JPH0442835B2 - - Google Patents
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- Publication number
- JPH0442835B2 JPH0442835B2 JP59197348A JP19734884A JPH0442835B2 JP H0442835 B2 JPH0442835 B2 JP H0442835B2 JP 59197348 A JP59197348 A JP 59197348A JP 19734884 A JP19734884 A JP 19734884A JP H0442835 B2 JPH0442835 B2 JP H0442835B2
- Authority
- JP
- Japan
- Prior art keywords
- bsf
- optical sensor
- manufacturing
- wafer
- infrared irradiation
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
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Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F71/00—Manufacture or treatment of devices covered by this subclass
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F10/00—Individual photovoltaic cells, e.g. solar cells
- H10F10/10—Individual photovoltaic cells, e.g. solar cells having potential barriers
- H10F10/14—Photovoltaic cells having only PN homojunction potential barriers
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
- Y02E10/547—Monocrystalline silicon PV cells
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- Photovoltaic Devices (AREA)
- Light Receiving Elements (AREA)
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は受光素子、太陽電池等として広く用い
られている光センサの製造方法、さらに詳しくい
えば赤外線照射により浅い接合とBSFを同時に
形成する光センサの製造方法に関する。[Detailed Description of the Invention] (Industrial Application Field) The present invention relates to a method for manufacturing an optical sensor widely used as a light receiving element, a solar cell, etc., and more specifically, a method for simultaneously forming a shallow junction and a BSF by infrared irradiation. The present invention relates to a method of manufacturing an optical sensor.
ここでBSFとは裏面に小数キヤリヤを押し戻
す電位勾配を形成して裏面での小数キヤリヤの再
結合を防ぐことができる効果をいう。 Here, BSF refers to an effect that can prevent recombination of fractional carriers on the backside by forming a potential gradient that pushes back the fractional carriers on the backside.
(従来の技術)
Si太陽電池の反射防止膜と受光面の浅い接合形
成をTiO2とP2O5の混合物をスピンオン法で、Si
のエツチ面に塗布して電気炉の中で900℃〜930℃
で15分程度加熱して、不純物Pを拡散によつて行
う。(Prior technology) A shallow junction between the anti-reflection film and the light-receiving surface of a Si solar cell is formed using a spin-on method using a mixture of TiO 2 and P 2 O 5 .
Apply to the etched surface and heat in an electric furnace at 900℃ to 930℃.
The impurity P is diffused by heating for about 15 minutes.
次にウエーハの裏面にスクリーン印刷で塗布し
たAl膜を電気炉で800℃〜825℃で2分程度加熱
してp+層を形成することにより、BSF効果を持
たせる。 Next, the Al film applied to the back side of the wafer by screen printing is heated in an electric furnace at 800°C to 825°C for about 2 minutes to form a p + layer, thereby imparting a BSF effect.
最後に受光面の電極は、銀ペーストをA・R膜
(TiO2膜)の上にスクリーン印刷して、600℃〜
610℃で加熱してつくり、最大効率16%の太陽電
池を得ている。Finally, the electrodes on the light-receiving surface are made by screen printing silver paste on the A/R film (TiO 2 film) and heating it at 600℃~
It is made by heating at 610 degrees Celsius, resulting in a solar cell with a maximum efficiency of 16%.
この方法には以下の問題がある。 This method has the following problems.
900℃〜930℃で15分と、受光層の浅い接合を
形成する時間が長い。 It takes 15 minutes at 900°C to 930°C, which is a long time to form a shallow junction in the light-receiving layer.
BSF効果を発生させるために800〜825℃で
2分間熱処理をする必要がある。と温度およ
び時間が異なり、同一のプロセスになりえな
い。 Heat treatment at 800-825°C for 2 minutes is required to generate the BSF effect. The temperature and time are different and the process cannot be the same.
高温処理(900℃〜930℃)時間が15分と長
く、基板の寿命が減少し、逆方向電流の増加、
開放電圧の減少、長波長応答の減少が予測され
る。 High temperature processing (900℃~930℃) time is as long as 15 minutes, which reduces the life of the board, increases reverse current,
It is expected that the open circuit voltage will decrease and the long wavelength response will decrease.
