained below, a large flux of lithium through tungsten oxide in the EC layer can produce lithium tungstate, which acts as an IC material. A lithium flux can be introduced, for example, during the initial activation cycle of a newly formed device. However, this need not be the case, as other opportunities for driving high ion flux may be more appropriate to achieve this conversion. The methods of the present invention can be performed by those of ordinary skill in the art without employing any one or more of the above mechanisms. FIG. 3A is a process flow 300 of the method according to the present invention. In particular, see 305, an EC layer is deposited (on eg the CL of the TCO). Next, see 310, a CE layer is deposited. After depositing the EC and CE layers, then, see 315, an interface region is formed between the EC and CE layers to serve as the IC layer. One embodiment of the present invention is a similar method (not depicted) in which steps 305 and 310 are reversed. The gist of the method is that the interfacial region that acts as the IC layer is formed after the EC and CE layers (in some embodiments, the interfacial region is formed using at least part of one of the EC and CE layers). For this reason, the interfacial region formed in this way is sometimes referred to as the "intrinsic" IC layer. In other embodiments, a dissimilar layer is formed between the EC layer and the CE layer, such as using an EC material or an oxygen-enriched version of the CE material, wherein the layer is again fully or partially converted into an interfacial region after forming the EC and CE layers . Various methods for forming the interface region after forming the EC-CE stack will be described below. Thus, as mentioned, one aspect of the invention is a method of manufacturing an electrochromic device, the method comprising: forming an electrochromic layer comprising an electrochromic material; forming an opposing layer in contact with the electrochromic layer. An electrode layer without first providing an ion-conducting electrically insulating layer between the electrochromic layer and the counter electrode layer, wherein the counter electrode layer includes a counter electrode material; and between the electrochromic layer and the counter electrode layer An interfacial region is formed between the electrode layers, wherein the interfacial region is substantially ionically conductive and substantially electrically insulating. The interfacial region may contain constituent materials of the EC layer, the CE layer, or both. As will be described in more detail below, this interfacial region can be formed in a number of ways. 3B is a graph showing the process flow according to the method described with respect to FIG. 3A (in particular, the process flow for depositing an EC layer, then depositing a CE layer, and finally forming an interfacial region between these layers that acts as an IC layer). Program flow 320 . More specifically, in this example, the EC layer comprises WO3 with various amounts of oxygen (compositions and configurations in particular) ; the CE layer comprises NiWO , the interfacial region comprises Li2WO4 , and the TCO materials of indium tin and fluorinated tin oxide. It should be noted that the layers of the electrochromic device will be described below with respect to solid state materials. Solid state materials are desirable due to reliability, consistent properties and process parameters and device performance. Exemplary solid-state electrochromic devices, methods, and apparatus for making them, as well as methods of making electrochromic windows with such devices, are described in Kozlowski et al., U.S. Nonprovisional Patent Application entitled "Fabrication of Low Defectivity Electrochromic Devices" Ser. No. 12/645,111 and U.S. Nonprovisional Patent Application No. 12/645,159 to Wang et al., entitled "Electrochromic Devices," which are hereby incorporated by reference for all purposes. In particular embodiments, the electrochromic devices of the present invention are all solid state and are fabricated in equipment that allows deposition of one or more layers of the stack in a controlled ambient environment. That is, in equipment where the layers are deposited without leaving the equipment and, for example, without breaking the vacuum between deposition steps, thereby reducing contamination and ultimately improving device performance. In certain embodiments, the apparatus of the present invention does not require a separate target for depositing the IC layer as is required in conventional apparatus. As will be appreciated by those of ordinary skill in the art, the present invention is not limited to these materials and methods, however, in certain embodiments, the materials making up the electrochromic stack and the precursor stack (as described below) are all inorganic, Solid (ie, being in a solid state) or inorganic and solid. Because organic materials tend to degrade over time, such as when exposed to ultraviolet light and heat associated with window applications, inorganic materials offer the advantage of reliable electrochromic stacks that can operate for long periods of time. Solid materials also offer the advantage of not having the contamination and leakage problems that liquid materials often have. It should be understood that any one or more of the layers in the stack may contain some amount of organic material, but in many implementations one or more of the layers contain little or no organic material. The same may be true for liquids that may be present in one or more layers in small amounts. It should also be understood that solid state materials may be deposited or otherwise formed by processes using liquid components, such as certain processes using sol-gel or chemical vapor deposition. Referring again to Figure 3B, see 325, the EC layer of WO 3 is deposited first. 4A-4C are schematic cross-sections depicting formation of electrochromic devices according to particular methods and apparatus of the present invention, and in particular according to program flow 320 . In particular, Figures 4A-4C are used to show three non-limiting examples of how an EC layer comprising WO 3 can be formed as part of a stack where the interfacial region serving as the IC layer is formed after deposition of the other layers of the stack . In each of Figures 4A-4C, the substrate 402, first TCO layer 404, CE layer 410, and second TCO layer 412 are substantially identical. Also, in each of the three embodiments, a stack is formed without an IC layer, and then the stack is further processed to form an interfacial region within the stack that acts as an IC layer, between the EC layer and the CE layer . Referring to each of Figures 4A-4C, hierarchical structures 400, 403, and 409, respectively, are depicted. Each of these layered structures includes a substrate 402 that is, for example, glass. Any material having suitable optical, electrical, thermal and mechanical properties can be used as the substrate 402 . Such substrates include, for example, glass, plastic, and mirror materials. Suitable plastic substrates include, for example, acrylic, polystyrene, polycarbonate, allyldiethylene glycol carbonate, SAN (styrene acrylonitrile copolymer), poly(4-methyl-1- pentene), polyester, polyamide, etc., and preferably, the plastic should be able to withstand high temperature processing conditions. If a plastic substrate is used, it is preferably hardcoated with, for example, a diamond-like protective coating, a silica/polysiloxane abrasion resistant coating, or the like, such as coatings well known in the art of plastic glazing layer for barrier protection and wear protection. Suitable glasses include clear or colored soda lime glass, including soda lime float glass. Glass can be tempered or untempered. In some embodiments, commercially available substrates such as glass substrates contain transparent conductive layer coatings. Examples of such glasses include conductive-coated glass sold under the trademarks TEC Glass™ (Pilkington of Toledo, Ohio) and SUNGATE™ 300 and SUNGATE™ 500 (PPG Industries of Pittsburgh, Pennsylvania). TEC Glass™ is glass coated with a conductive layer of fluorinated tin oxide. In some embodiments, the optical transmittance (ie, the ratio of transmitted radiation or spectrum to incident radiation or spectrum) of substrate 402 is about 90% to 95%, eg, about 90% to 92%. The substrate can be of any thickness as long as it has suitable mechanical properties to support the electrochromic device. While substrate 402 may be of any size, in some embodiments it is about 0.01 mm to 10 mm thick, preferably about 3 mm to 9 mm thick. In some embodiments of the invention, the substrate is architectural glass. Architectural glass is glass used as a building material. Architectural glass is commonly used in commercial buildings, but can also be used in residential buildings, and often (but not necessarily) separates the indoor environment from the outdoor environment. In certain embodiments, the architectural glass is at least 20 inches by 20 inches, and may be larger, for example, up to about 72 inches by 120 inches. Architectural glass is typically at least about 2 mm thick. Architectural glass less than about 3.2 mm thick cannot be tempered. In some embodiments of the invention with architectural glass as the substrate, the substrate can be tempered even after the electrochromic stack has been fabricated on the substrate. In some embodiments where architectural glass is used as the substrate, the substrate is soda lime glass from a tin float line. The percent transmission over the visible spectrum (ie, the overall transmission across the visible spectrum) of architectural glass substrates is typically 80% greater than that of neutral substrates, but it may be lower than that of colored substrates. Preferably, the substrate has a percent transmission over the visible spectrum of at least about 90% (eg, about 90% to 92%). The visible spectrum is the spectrum to which the typical human eye responds, generally from about 380 nm (purple) to about 780 nm (red). In some cases, the glass has a surface roughness between about 10 nm and about 30 nm. In one embodiment, the substrate 402 is a sodium glass with a sodium diffusion barrier (not shown) to prevent the diffusion of sodium ions into the electrochromic device. For purposes of this description, this configuration is referred to as "substrate 402." Referring again to layered structures 400 , 403 , and 409 , a first TCO layer 404 , for example made of fluorinated tin oxide or other suitable material that is conductive and transparent, is deposited over substrate 402 . Transparent conductive oxides include metal oxides and metal oxides doped with one or more metals. Examples of such metal oxides and doped metal oxides include indium oxide, indium tin oxide, doped indium oxide, tin oxide, doped tin oxide, zinc oxide, aluminum zinc oxide, doped Zinc oxide, ruthenium oxide, doped ruthenium oxide and the like. In one embodiment, the second TCO layer has a thickness between about 20 nm