受光層の浅い接合を形成する時間を短くして前
記問題を解決するために本件発明者の一人は1984
年6月28日付けで「トランジエント光照射技術を
用いた低コストSi太陽電池」(論文番号SSD84−
27)と題して社団法人電子通信学会において発表
を行つている。 In order to solve the above problem by shortening the time to form a shallow junction in the light-receiving layer, one of the inventors of the present invention made a research in 1984.
“Low-cost Si solar cells using transient light irradiation technology” (paper number SSD84-
27) at the Institute of Electronics and Communication Engineers.
前記論文記載の方法によれば、極めて短時間の
熱処理により浅い接合層を形成することができ
る。熱平衡状態だけでは説明できない増速された
拡散が発生していると推定される。これは半導体
ウエーハと不純物を含んだ絶縁膜間に熱膨張係数
の差による歪が発生することによると考えられ
る。短時間の熱処理による拡散により基板の拡散
長の劣化を防止することができるので、短時間で
良質の接合を形成することができ、従来の太陽電
池等の製造プロセスを大幅に改善できる。 According to the method described in the paper, a shallow bonding layer can be formed by extremely short heat treatment. It is presumed that accelerated diffusion is occurring that cannot be explained solely by the thermal equilibrium state. This is thought to be due to distortion occurring due to the difference in thermal expansion coefficient between the semiconductor wafer and the impurity-containing insulating film. Since deterioration of the diffusion length of the substrate can be prevented by diffusion caused by short-time heat treatment, a high-quality bond can be formed in a short time, and the conventional manufacturing process for solar cells and the like can be significantly improved.
本件発明者等は前記熱処理をさらに検討した結
果、前記異常拡散についてのより多くのデータを
得るとともに、半導体ウエーハの裏面にBSF効
果を与える半導体のハイ・ロー結合層を同時に形
成できることを突き止めた。 As a result of further investigation of the heat treatment, the present inventors obtained more data on the anomalous diffusion and found that it is possible to simultaneously form a semiconductor high-low bonding layer that provides a BSF effect on the back surface of a semiconductor wafer.
(発明の目的)
本発明の目的は赤外線照射による極短時間の熱
処理により浅い接合とBSF効果を与える半導体
のハイ・ロー結合層を同時に形成できる光センサ
の製造方法を提供することにある。(Objective of the Invention) The object of the present invention is to provide a method for manufacturing an optical sensor that can simultaneously form shallow junctions and semiconductor high and low bonding layers that provide a BSF effect by extremely short heat treatment using infrared irradiation.
(発明の構成)
前記目的を達成するために本発明による赤外線
照射により浅い接合とBSFを同時に形成する光
センサの製造方法は、
拡散により表面に接合を形成する光センサの製
造方法において、
半導体ウエーハの裏面にハイ・ロー接合用の金
属膜を形成し、
半導体ウエーハの表面に前記半導体とは異なる熱
膨張係数を持ち拡散しようとする不純物を含んだ
絶縁膜を形成し、
前記半導体ウエーハを赤外線源を持つ炉中に配
置し、前記半導体ウエーハと不純物を含んだ絶縁
膜間に熱膨張係数の差による歪が発生する急激な
温度勾配で昇温し極短時間加熱して受光面に浅い
接合と裏面にBSF効果を呈するハイ・ロー接合
を同時に形成するよう構成されている。(Structure of the Invention) In order to achieve the above object, a method of manufacturing an optical sensor in which a shallow junction and a BSF are simultaneously formed by infrared irradiation according to the present invention includes: A method of manufacturing an optical sensor in which a junction is formed on a surface of a semiconductor wafer by diffusion. A metal film for high/low junction is formed on the back surface of the semiconductor wafer, an insulating film containing impurities that have a coefficient of thermal expansion different from that of the semiconductor and which tends to diffuse is formed on the surface of the semiconductor wafer, and the semiconductor wafer is exposed to an infrared ray source. The semiconductor wafer and the impurity-containing insulating film are placed in a furnace with a steep temperature gradient that causes distortion due to the difference in thermal expansion coefficient between the semiconductor wafer and the impurity-containing insulating film, and are heated for a very short time to form a shallow junction on the light receiving surface. It is configured to simultaneously form high and low junctions exhibiting a BSF effect on the back surface.
(実施例)
以下、図面等を参照して本発明をさらに詳しく
説明する。(Example) Hereinafter, the present invention will be described in more detail with reference to the drawings and the like.
第1図は本発明による赤外線照射による光セン
サの方法の第1の実施例の製造工程を示す工程図
である。 FIG. 1 is a process diagram showing the manufacturing process of a first embodiment of the method for producing an optical sensor using infrared irradiation according to the present invention.
この工程図な、面方位(100)比抵抗10Ωcmの
CZシリコンp形ウエーハについて示されている。 This process diagram shows the surface orientation (100) and resistivity of 10Ωcm.
Shown for a CZ silicon p-type wafer.
シリコンウエーハ準備工程10で前記ウエーハ
を準備する。なおウエーハの熱膨張係数は2.5×
10-6/℃である。 In a silicon wafer preparation step 10, the wafer is prepared. The thermal expansion coefficient of the wafer is 2.5×
10 -6 /℃.
裏面の処理工程11で前記ウエーハの裏面に真
空蒸着によりアルミニユウム(Al)を蒸着する。
不純物を含む絶縁膜形成工程12により前記ウエ
ーハの表面に拡散しようとする不純物を含む絶縁
膜を形成する。 In a backside treatment step 11, aluminum (Al) is deposited on the backside of the wafer by vacuum deposition.
In step 12 of forming an insulating film containing impurities, an insulating film containing impurities that are likely to diffuse into the surface of the wafer is formed.
良く知られているスピンオン法によりPをドー
プした2000〜3000ÅのSiO2膜を形成した。 A P-doped SiO 2 film with a thickness of 2000 to 3000 Å was formed by the well-known spin-on method.
なお前記不純物を含む絶縁膜の熱膨張係数は
0.5×10-6/℃である。 The coefficient of thermal expansion of the insulating film containing the impurities is
It is 0.5×10 -6 /℃.
照射加温工程13において、前記アルミ蒸着面
と不純物を含む絶縁膜が形成されたウエーハをハ
ロゲンランプの炉中に配置して、不活性ガス
(N2)中でトランジエント加熱を行つた。 In the irradiation heating step 13, the wafer on which the aluminum vapor-deposited surface and the impurity-containing insulating film were formed was placed in a halogen lamp furnace, and transient heating was performed in an inert gas (N 2 ).
第2図は、トランジエント加熱の一例を示す温
度プログラム図である。 FIG. 2 is a temperature program diagram showing an example of transient heating.
温度のモニタは、クロメル−アルメル熱電対を
前記ウエーハに接触させておこなつた。 Temperature was monitored using a chromel-alumel thermocouple in contact with the wafer.
ハロゲンランプを点炉する前にウエーハ温度を
100℃に保つておく。 Check the wafer temperature before lighting the halogen lamp.
Keep it at 100℃.
第2図には炉内温度を900℃まで、昇温スピー
ドは50℃/secで上昇させる例を示している。こ
のようにして熱処理されたウエーハはよく知られ
ている電極作成工程15を経て、素子切出し工程
16で1×1cm2のチツプに加工される。 Figure 2 shows an example in which the temperature inside the furnace is increased to 900°C at a rate of 50°C/sec. The wafer heat-treated in this manner is processed into chips of 1×1 cm 2 in a well-known electrode forming step 15 and an element cutting step 16.
ハロゲンランプを点灯してから設定温度(第2
図では900℃)に達してから短時間、設定温度を
保つ、この明細書では、設定温度の98%に達した
時点からハロゲンランプを消燈するまでの時間を
拡散時間と仮に定義して用いる。 After turning on the halogen lamp, set the temperature (second
The set temperature is maintained for a short time after reaching 900℃ (in the figure). In this specification, the time from when the set temperature reaches 98% until the halogen lamp is turned off is tentatively defined as the diffusion time. .
設定時間、800、850、900、950℃において、拡
散時間を1〜20秒の範囲で適当に選び種々の試料
を得た。 Various samples were obtained by appropriately selecting diffusion times in the range of 1 to 20 seconds at set times of 800, 850, 900, and 950°C.
ホール測定4、これらの試料につき陽極酸化と
ホール測定を繰り返して行うことにより、拡散さ
れたキヤリヤ濃度の深さ方向の分布を測定した。 Hall measurement 4: By repeating anodic oxidation and Hall measurement on these samples, the distribution of the diffused carrier concentration in the depth direction was measured.