and about 1200 nm, in another embodiment between about 100 nm and about 600 nm, in another embodiment, about 350 nm nm thick. The TCO layers should have a suitable sheet resistance ( Rs ) due to the relatively large area spanned by the layers. In some embodiments, the sheet resistance of the TCO layer is between about 5 ohms and about 30 ohms per square. In some embodiments, the sheet resistance of the TCO layer is about 15 ohms per square. In general, it is desired that the sheet resistance of each of the two conductive layers be approximately the same. In one embodiment, the two layers (eg, 404 and 412 ) each have a sheet resistance of about 10-15 ohms per square. Each of the layered structures 400, 403, and 409 includes a stack 414a, 414b, and 414c, respectively, each of which includes a first TCO layer 404, a CE layer 410, and a second TCO layer over a substrate 402. Layer 412. Each of the layered structures 400, 403 and 409 differs in how the EC layer system is formed, which in each case affects the morphology of the resulting interfacial region. Consistent with process flow 320 of FIG. 3B , each of stacks 414 a , 414 b , and 414 c includes an electrochromic layer deposited over first TCO layer 404 . The electrochromic layer can contain any one or more of a number of different electrochromic materials including metal oxides. Such metal oxides include tungsten oxide (WO 3 ), molybdenum oxide (MoO 3 ), niobium oxide (Nb 2 O 5 ), titanium oxide (TiO 2 ), copper oxide (CuO), iridium oxide (Ir 2 O 3 ) , chromium oxide (Cr 2 O 3 ), manganese oxide (Mn 2 O 3 ), vanadium oxide (V 2 O 5 ), nickel oxide (Ni 2 O 3 ), cobalt oxide (Co 2 O 3 ), and the like. In some embodiments, the metal oxide is doped with one or more dopants, such as lithium, sodium, potassium, molybdenum, niobium, vanadium, titanium, and/or other suitable metals or metal-containing compounds. Mixed oxides (eg, W-Mo oxide, WV oxide) may also be used in certain embodiments, ie, the electrochromic layer includes two or more of the aforementioned metal oxides. An electrochromic layer comprising a metal oxide is capable of receiving ions transferred from a counter electrode layer. In some embodiments, tungsten oxide or doped tungsten oxide is used for the electrochromic layer. In one embodiment of the invention, the electrochromic layer is made essentially of WOx, where "x " refers to the atomic ratio of oxygen to tungsten in the electrochromic layer, and x is between about 2.7 and 3.5. It has been suggested that only substoichiometric tungsten oxide exhibits electrochromism; that is, stoichiometric tungsten oxide (WO 3 ) does not exhibit electrochromism. In a more particular embodiment, WO x , where x is less than 3.0 and is at least about 2.7, is used for the electrochromic layer. In another embodiment, the electrochromic layer is WO x , where x is between about 2.7 and about 2.9. Techniques such as Rutherford Backscattering Spectroscopy (RBS) can identify the total number of oxygen atoms including oxygen atoms bonded to tungsten and oxygen atoms not bonded to tungsten. In some instances, tungsten oxide layers (where x is 3 or greater) exhibit electrochromism, possibly due to unbound excess oxygen and substoichiometric tungsten oxide. In another embodiment, the tungsten oxide layer has a stoichiometric amount of oxygen or more, where x is from 3.0 to about 3.5. In some embodiments of the invention, at least a portion of the EC layer has an excess of oxygen. This more highly oxidized region of the EC layer is used as a precursor to form the ion-conducting electrically insulating region that acts as the IC layer. In other embodiments, a dissimilar layer of highly oxidized EC material is formed between the EC layer and the CE layer for eventual conversion at least partially to an ion-conducting electrically insulating interfacial region. In particular embodiments, the tungsten oxide is crystalline, nanocrystalline or amorphous. In some embodiments, tungsten oxide is substantially nanocrystalline and has an average grain size of about 5 nm to 50 nm (or about 5 nm to 20 nm), as characterized by transmission electron microscopy (TEM) . Tungsten oxide morphology or microstructure can also be characterized as nanocrystalline using x-ray diffraction (XRD) and/or electron diffraction such as selected area electron diffraction (SAED). For example, nanocrystalline electrochromic tungsten oxide may be characterized by the following XRD characteristics: a crystal size of about 10 to 100 nm (eg, about 55 nm). In addition, nanocrystalline tungsten oxide can exhibit limited long-range order, eg, about a few (about 5 to 20) tungsten oxide unit cells. Therefore, for convenience, the remainder of the process flow 320 in FIG. 3B will be further described with respect to the first embodiment, including the formation of the EC layer 406 shown in FIG. 4A. Next, the second and third embodiments respectively represented in FIGS. 4B and 4C will be described below, with particular emphasis on the formation and morphology and/or microstructure of their respective EC layers. As mentioned with reference to Figure 3B, see 325, an EC layer is deposited. In a first embodiment (shown in FIG. 4A ), a substantially homogeneous EC layer 406 (comprising WO 3 ) is formed as part of stack 414 a , wherein the EC layer is in direct contact with CE layer 410 . In one embodiment, the EC layer comprises WO3, as described above. In one embodiment, heating is applied during at least a portion of the deposition of WO 3 . In a particular embodiment, several passes are made through the sputtering target, with a portion of the WO3 being deposited on each pass, and after each pass, heat is applied to, for example, the substrate 402 to deposit a layer of WO3 on the deposited layer 406. Adjust WO3 before the next section. In other embodiments, the WO 3 layer can be continuously heated during deposition, and the deposition can be done in a continuous fashion rather than several passes over the sputtering target. In one embodiment, the thickness of the EC layer is between about 300 nm and about 600 nm. As mentioned, the thickness of the EC layer depends on the desired result and the method of forming the IC layer. In the embodiment described with respect to FIG. 4A , the EC layer is between about 500 nm and about 600 nm thick using a tungsten target and includes between about 40% and about 80% O and about 20 % and about A sputtering gas of between 60% Ar sputters WO 3 , and the substrate in which WO 3 is deposited is at least intermittently heated to between about 150° C. and about 450° C. during the formation of the EC layer. In a specific embodiment, the EC layer is about 550 nm thick WO3 sputtered using a tungsten target, wherein the sputtering gas includes about 50% to about 60% O2 and about 40% to about 50% O2 Ar, and the substrate deposited with WO 3 is at least intermittently heated to between about 250° C. and about 350° C. during the formation of the electrochromic layer. In these examples, the WO 3 layer is substantially homogeneous. In one embodiment, WO 3 is substantially polycrystalline. It is believed that heating WO 3 at least intermittently during deposition aids in the formation of polycrystalline forms of WO 3 . As mentioned, many materials are suitable for the EC layer. In general, in electrochromic materials, the coloring (or any optical property, such as a change in absorbance, reflectivity, and transmittance) of an electrochromic material is achieved by reversible ion intercalation (e.g., intercalation) into the material. ) and the corresponding injection of charge-balancing electrons. Typically, a certain fraction of the ions responsible for the optical transition are irreversibly bound together in the electrochromic material. As described herein, some or all of the irreversibly bound ions serve to compensate for a "blind charge" in the material. In most electrochromic materials, suitable ions include lithium ions (Li + ) and hydrogen ions (H + ) (ie, protons). However, in some cases other ions will be suitable. Such ions include, for example, deuterium ions (D + ), sodium ions (Na + ), potassium ions (K + ), calcium ions (Ca ++ ), barium ions (Ba ++ ), strontium ions (Sr ++ ) and magnesium ions (Mg ++ ). In various embodiments described herein, lithium ions are used to generate electrochromism. The intercalation of lithium ions into tungsten oxide (WO 3-y (0<y≤~0.3)) changes tungsten oxide from transparent (discolored state) to blue (colored state). In a typical process where the EC layer comprises or is tungsten oxide, lithium is deposited on the EC layer 406, for example by sputtering, to satisfy blind charging (discussed in more detail below with reference to FIGS. 6 and 7), see FIG. 3B 330 of the program flow. In one embodiment, lithiation is performed in an integrated deposition system in which the vacuum is not broken between deposition steps. It should be noted that in some embodiments lithium is not added at this stage, but can be added after the counter electrode layer is deposited, or in other embodiments lithium is added after the TCO is deposited. Referring again to FIG. 4A , next, a CE layer 410 is deposited on the EC layer 406 . In some embodiments, the counter electrode layer 410 is inorganic and/or solid. The counter electrode layer may comprise one or more of a number of different materials capable of acting as a reservoir for ions when the electrochromic device is in a faded state. During an electrochromic transition initiated by, for example, application of an appropriate potential, the counter electrode layer transfers some or all of the ions it holds to the electrochromic layer, causing the electrochromic layer to change to a colored state. Meanwhile, in the case of NiO and/or NiWO, the counter electrode layer is colored due to loss of ions. In some embodiments, suitable materials for the counter electrode include nickel oxide (NiO), nickel tungsten oxide (NiWO), nickel vanadium oxide, nickel chromium oxide, nickel aluminum oxide, nickel manganese oxide, nickel magnesium oxide, chromium oxide (Cr 2 O 3 ), manganese oxide (MnO 2 ) and Prussian blue. Optical passive counter electrodes include cerium titanium oxide (CeO 2 -TiO 2 ), cerium zirconium oxide (CeO 2 -ZrO 2 ), nickel oxide (NiO), nickel tungsten oxide (NiWO), vanadium oxide (V 2 O 5 ) and A mixture of oxides (for example, a mixture of Ni 2 O 3 and WO 3 ). Doped formulations of these oxides may also be used, where dopants include, for example, tantalum and tungsten. Since the counter electrode layer 410 contains ions for producing the electrochromic phenomenon in the electrochromic material when the electrochromic material is in a faded state, the counter electrode preferably has a high Transmittance and neutral color. The shape of the counter electrode can be crystalline, nanocrystalline or amorphous. In some embodiments, where the counter electrode layer is nickel tungsten oxide, the counter electrode material is amorphous or substantially amorphous. Such substantially amorphous nickel tungsten oxide counter electrodes