第3図に前記測定で得られたキヤリヤ濃度およ
び移動度のグラフを示す。 FIG. 3 shows a graph of the carrier concentration and mobility obtained in the above measurements.
設定温度900℃、950℃のときは、いずれも、最
初の1秒間で異常に大きな拡散が生じ、1秒から
5秒の間よりも大きな拡散が観測される。 When the set temperature is 900°C and 950°C, an abnormally large amount of diffusion occurs in the first second, and a larger amount of diffusion is observed between 1 and 5 seconds.
このことは前記論文において詳述されている。 This is detailed in the above article.
本件発明者等は設定温度900℃において、前記
50℃/sec以外の他の昇温率10℃/sec、20℃/
sec、30℃/sec、を選定して、拡散時間を5秒と
して熱処理を行つた。 At a set temperature of 900°C, the inventors of the present invention
Other temperature increase rates other than 50℃/sec: 10℃/sec, 20℃/sec
sec, 30° C./sec was selected, and the heat treatment was performed with a diffusion time of 5 seconds.
キヤリア濃度の測定結果を第4図に示す。 Figure 4 shows the measurement results of carrier concentration.
この測定結果からも、昇温率が大きかつたもの
のほうがより大きな拡散深さを得ることができる
ことが理解できる。 It can be understood from this measurement result that a larger diffusion depth can be obtained with a larger temperature increase rate.
次に本発明方法によりBSF効果層を形成した
太陽電池(n+/pp+形)と、同じ熱処理を施した
がBSF効果層を形成しなかつた太陽電池(n+/
p形)のそれぞれの特性を比較する。 Next, a solar cell (n + /pp + type) in which a BSF effect layer was formed by the method of the present invention, and a solar cell (n + /pp + type) which was subjected to the same heat treatment but without forming a BSF effect layer.
Compare the characteristics of each type (p type).
BSF効果層を形成するためにρ=10Ωcm、厚さ
500μmのp形Siウエーハの裏面に3000ÅのAlを
蒸着して、表面に前記方法で不純物を含む絶縁層
を形成する。 ρ=10Ωcm, thickness to form BSF effect layer
3000 Å of Al is deposited on the back surface of a 500 μm p-type Si wafer, and an insulating layer containing impurities is formed on the surface using the above method.
他の試料は同一のウエーハの表面に不純物を含
む絶縁層を形成する。 Other samples form an insulating layer containing impurities on the surface of the same wafer.
両ウエーハを設定温度900℃、拡散時間10秒、
昇温率50℃/secで熱処理をおこなつた。 Both wafers were set at a temperature of 900°C and a diffusion time of 10 seconds.
Heat treatment was performed at a temperature increase rate of 50°C/sec.
第5図に前記各太陽電池の分光特性を比較して
示してある。 FIG. 5 shows a comparison of the spectral characteristics of each of the solar cells.
BSF効果層を形成した太陽電池は、BSF効果
層を持たない太陽電池に比較して長波長側が高感
度化されている。 Solar cells with a BSF effect layer have higher sensitivity on the long wavelength side than solar cells without a BSF effect layer.
第6図に前記各太陽電池のI−V特性を比較し
て示してある。 FIG. 6 shows a comparison of the IV characteristics of each of the solar cells.
BSF効果層を形成した太陽電池は、BSF効果
層を持たない太陽電池に比較して効率も9.01%か
ら10.88%となり、約2割の上昇が見られる。以
上のデータは表面に反射防止膜を施していないも
のであるが反射防止膜をつければ30〜40%効率が
上昇することが知られている。 Compared to solar cells without a BSF effect layer, solar cells with a BSF effect layer have an efficiency of 9.01% to 10.88%, an increase of approximately 20%. The above data is based on the case where no anti-reflection film is applied to the surface, but it is known that adding an anti-reflection film can increase efficiency by 30 to 40%.
したがつて反射防止膜を形成することにより効
率を35%上昇できるとすると、本発明方法による
太陽電池に反射防止膜を形成すれば14.7%程度の
効率の太陽電池が得られることになる。 Therefore, assuming that the efficiency can be increased by 35% by forming an antireflection film, if the antireflection film is formed on a solar cell according to the method of the present invention, a solar cell with an efficiency of about 14.7% will be obtained.