have been found to perform better under certain conditions than their crystalline counterparts. As described below, the amorphous state of nickel tungsten oxide can be obtained by using specific processing conditions. While not wishing to be bound by any theory or mechanism, it is believed that amorphous nickel-tungsten oxide is produced by relatively high energy atoms in the sputtering process. Higher energy atoms are obtained, for example, in sputtering processes with higher target power, lower chamber pressure (ie, higher vacuum), and smaller source-to-substrate distance. Under the described processing conditions, higher density films with better stability under UV/heat exposure were produced. In certain embodiments, the amount of nickel present in the nickel tungsten oxide may be up to about 90% by weight of the nickel tungsten oxide. In a specific embodiment, the mass ratio of nickel to tungsten in the nickel tungsten oxide is between about 4:6 and 6:4, and in one example is about 1:1. In one embodiment, NiWO includes between about 15 atomic percent and about 60 percent Ni, and between about 10 percent and about 40 percent W. In another embodiment, NiWO comprises between about 30 atomic percent and about 45 percent Ni, and between about 15 percent and about 35 percent W. In another embodiment, NiWO comprises between about 30 atomic percent and about 45 percent Ni, and between about 20 percent and about 30 percent W. In one embodiment, NiWO includes about 42 atomic percent Ni and about 14 percent W. In one embodiment, as described above, see 335 of FIG. 3B , the CE layer 410 is NiWO. In one embodiment, the thickness of the CE layer is between about 150 nm and about 300 nm, in another embodiment between about 200 nm and about 250 nm, in another embodiment about 230 nm. In a typical process, lithium is also applied to the CE layer until the color of the CE layer fades. It should be understood that reference to transitions between colored and faded states is non-limiting and implies only one example of many possible electrochromic transitions that may be implemented. Unless otherwise stated herein, whenever a fade-to-color transition is mentioned, the corresponding device or process encompasses other optical state transitions such as non-reflective-reflective, transparent-opaque, and the like. In addition, the term "faded" refers to an optically neutral state, such as uncolored, transparent or translucent. Still further, unless otherwise stated herein, the "color" of an electrochromic transition is not limited to any particular wavelength or range of wavelengths. As is generally understood by those skilled in the art, selection of appropriate electrochromic materials and counter electrode materials governs the associated optical transition. In a particular embodiment, see 340 of FIG. 3B , lithium is added (eg, via sputtering) to the NiWO CE layer. In a particular embodiment, see 345 of FIG. 3B , an additional amount of lithium is added after enough lithium has been introduced to completely decolorize the NiWO (this procedure is optional, and in one embodiment, is not used at this stage of the procedure. Add excess lithium). In one embodiment, the additional amount is between about 5% and about 15% excess based on the amount needed to discolor the counter electrode layer. In another embodiment, the excess lithium added to the CE layer is about a 10% excess based on the amount needed to discolor the counter electrode layer. After depositing the CE layer 410, decolorizing it with lithium, and adding additional lithium, see 350 of FIG. 3B, a second TCO layer 412 is deposited over the counter electrode layer. In one embodiment, the transparent conductive oxide includes indium tin oxide, and in another embodiment, the TCO layer is indium tin oxide. In one embodiment, the thickness of this second TCO layer is between about 20 nm and about 1200 nm, in another embodiment between about 100 nm and about 600 nm, in another embodiment about 350 nm nm. Referring again to FIG. 4A, once layered structure 400 is complete, it is subjected to thermochemical conditioning that converts at least a portion of stack 414a into an IC layer (if it has not been converted due to lithium diffusion or other mechanisms). Stack 414a is a precursor and not an electrochromic device because it does not yet have an ionically conductive/electrically insulating layer (or region) between EC layer 406 and CE layer 410 . In this particular embodiment, a portion of the EC layer 406 is converted to an IC layer 408 to form a functional electrochromic device 401 in a two-step process. Referring to Figure 3B, see 355, the layered structure 400 is subject to MTCC. In one embodiment, the stack is first subjected to heating at between about 150° C. and about 450° C. for between about 10 minutes and about 30 minutes under an inert atmosphere (eg, argon), and then heated under O for Between about 1 minute and about 15 minutes. In another embodiment, the stack is heated at about 250° C. under an inert atmosphere for about 15 minutes, and then heated under O 2 for about 5 minutes. Next, layered structure 400 is subjected to heating in air. In one embodiment, the stack is heated in air at between about 250° C. and about 350° C. for between about 20 minutes and about 40 minutes. In another embodiment, the stack is heated in air at about 300° C. Heating took about 30 minutes. The energy required to implement MTCC need not be radiant heat energy. For example, in one embodiment, MTCC is implemented using ultraviolet radiation. Other energy sources may also be used without departing from the scope of the present invention. After the multi-step thermochemical conditioning, program flow 320 is complete and a functional electrochromic device is established. As mentioned, and while not wishing to be bound by theory, it is believed that the lithium in stack 414a combines with a portion of EC layer 406 and/or CE layer 410 to form interfacial region 408 which acts as an IC layer. It is believed that the interface region 408 is mainly lithium tungstate (Li 2 WO 4 ), which is known to have good ion-conducting and electrical-insulating properties compared to conventional IC layer materials. As discussed above, it is not clearly known how this phenomenon occurs. There are chemical reactions that must occur during the multi-step thermochemical conditioning to form the ion-conducting electrically insulating region 408 between the EC layer and the CE layer, but it is also believed that the initial flux of lithium traveling through the stack (e.g., by The excess lithium added to the CE layer (provided) plays a role in the formation of the IC layer 408 . The thickness of the ion-conducting electrically insulating region can vary depending on the materials used and the processing conditions used to form the layer. In some embodiments, the interfacial region 408 has a thickness between about 10 nm and about 150 nm, in another embodiment between about 20 nm and about 100 nm, and in other embodiments between about 30 nm and about 100 nm. between about 50 nm. As mentioned above, there are many suitable materials for forming the EC layer. Thus, using, for example, lithium or other suitable ions in the above method, one can make other interfacial regions that serve as IC layers starting from oxygen-enriched EC materials. Suitable EC materials for this purpose include, but are not limited to, SiO2 , Nb2O5 , Ta2O5 , TiO2 , ZrO2 , and CeO2 . In particular embodiments using lithium ions, ion-conducting materials such as, but not limited to, lithium silicate, lithium aluminum silicate, lithium aluminum borate, lithium aluminum fluoride, lithium borate, lithium nitride, lithium zirconium silicate, Lithium niobate, lithium borosilicate, lithium phosphosilicate, and other such lithium-based ceramic materials, silica or silicon oxide (including lithium silicon oxide) can be made to act as the interfacial region of the IC layer. As mentioned, in one embodiment, the precursor to the ion-conducting region is an oxygen-rich (superstoichiometric) layer converted to an ion-conducting/electrically insulating region via lithiation and MTCC as described herein. While not wishing to be bound by theory, it is believed that after lithiation, excess oxygen forms lithium oxide, which further forms lithium salts (i.e., lithium electrolytes), such as lithium tungstate ( Li2WO4 ) , lithium molybdate (Li 2 MoO 4 ), lithium niobate (LiNbO 3 ), lithium tantalate (LiTaO 3 ), lithium titanate (Li 2 TiO 3 ), lithium zirconate (Li 2 ZrO 3 ), and the like. In one embodiment, the interface region includes at least one of the following: tungsten oxide (WO 3+x , 0≤x≤1.5), molybdenum oxide (MoO 3+x , 0≤x≤1.5), niobium oxide (Nb 2 O 5+x , 0≤x≤2), titanium oxide (TiO 2+x , 0≤x≤1.5), tantalum oxide (Ta 2 O 5+x , 0≤x≤2), zirconia ( ZrO 2+x , 0≤x≤1.5) and cerium oxide (CeO 2+x , 0≤x≤1.5). However, any material can be used for the ion-conducting interfacial region as long as the material can be fabricated to have a low degree of defectivity and it allows the passage of ions between the counter electrode layer 410 and the electrochromic layer 406 while substantially preventing the passage of electrons. Can. The material can be characterized as substantially conducting ions and substantially resisting electrons. In one embodiment, the ionic conductor material has an ionic conductivity between about 10 −10 Siemens/cm (or ohm −1 cm −1 ) and about 10 −3 Siemens/cm and greater than 10 5 ohm-cm resistivity. In another embodiment, the ionic conductor material has an ionic conductivity between about 10 −8 Siemens/cm and about 10 −3 Siemens/cm and a resistivity greater than 10 10 ohm-cm. While ionically conducting layers should be substantially resistant to leakage current (e.g., providing a leakage current of no greater than about 15 μA/cm), it has been found that some devices fabricated as described herein have surprisingly high leakage currents (e.g., , between about 40 μA/cm and about 150 μA/cm), yet still provide good color variation across the device and operate efficiently. As mentioned above, there are at least two other ways of creating an ionically conductive electrically insulating region between the EC layer and the CE layer after forming the stack. These additional embodiments will be described below with reference to the specific example of using tungsten oxide for the IC layer. Also, as mentioned above, interfacial regions with IC properties can be formed in situ during fabrication of the stack when, for example, lithium diffusion or heat converts some of the EC and/or CE layers into interfacial regions. In general, there are particular benefits to establishing ion-conducting regions later in the process. First, the ion-conducting material can be protected from some of the harsh processing that occurs during deposition and lithiation of the EC and CE layers. For example, depositing these layers by a plasma process is often accompanied by a large voltage drop immediately after the stack, often in the order of 15-20 volts. These large voltages can damage or cause decomposition of sensitive ion-conducting materials. By moving IC material formation to a later stage in the process, the material is not exposed to potentially damaging voltage extremes. Second, by forming the IC material later in the process, we can better control some processing conditions that were not possible before completing both the EC and CE layers. These conditions include lithium diffusion and current flow between the electrodes. Controlling these and other conditions late in the process provides additional flexibility in tailoring the physical and chemical properties of IC materials to specific applications. Thus, not all of the benefits of the present invention are due to the unique interfacial region serving as the IC layer, ie, there are manufacturing and other benefits as well. It has been observed that ion-conducting materials formed according to some of the embodiments described herein have superior efficacy. For example, it has been found that the device switching speed is very fast (eg, less than 10 minutes, in one example about 8 minutes) to achieve about 80% final state, compared to 20-25 minutes or more for conventional devices. In some examples, the devices described herein have switching speeds that are orders of magnitude better than conventional devices. This may be attributable to a larger amount of lithium disposed in the interfacial region and/or in the graded interface that can be easily transferred (eg, between the EC and the interfacial region and/or between the CE and the interfacial region). Such lithium may be in the EC and/or CE phase intermingled with the IC present in the interfacial region. It may also be due to the relatively thin layer or network of IC material present in the interfacial region. In support of this notion, it has been observed that some devices fabricated according to the teachings herein have high leakage current, yet surprisingly exhibit good color change and good efficiency. In some cases, robustly performing devices have been found to have leakage current densities of at least about 100 μA/cm. Referring now to FIG. 4B, in a second embodiment, the initially deposited EC material of the stack 414b is actually two layers: a first WO3 layer 406, which is similar to layer 406 in FIG. 4A, but is about 350 nm thick. Between about 450 nm and about 450 nm, the first layer is sputtered using a tungsten target and a first sputtering gas comprising between about 40% and about 80% O and between about 20 % and about 60% Ar and a second WO 3 layer 405 having a thickness between about 100 nm and about 200 nm, the second layer using a tungsten target and comprising between about 70% and 100% O 2 and between 0% and about 30% The second sputtering gas sputtering with Ar between %. In this embodiment, heat is applied by at least intermittently heating the substrate 402 to between about 150° C. and about 450° C. during the deposition of the first WO 3 layer 406 , but during the deposition of the second WO 3 layer 405 No heating or substantially no heating during the period. In a more particular embodiment, layer 406 is about 400 nm thick, and the first sputtering gas includes between about 50% and about 60% O2 and between about 40% and about 50% Ar; The second WO 3 layer 405 is about 150 nm thick, and the second sputtering gas is substantially pure O 2 . In this embodiment, heat is applied at least intermittently to between about 200° C. and about 350° C. during the formation of the first WO 3 layer 406 , but no heat or substantially no heat is applied during the formation of the second WO 3 layer 405 . heating. In this way, the first WO 3 layer is substantially polycrystalline, while the second WO 3 layer need not be. Referring again to FIG. 4B, as described above with respect to FIGS. 3B and 4A, the stack is completed by lithiation of EC layers 406 and 405 to substantially or substantially satisfy the blind charge, deposition of CE layer 410, lithiation of CE layer To a faded state, additional lithium is added and a second TCO layer 412 is deposited to complete the layered stack 403 . Similar thermochemical adjustments are performed on layered stack 403 to provide layered stack 407, a functional electrochromic device including ion-conducting electrically insulating region 408a. While not wishing to be bound by theory, in this example it is believed that the oxygen-rich layer 405 of WO 3 acts primarily as a source of precursor material to form the interfacial region 408a. In this example, the entire oxygen-enriched WO 3 layer is depicted as converting into interfacial region 408a, however, it has been found that this is not always the case. In some embodiments, only a portion of the oxygen-rich layer is converted to form an interfacial region that functions as an IC layer. Referring now to FIG. 4C, in a third embodiment, layered stack 409 includes EC layer 406a (which has a graded composition of WO 3 and is formed as part of stack 414c), wherein the graded composition includes varying amounts of oxygen. In a non-limiting example, there is a higher oxygen concentration in the EC layer 406a at the interface of the EC-CE layer (410) than at the interface of the TCO layer 404 and the EC layer 406a. In one embodiment, the EC layer 406a is a graded composition WO 3 layer sputtered with a tungsten target and a sputtering gas with a thickness between about 500 nm and about 600 nm, wherein the sputtering gas The color changing layer initially comprises between about 40% and about 80% O and between about 20 % and about 60% Ar, and the sputtering gas comprises about 70% and Ar at the end of sputtering the electrochromic layer. Between 100% O and between 0 % and about 30% Ar, and wherein heat is applied to the substrate 402, for example, to about 150°C and about 450°C at least intermittently during the initiation of the formation of the EC layer 406a In between, but not or substantially not, heat is applied during the deposition of at least a final portion of the EC layer 406a. In a more specific embodiment, the graded composition WO layer is about 550 nm thick; the sputtering gas comprises between about 50% and about 60% O and 40 % O at the start of sputtering the electrochromic layer and about 50% Ar, and the sputtering gas is substantially pure O at the end of sputtering the electrochromic layer ; and wherein heat is applied at least intermittently during the beginning of formation of the electrochromic layer to For example, substrate 402 to between about 200°C and about 350°C, but no or substantially no heat is applied during deposition of at least a final portion of the electrochromic layer. In one embodiment, heat is applied at the temperature range at the beginning of the deposition and is tapered to no heat when about half of the EC layer is deposited, while the sputtering gas composition is along the A substantially linear rate is adjusted from between about 50% and about 60% O2 and between about 40% and about 50% Ar to substantially pure O2 . More generally, the interfacial region typically (but not necessarily) has a heterostructure comprising at least two discrete components represented by different phases and/or compositions. Additionally, the interfacial region may include a gradient among the two or more discrete components, such as an ion-conducting material and an electrochromic material (eg, a mixture of lithium tungstate and tungsten oxide). The gradient can provide, for example, variable composition, microstructure, resistivity, dopant concentration (eg, oxygen concentration), stoichiometry, density, and/or grain size range. The gradient can have transitions of many different forms, including linear transitions, S-shaped transitions, Gaussian transitions, and the like. In one example, the electrochromic layer includes regions of tungsten oxide transitioning into regions of superstoichiometric tungsten oxide. Part or all of the superstoichiometric oxide region is converted into an interfacial region. In the final structure, the tungsten oxide region is substantially polycrystalline, and the microstructure transitions to substantially amorphous at the interface region. In another example, the electrochromic layer includes regions of tungsten oxide transitioning into regions of (superstoichiometric) niobium oxide. Part or all of the niobium oxide region is converted into an interfacial region. In the final structure, the tungsten oxide region is substantially polycrystalline, and the microstructure transitions to substantially amorphous at the interface region. Referring again to FIG. 4C, as described above with respect to FIGS. 3B and 4A, the stacking is accomplished by: lithiation of the EC layer 406a to substantially or substantially satisfy the blind charge, deposition of the CE layer 410, lithiation of the CE layer to a faded state , adding additional lithium and depositing a second TCO layer 412 to complete the layered stack 409 . A similar multi-step thermochemical conditioning is performed on the layered stack 409 to provide the layered stack 411, comprising at least a portion of the ionically conductive electrically insulating region 408b and the original layered EC layer 406a (which serves as the EC in the functional electrochromic device 411 layer) functional electrochromic device. While not wishing to be bound by theory, in this example it is believed that the uppermost oxygen-rich portion of the graded layer of WO 3 primarily forms the graded interfacial region 408b. While not wishing to be bound by theory, it is possible that the formation of the interfacial region is self-limiting and depends on the relative amounts of oxygen, lithium, electrochromic material and/or counter electrode material in the stack. In various embodiments described herein, electrochromic stacks are described as having no or substantially no heating during certain processing stages. In one embodiment, after the heating step, the stack is actively or passively (eg, using a heat sink) cooled. The apparatus of the present invention includes active and passive cooling components, for example, active cooling can include platen cooling by fluid circulation, cooling by exposure to cold (eg, via expansion) gas, refrigeration units, and the like. Passively cooled components may include heat sinks, such as metal blocks and the like, or simply remove the substrate from heat exposure. Another aspect of the present invention is a method of manufacturing an electrochromic device, the method comprising: (a) forming an electrochromic layer comprising an electrochromic material or a counter electrode layer comprising a counter electrode material; (b) An intermediate layer is formed over the electrochromic layer or the counter electrode layer, wherein the intermediate layer includes an oxygen-enriched form of at least one of the electrochromic material, the counter electrode material, and an additional material, wherein the additional material comprising a dissimilar electrochromic material or counter electrode material, wherein the intermediate layer is not substantially electrically