前述した第1の実施例と同様な工程−V属化
合物ウエーハによる光センサを製造することもで
きる。 It is also possible to manufacture an optical sensor using a group V compound wafer in the same process as in the first embodiment described above.
ガリウム・砒素・燐(GaAsP)ウエーハによ
る第2の実施例について説明する。 A second embodiment using a gallium-arsenic-phosphorus (GaAsP) wafer will be described.
前記実施例同様にウエーハの準備工程10、裏
面の処理工程11、不純物を含む絶縁膜形成工程
12を経て、照射加温工程13において、前記ア
ルミ蒸着面と不純物を含む絶縁膜が形成されたウ
エーハを800℃で2秒間拡散を行う。 Similar to the above embodiment, the wafer is subjected to a wafer preparation step 10, a backside treatment step 11, an impurity-containing insulating film forming step 12, and then an irradiation heating step 13 on which the aluminum vapor-deposited surface and an impurity-containing insulating film are formed. Perform diffusion at 800℃ for 2 seconds.
続いて工程15,16を経てガリウム・砒素・
燐ウエーハによる光センサを得た。 Next, through steps 15 and 16, gallium, arsenic,
An optical sensor using a phosphor wafer was obtained.
第7図に前記工程で得られた光センサと、同じ
基板に従来の拡散方法(800℃、60分)を用いて
形成したものとを、それぞれの電圧電流特性を比
較して示してある。 FIG. 7 shows a comparison of the voltage-current characteristics of the optical sensor obtained in the above process and one formed on the same substrate using the conventional diffusion method (800° C., 60 minutes).
第8図は第2の実施例による光センサと、前記
従来の拡散方法(800℃、60分)を用いて形成し
たものとを、それぞれの分光感度特性を比較して
示したグラフである。 FIG. 8 is a graph comparing the spectral sensitivity characteristics of the optical sensor according to the second embodiment and one formed using the conventional diffusion method (800° C., 60 minutes).
第2の実施例によるものは優れた電圧電流特性
を示し、短波長側にも充分な感度をもつことが理
解できる。 It can be seen that the second example exhibits excellent voltage-current characteristics and has sufficient sensitivity even on the short wavelength side.
(変形例)
以上詳しく説明した実施例につき本発明の範囲
内で種々の変形を施すことができる。(Modifications) Various modifications can be made to the embodiments described in detail above within the scope of the present invention.
前記各実施例において前記不純物を含む絶縁膜
形成工程12の次に不純物を含まない絶縁膜形成
工程を設けると不純物が気相に散逸することを防
止できる。 In each of the embodiments described above, if an insulating film forming step not containing impurities is provided next to the step 12 of forming an insulating film containing impurities, it is possible to prevent impurities from dissipating into the gas phase.
前記各実施例において照射加温工程13の炉内
の不活性ガスを大気に、また水素に置き換えても
良い。 In each of the above embodiments, the inert gas in the furnace in the irradiation and heating step 13 may be replaced with air or hydrogen.
また第2の実施例としてガリウム・砒素・燐
(GaAsP)のウエーハの例を示したが他の−V
族化合物(GaAs)(GaP)等について同様な工
程を適用することができる。 In addition, although an example of a gallium-arsenic-phosphorus (GaAsP) wafer is shown as a second embodiment, other -V
A similar process can be applied to group compounds (GaAs) (GaP), etc.
(発明の効果)
以上説明したように、本発明による製造方法に
よれば、一回の短時間の熱処理により、表面の薄
い接合と裏面のBSF効果層を同時に形成するこ
とができ、しかも従来の太陽電池よりも高い効率
の太陽電池が得られる。(Effects of the Invention) As explained above, according to the manufacturing method of the present invention, a thin bond on the front surface and a BSF effect layer on the back surface can be simultaneously formed by one short heat treatment, and moreover, it is possible to simultaneously form a thin bond on the front surface and a BSF effect layer on the back surface. Solar cells with higher efficiency than solar cells can be obtained.
また製造工程が簡単でかつ短時間でよいから太
陽電池等の製造工程を大幅に合理化することがで
きる。 Furthermore, since the manufacturing process is simple and takes only a short time, the manufacturing process for solar cells and the like can be significantly streamlined.