insulating; (c) forming the other of the electrochromic layer and the counter electrode layer; and (d ) allows at least a portion of the intermediate layer to become substantially electrically insulating. In one embodiment, the electrochromic material is WO 3 . In another embodiment, (a) includes sputtering WO using a tungsten target and a first sputtering gas comprising between about 40% and about 80% O and between about 20 % and about 60% Ar. 3 to achieve a thickness between about 350 nm and about 450 nm, and at least intermittently heating to between about 150° C. and about 450° C. during formation of the electrochromic layer. In another embodiment, (b) includes a second sputtering without heating using a tungsten target and including between about 70% and 100% O and between 0 % and about 30% Ar The WO 3 is gas sputtered to a thickness between about 100 nm and about 200 nm. In yet another embodiment, the method further comprises sputtering lithium onto the intermediate layer until the blind charge is substantially or substantially satisfied. In one embodiment, the counter electrode layer includes NiWO with a thickness between about 150 nm and about 300 nm. In another embodiment, lithium is sputtered onto the counter electrode layer until the counter electrode layer fades. In another embodiment, an additional amount of lithium is sputtered onto the counter electrode layer between about 5% and about 15% over the amount needed to decolorize the counter electrode layer. In another embodiment, a transparent conductive oxide layer is deposited over the counter electrode layer. In one embodiment, the transparent conductive oxide includes indium tin oxide, and in another embodiment, the transparent conductive oxide is indium tin oxide. In another embodiment, the stack formed according to the above embodiments is heated under Ar at between about 150° C. and about 450° C. for between about 10 minutes and about 30 minutes, and then heated under O for about 1 minutes and about 15 minutes, and then heated in air at between about 250° C. and about 350° C. for between about 20 minutes and about 40 minutes. In another embodiment, (a) comprises a first electrochromic material of sputtered MO x , wherein M is a metal or non-metal element, and x indicates the ratio of stoichiometric oxygen to M, and (b) comprises The second electrochromic material of sputtered NO y is used as an intermediate layer, wherein N is the same or different metal or non-metal element, and y indicates the ratio of superstoichiometric oxygen to N. In one embodiment, M is tungsten and N is tungsten. In another embodiment, M is tungsten, and N is selected from the group consisting of niobium, silicon, tantalum, titanium, zirconium, and cerium. Another embodiment of the present invention is an electrochromic device comprising: (a) an electrochromic layer comprising an electrochromic material; (b) a counter electrode layer comprising a counter electrode material; and (c) an electrochromic layer comprising an electrochromic material; The interface region between the electrochromic layer and the counter electrode layer, wherein the interface region includes an electrically insulating ion-conducting material and at least one of the electrochromic material, the counter electrode material, and an additional material, wherein the Additional materials include dissimilar electrochromic materials or counter electrode materials. In one embodiment, at least one of the electrically insulating ion-conducting material and the electrochromic material, the counter electrode material and the additional material are substantially uniformly distributed within the interface region. In another embodiment, at least one of the electrically insulating ion-conducting material and the electrochromic material, the counter electrode material and the additional material comprises a compositional gradient in a direction perpendicular to the layers. In another embodiment, consistent with any of the two preceding embodiments, the electrically insulating ion-conducting material includes lithium tungstate, the electrochromic material includes tungsten oxide, and the counter electrode material includes nickel tungsten oxide . In a specific implementation of one of the foregoing embodiments, no additional material is present. In one embodiment, the thickness of the electrochromic layer is between about 300 nm and about 500 nm, the thickness of the interface region is between about 10 nm and about 150 nm, and the thickness of the counter electrode layer is about Between 150 nm and about 300 nm. In another embodiment, the thickness of the electrochromic layer is between about 400 nm and about 500 nm; the thickness of the interface region is between about 20 nm and about 100 nm, and the thickness of the counter electrode layer is between Between about 150 nm and about 250 nm. In yet another embodiment, the thickness of the electrochromic layer is between about 400 nm and about 450 nm; the thickness of the interface region is between about 30 nm and about 50 nm, and the thickness of the counter electrode layer is between Between about 200 nm and about 250 nm. Another embodiment is a method of fabricating an electrochromic device, the method comprising: by using a sputtering gas comprising between about 40% and about 80% O and between about 20 % and about 60% Ar sputtering a tungsten target to produce WO3 to a thickness between about 500 nm and about 600 nm to deposit an electrochromic layer, wherein the substrate on which the WO3 is deposited is at least intermittently during formation of the electrochromic layer heating to between about 150° C. and about 450° C.; sputtering lithium onto the electrochromic layer until the blind charge is satisfied; depositing a counter electrode layer on the electrochromic layer without first providing an ion-conducting electrically insulating layer between the electrochromic layer and the counter electrode layer, wherein the counter electrode layer comprises NiWO; sputtering lithium onto the counter electrode layer until the counter electrode layer is substantially discolored; And an interfacial region is formed between the electrochromic layer and the counter electrode layer, wherein the interfacial region is substantially ionically conductive and substantially electrically insulating. In one embodiment, forming the interfacial region includes the stack of MTCCs alone or together with substrate, conductive layer and/or encapsulation layer. The electrochromic device of the present invention may include one or more additional layers (not shown) such as one or more passive layers, for example, to improve certain optical properties (provide moisture or scratch resistance) to hermetically seal Sealing the electrochromic device and the like. Typically, but not necessarily, a capping layer is deposited on the electrochromic stack. In some embodiments, the capping layer is SiAlO. In some embodiments, the capping layer is deposited by sputtering. In one embodiment, the thickness of the capping layer is between about 30 nm and about 100 nm. As should be appreciated from the foregoing discussion, the electrochromic devices of the present invention can be sputtered in a single chamber apparatus (e.g., with, for example, tungsten targets, nickel targets, and lithium targets and oxygen and argon sputtering gases. tool) made in. As mentioned, due to the nature of the interfacial region formed to serve the purpose of a conventional dissimilar IC layer, a separate target for sputtering the IC layer is not necessary. It is of particular interest to the inventors, for example, to fabricate electrochromic devices of the present invention in a high-throughput manner, and therefore it is desirable to have equipment that can sequentially fabricate electrochromic devices of the present invention as substrates pass through an integrated deposition system. For example, the inventors are particularly interested in fabricating electrochromic devices on windows, particularly architectural glass flake windows (described above). Accordingly, another aspect of the invention is an apparatus for fabricating an electrochromic device comprising: an integrated deposition system comprising: (i) a first deposition station containing a material source configured to deposit an electrochromic layer of an electrochromic material; and (ii) a second deposition station configured to deposit a counter electrode layer comprising a counter electrode material; The manner of depositing a stack having an intermediate layer sandwiched between the electrochromic layer and the counter electrode layer delivers the substrate through the first deposition station and the second deposition station; wherein the first deposition Either or both of the station and the second deposition station are also configured to deposit the intermediate layer over the electrochromic layer or the counter electrode layer, and wherein the intermediate layer includes the electrochromic material or the counter electrode layer To an oxygen-enriched form of the electrode material, and wherein the first deposition station and the second deposition station are interconnected in series and are operable to transfer a substrate from one station to the next without exposing the substrate to the external environment. In one embodiment, the apparatus of the present invention is operable to transfer the substrate from one station to the next without breaking vacuum, and may include operable to deposit lithium from a source of lithium-containing material on the electrochromic device. One or more lithiation sites on one or more layers. In one embodiment, the apparatus of the present invention is operable to deposit the electrochromic stack on an architectural glass substrate. In an embodiment, the apparatus is operable to transfer the substrate from one stage to the next without breaking vacuum. In another embodiment, the integrated deposition system further comprises one of or operable to deposit lithium from a lithium-containing material source on at least one of the electrochromic layer, the intermediate layer, and the counter electrode layer. Multiple lithiation stations. In yet another embodiment, the integrated deposition system is operable to deposit the stack on an architectural glass substrate. In another embodiment, the integrated deposition system further includes a substrate holder and a transport mechanism operable to hold the architectural glass substrate in a vertical orientation as the architectural glass substrate is passed through the integrated deposition system. In another embodiment, the apparatus further comprises one or more load locks for transferring the substrate between an external environment and the integrated deposition system. In another embodiment, the apparatus further comprises at least one slit valve operable to permit the one or more lithium deposition stations and at least one of the first deposition station and the second deposition station isolated. In one embodiment, the integrated deposition system includes one or more heaters configured to heat the substrate. 5 depicts a simplified representation of an integrated deposition system 500 in perspective view and includes a cross-sectional view of the interior in more detail. In this example, system 500 is a module in which inlet 502 and outlet 504 are connected to a deposition module 506 . There is an inlet port 510 (the vacuum chamber 504 has a corresponding outlet port) for loading, for example, an architectural glass substrate 525 . Substrates 525 are supported by pallets 520 that travel along rails 515 . In this example, the pallet 520 is supported by the rail 515 via suspension, but the pallet 520 could also be supported on a rail located near the bottom of the apparatus 500 or between the top and bottom of the apparatus 500, for example. top. The pallet 520 can translate forward and/or backward in the system 500 (as indicated by the double-headed arrow). For example, during lithium deposition, the substrate can be moved forward and backward in front of the lithium target 530, resulting in multiple passes to achieve the desired lithiation. However, this functionality is not limited to lithium targets, for example, a tungsten target can be passed multiple times over a substrate, or the substrate can be passed in front of the tungsten target via a forward/backward motion path to deposit, for example, an electrochromic layer. Pallet 520 and substrate 525 are in a substantially vertical orientation. The substantially vertical orientation is not limiting, but it can help prevent defects because particulate matter, which may for example arise from the coalescence of atoms from sputtering, will tend to be gravitational and thus not deposited on the substrate 525 . Also, because architectural glass substrates tend to be large, the vertical orientation of the substrates enables the coating of thinner glass substrates as it traverses the stages of the integrated deposition system because of the effects on thicker thermal glass. There is less concern about sagging. Target 530 , in this case a cylindrical target, is oriented substantially parallel to and in front of the substrate surface on which deposition will occur (other sputtering means are not depicted here for convenience). Substrate 525 may translate past target 530 during deposition, and/or target 530 may move in front of substrate 525 . The path of movement of the target 530 is not limited to translation along the path of the substrate 525 . The target 530 can be rotated along an axis through its length, translated along a path of the substrate (forward and/or backward), translated along a path perpendicular to the path of the substrate, circular in a plane parallel to the substrate 525 path movement, etc. The target 530 need not be cylindrical, it can be flat or any shape needed to deposit the desired layer with the desired properties. Also, there may be more than one target in each deposition station, and/or targets may move between stations depending on the desired process. The various stations of the integrated deposition system of the present invention may be modules, but once connected form a continuous system in which a controlled ambient environment is established and maintained for processing substrates at the various stations within the system. More detailed aspects of how to deposit electrochromic materials using the integrated deposition system 500 are described in the aforementioned US Nonprovisional Patent Application Nos. 12/645,111 and 12/645,159. The integrated deposition system 500 also has various vacuum pumps, gas inlets, pressure sensors, and the like to establish and maintain a controlled ambient environment within the system. Such components are not shown, but would be understood by those of ordinary skill in the art. System 500 is controlled, for example, via a computer system or other controller represented by LCD and keypad 535 in FIG. 5 . Those of ordinary skill in the art will appreciate that embodiments of the invention may employ a variety of processes involving data stored on or transmitted through one or more computer systems. Embodiments of the invention also relate to devices for performing these operations, such computers and microcontrollers. Such equipment and processes can be used to deposit the electrochromic materials of the methods of the present invention and devices designed to carry out the methods. The control device of the present invention may be specially constructed for the required purpose, or the control device may be a general purpose computer selectively activated or reconfigured by computer programs and/or data structures stored in the computer. The programs presented herein are not inherently tied to any particular computer or other device. In particular, various general purpose machines may be used with programs written in accordance with the teachings herein, or it may be more convenient to construct more specific apparatus to execute and/or control the desired methods and programs. As can be seen from the description above (particularly of FIGS. 3A-3B ), using the method of the present invention, one can fabricate not only electrochromic devices, but also pre-fabricated layered stacks (eg, 400, 403, and 409 ), which in some Cases may be converted to electrochromic devices via subsequent processing such as described herein. Such "electrochromic device precursors" may be of particular value, although not functional electrochromic devices because they do not have an ionically conductive and electrically insulating region between the EC layer and the CE layer. This is especially the case where the device precursors are fabricated at high purity in an integrated processing facility as described herein, where the material layers are all deposited in a controlled ambient environment in which the vacuum is never broken, for example. In this way, high-purity low-defect materials are stacked and substantially "sealed," eg, by the final TCO layer and/or capping layer, before leaving the integrated system. As with the electrochromic device of the present invention described above, the electrochromic device precursor may also include one or more additional layers (not shown) such as one or more passive layers (not shown), for example, to modify certain optical properties (providing moisture or scratch resistance) to hermetically seal the device precursors and the like. In one embodiment, a capping layer is deposited on the TCO layer of the precursor stack. In some embodiments, the capping layer is SiAlO. In some embodiments, the capping layer is deposited by sputtering. In one embodiment, the thickness of the capping layer is between about 30 nm and about 100 nm. Subsequent processing of the cap layer in place forms the IC layer without contamination from the environment, ie, with the additional protection of the cap layer. Conversion to a functional electrochromic device can, if desired, occur outside the integrated system because the internal stack is protected from the external environment and conditions of somewhat less stringent purity are used to convert the precursors Necessary for the final conditioning step to convert the stack into a functional device. Such stacked electrochromic device precursors may have advantages, for example, due to a longer lifetime of switching to the electrochromic device only when needed, by having, for example, storability and where the switching parameters depend on the final product Flexibility resulting from a single precursor stack for use in conversion that requires and must meet quality standards that can be modified or fed to different conversion chambers and/or points of consumption for conversion. Again, such precursor stacks can be used for testing purposes, eg, quality control or research efforts. Therefore, one embodiment of the present invention is an electrochromic device precursor, which includes: (a) a substrate; (b) a first transparent conductive oxide layer on the substrate; (c) the first transparent conductive oxide A stack on a layer, the stack comprising: (i) an electrochromic layer comprising an electrochromic material, and (ii) a counter electrode layer comprising a counter electrode material; wherein the stack does not comprise an electrochromic layer between the electrochromic layer an ionically conductive and electrically insulating region from the counter electrode layer; and (d) a second transparent conductive oxide layer on top of the stack. In one embodiment, the electrochromic layer includes tungsten oxide, and the counter electrode layer includes nickel-tungsten oxide. In one embodiment, at least one of the stack and the electrochromic layer contains lithium. In another embodiment, the electrochromic layer is tungsten oxide having a superstoichiometric oxygen content at least at the interface with the counter electrode layer. In another embodiment, the stack includes an IC precursor layer between the counter electrode layer and the electrochromic layer, the IC precursor layer comprising Oxygen Tungsten Oxide. In one embodiment, in the absence of an IC precursor layer between the EC layer and the CE layer, the thickness of the electrochromic layer is between about 500 nm and about 600 nm, and the thickness of the counter electrode layer is Between about 150 nm and about 300 nm. In another embodiment, where there is an IC precursor layer between the EC layer and the CE layer, the thickness of the electrochromic layer is between about 350 nm and about 400 nm, the thickness of the IC precursor layer is between between about 20 nm and about 100 nm, and the thickness of the opposite electrode layer is between about 150 nm and about 300 nm. In one embodiment, the precursor devices described herein are exposed to heat to convert the devices into functional electrochromic devices. In one embodiment, heating is part of the MTCC. Another embodiment is an electrochromic device comprising: (a) an electrochromic layer comprising an electrochromic material; and (b) a counter electrode layer comprising a counter electrode material, wherein the device does not contain A compositionally homogeneous layer of electrically insulating ion-conducting material between the electrochromic layer and the counter electrode. In one embodiment, the electrochromic material is tungsten oxide, the counter electrode material is nickel tungsten oxide, and the layer between the electrochromic layer and the counter electrode layer includes lithium tungstate and tungsten oxide. and an interface region of a mixture of at least one of nickel and tungsten oxide. In another embodiment, the thickness of the electrochromic layer is between about 300 nm and about 500 nm; the thickness of the interface region is between about 10 nm and about 150 nm, and the thickness of the counter electrode layer is between Between about 150 nm and about 300 nm. EXAMPLES FIG. 6 is a graph of a process flow used as a scheme for fabricating electrochromic devices of the present invention. The y -axis units are optical density and the x -axis units are time/program flow. In this example, an