第1図は本発明により赤外線照射による光セン
サの製造工程の実施例を示す工程図である。第2
図は炉内温度の制御例を示すグラフである。第3
図は前記測定で得られたキヤリヤ濃度およびホー
ル移動度を示すグラフである。第4図は昇温速度
を変えて、拡散の深さを比較したグラフである。
第5図は本発明による方法で製造した太陽電池の
分光特性を示すグラフ、第6図は本発明による方
法で製造した太陽電池のI−V性を示すグラフで
あつて、それぞれ同一の熱処理を施して製造した
太陽電池でBSF効果層を形成していないものの
特性と比較して示してある。第7図は本発明によ
る方法で、ガリウム・砒素・燐(GaAsP)のウ
エーハを用いて製造した光センサと、同じウエー
ハに従来の拡散方法を適用して製造した光センサ
とを、それぞれの電圧電流特性を比較して示した
グラフである。第8図は本発明による方法で、ガ
リウム・砒素・燐(GaAsP)のウエーハを用い
て製造した光センサと、同じウエーハに従来の拡
散方法を適用して製造した光センサとを、それぞ
れの分光感度特性を比較して示栄したグラフであ
る。
10……シリコンウエーハ準備工程、11……
Al蒸着工程、12……不純物を含む絶縁膜形成
工程、13……照射加温工程、14……ホール測
定、15……電極作成工程、16……素子切出し
工程。
FIG. 1 is a process diagram showing an embodiment of the manufacturing process of an optical sensor using infrared irradiation according to the present invention. Second
The figure is a graph showing an example of controlling the temperature inside the furnace. Third
The figure is a graph showing the carrier concentration and hole mobility obtained in the above measurements. FIG. 4 is a graph comparing the depth of diffusion by changing the heating rate.
FIG. 5 is a graph showing the spectral characteristics of the solar cell manufactured by the method according to the present invention, and FIG. 6 is a graph showing the I-V properties of the solar cell manufactured by the method according to the present invention, both of which were subjected to the same heat treatment. A comparison is shown with the characteristics of a solar cell manufactured by applying the BSF effect layer without forming a BSF effect layer. FIG. 7 shows a method according to the present invention, in which an optical sensor manufactured using a gallium-arsenic-phosphorus (GaAsP) wafer and an optical sensor manufactured by applying a conventional diffusion method to the same wafer are connected at different voltages. It is a graph showing a comparison of current characteristics. FIG. 8 shows a method according to the present invention, in which an optical sensor manufactured using a gallium-arsenic-phosphorus (GaAsP) wafer and an optical sensor manufactured by applying a conventional diffusion method to the same wafer are separated into spectral spectra. This is a graph showing a comparison of sensitivity characteristics. 10...Silicon wafer preparation process, 11...
Al vapor deposition process, 12... Insulating film formation process containing impurities, 13... Irradiation heating process, 14... Hole measurement, 15... Electrode creation process, 16... Element cutting process.
Claims (1)
製造方法において、 半導体ウエーハの裏面にハイ・ロー接合用の金
属膜を形成し、 半導体ウエーハの表面に前記半導体とは異なる
熱膨張係数を持ち拡散しようとする不純物を含ん
だ絶縁膜を形成し、 前記半導体ウエーハを赤外線源を持つ炉中に配
置し、 前記半導体ウエーハと不純物を含んだ絶縁膜間
に熱膨張係数の差による歪が発生する急激な温度
勾配で昇温し極短時間加熱した受光面に浅い接合
と裏面にBSF効果を呈するハイ・ロー接合を同
時に形成するよう構成したことを特徴とする赤外
線照射により浅い接合とBSFを同時に形成する
光センサの製造方法。 2 前記半導体ウエーハはシリコンウエーハであ
る特許請求の範囲第1項記載の赤外線照射により
浅い接合とBSFを同時に形成する光センサの製
造方法。 3 前記シリコンウエーハは面方位(100)比抵
抗10ΩcmのCZシリコンp形ウエーハである特許
請求の範囲第2項記載の赤外線照射により浅い接
合とBSFを同時に形成する光センサの製造方法。 4 前記不純物を含んだ絶縁膜はスピンオン法に
より形成されたPをドープしたSiO2膜である特
許請求の範囲第2項記載の赤外線照射により浅い
接合とBSFを同時に形成する光センサの製造方
法。 5 前記不純物を含んだ絶縁膜の厚さは、2000〜
3000Åである特許請求の範囲第4項記載の赤外線
照射により浅い接合とBSFを同時に形成する光
センサの製造方法。 6 前記ハイ・ロー接合用の金属膜はアルミニユ
ウムである特許請求の範囲第1項記載の赤外線照
射により浅い接合とBSFを同時に形成する光セ
ンサの製造方法。 7 前記半導体ウエーハは−V族化合物である
特許請求の範囲第1項記載の赤外線照射により浅
い接合とBSFを同時に形成する光センサの製造