electrochromic device similar to that described with respect to FIG. 4A was fabricated in which the substrate was glass with fluorinated tin oxide as the first TCO and the EC layer was a glass with excess oxygen in the matrix. WO3 ( e.g., sputtered using a tungsten target, where the sputtering gas is about 60% O2 and about 40% Ar), the CE layer is formed on top of the EC layer and is made of NiWO, and the second TCO is Indium tin oxide (ITO). Lithium was used as ion source for the electrochromic transition. Optical density is used to determine endpoints during fabrication of electrochromic devices. Optical density was measured as the EC layer (WO3 ) was deposited on the substrate (glass+TCO) starting from the origin of the graph. The optical density of the glass substrate had a baseline optical density of about 0.07 (absorbance units). As the EC layer builds, the optical density increases from this point because tungsten oxide (although substantially transparent) absorbs some visible light. For a desired thickness of a tungsten oxide layer of about 550 nm thick, the optical density rises to about 0.2 as described above. After depositing the tungsten oxide EC layer, lithium was sputtered on the EC layer, as indicated by the first time period indicated by "Li". During this period, the optical density increases further along the curve to 0.4, which indicates that the blind charge of tungsten oxide has been satisfied due to the coloring of tungsten oxide with lithium addition. The time period indicated by "NiWO" indicates the deposition of the NiWO layer during which the optical density increases because the NiWO is colored. Due to the addition of an approximately 230 nm thick NiWO layer, the optical density further increased from approximately 0.4 to approximately 0.9 during NiWO deposition. Note that some lithium can diffuse from the EC layer to the CE layer as NiWO is deposited. This serves to maintain the optical density at a relatively low value during NiWO deposition, or at least during the initial stages of deposition. The second time period indicated by "Li" indicates the addition of lithium to the NiWO EC layer. The optical density decreased from about 0.9 to about 0.4 during this stage due to the discoloration of NiWO by lithiation of NiWO. Lithiation was performed until the NiWO faded (including a local minimum of optical density at about 0.4). The optical density starts to pick up around 0.4 because the WO 3 layer is still lithiated and affects the optical density. Next, additional lithium was sputtered onto the NiWO layer as indicated by the time period "Extra Li", in this example about 10% of the additional lithium compared to the lithium added to NiWO discolored the NiWO layer. During this phase, the optical density increases slightly. Next, indium tin oxide TCO is added, as indicated by "ITO" in the graph. Again, the optical density continued to rise slightly to about 0.6 during the formation of the ITO layer. Next, as indicated by the time period indicated by "MSTCC", the device was heated to about 250°C under Ar for about 15 minutes, and then heated under O2 for about 5 minutes. Next, the device was annealed at about 300° C. for about 30 minutes in air. During this time, the optical density decreased to about 0.4. Thus, optical density is useful in fabricating devices of the present invention (e.g., for determining layer thickness based on deposited material and morphology, and especially for titrating lithium onto various layers for satisfying blind charges and/or achieving fading status) useful tool. Consistent with the approach described with respect to Figure 6, Figure 7 shows a cross-sectional TEM of an electrochromic device 700 fabricated using the method of the present invention. Device 700 has a glass substrate 702 on which an electrochromic stack 714 is formed. Substrate 702 has an ITO layer 704 acting as a first TCO. Tungsten oxide EC layer 706 is deposited on TCO 704 . Layer 706 was formed at a thickness of approximately 550 nm (ie, WO3 formed by sputtering tungsten with oxygen and argon), as described above with respect to FIG. 6 . Lithium is added to the EC layer. Next, an approximately 230 nm thick NiWO CE layer 710 is added, followed by lithium for decolorization and then an approximately 10% excess lithium. Finally, an indium tin oxide layer 712 is deposited, and the stack is subjected to multi-step thermochemical conditioning, as described above with respect to Figure 4A. After MSTCC, this TEM was performed. As can be seen, a new region 708 of ion conducting and electrically insulating is formed. Figure 7 also shows five selected area electron diffraction (SAED) patterns for various layers. First, 704a indicates that the ITO layer is highly crystalline. Pattern 706a shows that the EC layer is polycrystalline. Pattern 708a shows that the IC layer is substantially amorphous. Pattern 710a shows that the CE layer is polycrystalline. Finally, pattern 712a shows that the indium tin oxide TCO layer is highly crystalline. Figure 8 is a cross-section of a device 800 of the present invention analyzed by scanning transmission electron microscopy (STEM). In this example, consistent with the scheme described with respect to Figure 4B, device 800 was fabricated using the methods of the present invention. Device 800 is an electrochromic stack formed on a glass substrate (not labeled). On the glass substrate is a layer of fluorinated tin oxide 804 that acts as the first TCO (for transparent electronic conductors, this layer is sometimes referred to as the "TEC" layer). Tungsten oxide EC layer 806 is deposited on TCO 804 . In this example, layer 806 is formed at a thickness of about 400 nm (i.e., WO3 formed by sputtering tungsten with oxygen and argon, as described above with respect to FIG. About 150 nm thick. Lithium is added to layer 805 . Next, an approximately 230 nm thick NiWO CE layer 810 is added, followed by lithium for decolorization and then an approximately 10% excess lithium. Finally, an indium tin oxide layer 812 is deposited and the stack is subjected to multi-step thermochemical conditioning, as described above with respect to Figure 4B. After MSTCC, do this STEM. As can be seen, a new region 808 of ion conducting and electrically insulating is formed. The difference between this example and the embodiment described with respect to FIG. 4B is that, unlike the similar layer 405 in FIG. 4B , the oxygen-rich layer 805 is only partially converted into an interfacial region 808 . In this case, only about 40 nm of the 150 nm of the oxygen-rich precursor layer 405 is converted into a region that acts as an ion-conducting layer. Figures 8B and 8C show a "before and after" comparison of the device 800 of the present invention (Figure 8C) with the device precursor prior to multi-step thermochemical conditioning (Figure 8B) as analyzed by STEM. In this example, only layers 804-810 (EC to CE) are depicted. The layers are numbered the same as in Figure 8A, with some exceptions. The dotted line in FIG. 8B is used to roughly distinguish the interface between the EC layer 806 and the oxygen-enriched layer 805 (which is more clearly shown in FIG. 8C ). Referring again to Figure 8B, it appears that there is at least lithium concentrated at the interface of the oxygen-rich layer 805 and the CE layer 810 (approximately 10-15 nm thick region), as indicated by 808a. After MTCC (FIG. 8C), it is evident that an interfacial region 808 has formed. While the foregoing invention has been described in some detail to facilitate understanding, the described embodiments should be considered illustrative rather than restrictive. It will be apparent to those of ordinary skill in the art that certain changes and modifications may be practiced within the scope of the appended claims.

100:電致變色裝置 102:基板 104:導電層(CL) 106:電致變色(EC)層 108:離子傳導(IC)層 110:對向電極(CE)層 112:導電層(CL) 114:電致變色堆疊 116:電壓源 300:程序流程 320:程序流程 400:分層結構 401:功能性電致變色裝置 402:基板 403:分層結構 404:第一TCO層 405:第二WO 3層 406:EC層 406a:EC層 407:分層堆疊 408:IC層/界面區 408a:離子傳導電絕緣區/界面區 408b:分級界面區 409:分層結構 410:CE層 411:分層堆疊/功能性電致變色裝置 412:第二TCO層 414a:堆疊 414b:堆疊 414c:堆疊 500:整合式沈積系統 502:入口真空預抽室 504:出口真空預抽室 506:沈積模組 510:入口埠 515:軌道 520:集裝架 525:基板 530:鋰標靶 535:LCD及鍵盤 700:電致變色裝置 702:玻璃基板 704:氧化銦錫(ITO)層 704a:圖案 706:氧化鎢EC層 706a:圖案 708:新區 708a:圖案 710:CE層 710a:圖案 712:氧化銦錫層 712a:圖案 714:電致變色堆疊 800:裝置 804:經氟化之氧化錫層 805:富氧前驅物層 806:氧化鎢EC層 808:新區/界面區 808a:鋰 810:CE層 812:氧化銦錫層 100: Electrochromic device 102: Substrate 104: Conductive layer (CL) 106: Electrochromic (EC) layer 108: Ion conduction (IC) layer 110: Counter electrode (CE) layer 112: Conductive layer (CL) 114 : Electrochromic stack 116: Voltage source 300: Program flow 320: Program flow 400: Layered structure 401: Functional electrochromic device 402: Substrate 403: Layered structure 404: First TCO layer 405: Second WO 3 Layer 406: EC layer 406a: EC layer 407: layered stack 408: IC layer/interface region 408a: ion conducting electrically insulating region/interface region 408b: graded interface region 409: layered structure 410: CE layer 411: layered stack /Functional electrochromic device 412: second TCO layer 414a: stack 414b: stack 414c: stack 500: integrated deposition system 502: entrance vacuum pre-pumping chamber 504: exit vacuum pre-pumping chamber 506: deposition module 510: entrance Port 515: Track 520: Pallet 525: Substrate 530: Lithium Target 535: LCD and Keypad 700: Electrochromic Device 702: Glass Substrate 704: Indium Tin Oxide (ITO) Layer 704a: Pattern 706: Tungsten Oxide EC Layer 706a: pattern 708: new area 708a: pattern 710: CE layer 710a: pattern 712: indium tin oxide layer 712a: pattern 714: electrochromic stack 800: device 804: fluorinated tin oxide layer 805: oxygen-enriched precursor layer 806: Tungsten Oxide EC Layer 808: New Area/Interface Area 808a: Lithium 810: CE Layer 812: Indium Tin Oxide Layer

圖1A為描繪電致變色裝置堆疊之習知形成之示意性橫截面。 圖1B為展示習知電致變色堆疊中之EC層、IC層及CE層之組成之曲線圖。 圖2A至圖2C為展示用於本發明之電致變色裝置之代表性組份組合物之曲線圖。 圖3A及圖3B為根據本發明之實施例之程序流程。 圖4A至圖4C為描繪根據本發明之特定實施例之電致變色裝置之形成的示意性橫截面。 圖5以透視圖描繪本發明之整合式沈積系統。 圖6為展示程序參數與終點示值讀數在根據本發明之實施例之電致變色堆疊之形成期間如何相關的曲線圖。 圖7及圖8A至圖8C為使用根據本發明之實施例之方法製造之電致變色裝置的實際橫截面。 Figure 1A is a schematic cross section depicting the conventional formation of an electrochromic device stack. FIG. 1B is a graph showing the composition of the EC layer, the IC layer and the CE layer in a conventional electrochromic stack. 2A-2C are graphs showing representative component compositions for electrochromic devices of the present invention. 3A and 3B are process flows according to an embodiment of the present invention. 4A-4C are schematic cross-sections depicting the formation of an electrochromic device according to certain embodiments of the invention. Figure 5 depicts the integrated deposition system of the present invention in perspective view. 6 is a graph showing how program parameters and endpoint indication readings relate during formation of an electrochromic stack according to an embodiment of the invention. 7 and 8A-8C are actual cross-sections of electrochromic devices fabricated using methods according to embodiments of the present invention.

320:程序流程 320: Program flow

Claims (24)

一種形成電致變色裝置之方法,該方法包含: (a)     沈積電致變色層於基板上; (b)     沈積金屬於該電致變色層上;及 (c)     氧化該金屬之至少一部分以形成離子傳導且電絕緣材料。 A method of forming an electrochromic device, the method comprising: (a) Depositing an electrochromic layer on a substrate; (b) deposit metal on the electrochromic layer; and (c) Oxidizing at least a portion of the metal to form an ionically conductive and electrically insulating material. 如請求項1之方法,其中該金屬為鋰。The method according to claim 1, wherein the metal is lithium. 如請求項2之方法,其中該離子傳導且電絕緣材料包含至少一種材料選自由以下組成之群:鎢酸鋰(Li 2WO 4)、鉬酸鋰(Li 2MoO 4)、鈮酸鋰(LiNbO 3)、鉭酸鋰(LiTaO 3)、鈦酸鋰(Li 2TiO 3)、鋯酸鋰(Li 2ZrO 3)及其組合。 The method of claim 2, wherein the ionically conductive and electrically insulating material comprises at least one material selected from the group consisting of lithium tungstate (Li 2 WO 4 ), lithium molybdate (Li 2 MoO 4 ), lithium niobate ( LiNbO 3 ), lithium tantalate (LiTaO 3 ), lithium titanate (Li 2 TiO 3 ), lithium zirconate (Li 2 ZrO 3 ), and combinations thereof. 如請求項3之方法,其中該電致變色層包含氧化鎢及該離子傳導且電絕緣材料包含鎢酸鋰。The method of claim 3, wherein the electrochromic layer comprises tungsten oxide and the ion-conducting and electrically insulating material comprises lithium tungstate. 如請求項3之方法,其中該電致變色層包含氧化鉬及該離子傳導且電絕緣材料包含鉬酸鋰。The method of claim 3, wherein the electrochromic layer comprises molybdenum oxide and the ionically conductive and electrically insulating material comprises lithium molybdate. 如請求項3之方法,其中該電致變色層包含氧化鈮及該離子傳導且電絕緣材料包含鈮酸鋰。The method of claim 3, wherein the electrochromic layer comprises niobium oxide and the ionically conductive and electrically insulating material comprises lithium niobate. 如請求項3之方法,其中該電致變色層包含氧化鉭及該離子傳導且電絕緣材料包含鉭酸鋰。The method of claim 3, wherein the electrochromic layer comprises tantalum oxide and the ionically conductive and electrically insulating material comprises lithium tantalate. 如請求項3之方法,其中該電致變色層包含氧化鈦及該離子傳導且電絕緣材料包含鈦酸鋰。The method of claim 3, wherein the electrochromic layer comprises titanium oxide and the ionically conductive and electrically insulating material comprises lithium titanate. 如請求項3之方法,其中該電致變色層包含氧化鋯及該離子傳導且電絕緣材料包含鋯酸鋰。The method of claim 3, wherein the electrochromic layer comprises zirconia and the ionically conductive and electrically insulating material comprises lithium zirconate. 如請求項1之方法,其中氧化該金屬之至少一部分以形成該離子傳導且電絕緣材料包含暴露該基板及/或該金屬至氧。The method of claim 1, wherein oxidizing at least a portion of the metal to form the ionically conductive and electrically insulating material comprises exposing the substrate and/or the metal to oxygen. 如請求項10的方法,其中該氧係提供以作為該電致變色層之部分。The method of claim 10, wherein the oxygen is provided as part of the electrochromic layer. 如請求項10的方法,其進一步包含沈積對向電極層,其中該氧係提供以作為該對向電極層之部分。The method of claim 10, further comprising depositing a counter electrode layer, wherein the oxygen is provided as part of the counter electrode layer. 如請求項10的方法,其中該氧係提供以作為該基板上的超化學劑量氧材料。The method of claim 10, wherein the oxygen system is provided as a superstoichiometric oxygen material on the substrate. 如請求項10之方法,其中該氧係提供在該基板被暴露至的氣氛中。The method of claim 10, wherein the oxygen is provided in an atmosphere to which the substrate is exposed. 如請求項1之方法,其中氧化該金屬之至少一部分以形成該離子傳導且電絕緣材料包含加熱該基板。The method of claim 1, wherein oxidizing at least a portion of the metal to form the ionically conductive and electrically insulating material comprises heating the substrate. 如請求項15之方法,其中加熱該基板引起該金屬與該電致變色層之材料之間的反應以形成該離子傳導且電絕緣材料。The method of claim 15, wherein heating the substrate causes a reaction between the metal and the material of the electrochromic layer to form the ionically conductive and electrically insulating material. 如請求項15之方法,其進一步包含沈積對向電極層,其中加熱該基板引起該金屬與該對向電極層之材料之間的反應以形成該離子傳導且電絕緣材料。The method of claim 15, further comprising depositing a counter electrode layer, wherein heating the substrate causes a reaction between the metal and a material of the counter electrode layer to form the ionically conductive and electrically insulating material. 如請求項1之方法,其進一步包含沈積對向電極層,其中氧化該金屬之至少一部分以形成該離子傳導且電絕緣材料在沈積該對向電極層前發生。The method of claim 1, further comprising depositing a counter electrode layer, wherein oxidizing at least a portion of the metal to form the ionically conductive and electrically insulating material occurs before depositing the counter electrode layer. 如請求項1之方法,其進一步包含沈積對向電極層,其中氧化該金屬之至少一部分以形成該離子傳導且電絕緣材料在沈積該對向電極層時發生。The method of claim 1, further comprising depositing a counter electrode layer, wherein oxidizing at least a portion of the metal to form the ionically conductive and electrically insulating material occurs when depositing the counter electrode layer. 如請求項1之方法,其進一步包含沈積對向電極層,其中氧化該金屬之至少一部分以形成該離子傳導且電絕緣材料在沈積該對向電極層後發生。The method of claim 1, further comprising depositing a counter electrode layer, wherein oxidizing at least a portion of the metal to form the ion conducting and electrically insulating material occurs after depositing the counter electrode layer. 如請求項1之方法,其進一步包含沈積對向電極層,及沈積額外之金屬在該對向電極層上。The method of claim 1, further comprising depositing a counter electrode layer, and depositing additional metal on the counter electrode layer. 如請求項21之方法,其中該額外之金屬係足以完全使該對向電極層褪色。The method of claim 21, wherein the additional metal is sufficient to completely discolor the counter electrode layer. 如請求項1之方法,其中(a)及(b)係在真空下執行,及其中在(a)與(b)之間並未破真空。The method of claim 1, wherein (a) and (b) are performed under vacuum, and wherein the vacuum is not broken between (a) and (b). 如請求項1之方法,其中該金屬係選自由鋰、鈉、鉀、鈣、鋇、鍶、鎂及其組合所組成之群。The method according to claim 1, wherein the metal is selected from the group consisting of lithium, sodium, potassium, calcium, barium, strontium, magnesium and combinations thereof.
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