方法。[Claims] 1. In a method for manufacturing an optical sensor that forms a junction on the surface by diffusion, a metal film for high/low junction is formed on the back surface of a semiconductor wafer, and the surface of the semiconductor wafer is exposed to heat different from that of the semiconductor. forming an insulating film containing an impurity that has an expansion coefficient and is likely to diffuse; placing the semiconductor wafer in a furnace with an infrared source; Shallow bonding by infrared irradiation characterized by a structure that simultaneously forms a shallow bond on the light-receiving surface that is heated with a sharp temperature gradient that causes strain and is heated for an extremely short time, and a high/low bond that exhibits a BSF effect on the back surface. A method for manufacturing an optical sensor that simultaneously forms BSF and BSF. 2. A method of manufacturing an optical sensor in which a shallow junction and a BSF are simultaneously formed by infrared irradiation according to claim 1, wherein the semiconductor wafer is a silicon wafer. 3. The method of manufacturing an optical sensor in which a shallow junction and a BSF are simultaneously formed by infrared irradiation according to claim 2, wherein the silicon wafer is a CZ silicon p-type wafer with a plane orientation (100) and a specific resistance of 10 Ωcm. 4. A method for manufacturing an optical sensor in which a shallow junction and a BSF are simultaneously formed by infrared irradiation according to claim 2, wherein the impurity-containing insulating film is a P-doped SiO 2 film formed by a spin-on method. 5 The thickness of the insulating film containing the impurity is 2000~
A method for manufacturing an optical sensor, in which a shallow junction and a BSF are simultaneously formed by infrared irradiation according to claim 4, which has a thickness of 3000 Å. 6. A method for manufacturing an optical sensor in which a shallow junction and a BSF are simultaneously formed by infrared irradiation according to claim 1, wherein the metal film for the high/low junction is aluminum. 7. A method of manufacturing an optical sensor in which a shallow junction and a BSF are simultaneously formed by infrared irradiation according to claim 1, wherein the semiconductor wafer is a -V group compound.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59197348A JPS6174378A (en) | 1984-09-20 | 1984-09-20 | Method for manufacturing an optical sensor that simultaneously forms shallow junctions and BSF by infrared irradiation |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59197348A JPS6174378A (en) | 1984-09-20 | 1984-09-20 | Method for manufacturing an optical sensor that simultaneously forms shallow junctions and BSF by infrared irradiation |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6174378A JPS6174378A (en) | 1986-04-16 |
| JPH0442835B2 true JPH0442835B2 (en) | 1992-07-14 |
Family
ID=16372984
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59197348A Granted JPS6174378A (en) | 1984-09-20 | 1984-09-20 | Method for manufacturing an optical sensor that simultaneously forms shallow junctions and BSF by infrared irradiation |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6174378A (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62256427A (en) * | 1986-04-28 | 1987-11-09 | Nec Corp | Impurity diffusion |
| US5223453A (en) * | 1991-03-19 | 1993-06-29 | The United States Of America As Represented By The United States Department Of Energy | Controlled metal-semiconductor sintering/alloying by one-directional reverse illumination |
| GB0114896D0 (en) * | 2001-06-19 | 2001-08-08 | Bp Solar Ltd | Process for manufacturing a solar cell |
| JP4957042B2 (en) * | 2006-03-29 | 2012-06-20 | 三菱電機株式会社 | Manufacturing method of solar cell |
| JP2013042042A (en) * | 2011-08-18 | 2013-02-28 | Tohoku Univ | Method of manufacturing silicon solar cell |
-
1984
- 1984-09-20 JP JP59197348A patent/JPS6174378A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6174378A (en) | 1986-04-16 |
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