JPH0240633A - Nonlinear optical material and nonlinear optical element - Google Patents
Nonlinear optical material and nonlinear optical elementInfo
- Publication number
- JPH0240633A JPH0240633A JP19101988A JP19101988A JPH0240633A JP H0240633 A JPH0240633 A JP H0240633A JP 19101988 A JP19101988 A JP 19101988A JP 19101988 A JP19101988 A JP 19101988A JP H0240633 A JPH0240633 A JP H0240633A
- Authority
- JP
- Japan
- Prior art keywords
- nonlinear optical
- group
- electron
- optical element
- denotes
- 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.)
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL 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
- G02F1/00—Devices 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
- G02F1/35—Non-linear optics
- G02F1/355—Non-linear optics characterised by the materials used
- G02F1/361—Organic materials
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- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Organic Low-Molecular-Weight Compounds And Preparation Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、レーザー光の高調波の発生、パラメトリック
増幅等に用いる有機非線形光学材料及び有機非線形光学
素子に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to organic nonlinear optical materials and organic nonlinear optical elements used for generation of harmonics of laser light, parametric amplification, and the like.
[発明の背景]
レーザー光等の強い光を物質に照射した時に顕著に現れ
る非線形光学効果は、波長変換、強度変調、スイッチン
グ等に応用できるものであり、近年、該非線形光学効果
を有する材料の探索研究が数多く為されている。[Background of the Invention] The nonlinear optical effect that appears when a material is irradiated with intense light such as a laser beam can be applied to wavelength conversion, intensity modulation, switching, etc., and in recent years, materials that have this nonlinear optical effect have been developed. Many exploratory studies have been conducted.
波長変換、特に2次の非線形光学効果に基づいた第2高
調波発生(Second HarllOnlCGene
ratlOn、以下SHGと略す、)では、従来知られ
ていたニオブ酸リチウム(LiNbO,)、燐酸二水素
カリウム(KDP)等の無機材料に比し、有機化合物が
桁違いに高い性能を有する可能性が指摘されている。(
例えば、「有機非線形光学材料」、加藤政雄、中西へ部
監修、シー・エム・シー社。Wavelength conversion, especially second harmonic generation based on second-order nonlinear optical effects
ratlOn (hereinafter abbreviated as SHG), organic compounds may have an order of magnitude higher performance than conventionally known inorganic materials such as lithium niobate (LiNbO) and potassium dihydrogen phosphate (KDP). has been pointed out. (
For example, "Organic Nonlinear Optical Materials", supervised by Masao Kato and Hehe Nakanishi, CMC Co., Ltd.
1985年刊)
有機化合物の非線形性の起源は分子内π電子であり、2
次の非線形分子分極率βは、該化合物が電子供与性基お
よび電子吸引性基の両方を有するとき、特に大きくなる
=
しかしながら、ρ−ニトロアニリンで代表されるように
、分子レベルの非線形分極が大きくても、結晶の状態で
は全<SHGを示さなかったり、示してもSHGの小さ
いものが数多くみられる。これは、極性の強い有機物結
晶の分子配列が反転対称になり易いことに起因する。(published in 1985) The origin of nonlinearity in organic compounds is the intramolecular π electrons, and 2
The following nonlinear molecular polarizability β becomes particularly large when the compound has both an electron-donating group and an electron-withdrawing group = However, as represented by ρ-nitroaniline, nonlinear polarization at the molecular level Even if they are large, there are many cases where they do not show total<SHG in the crystalline state, or even if they do show, the SHG is small. This is due to the fact that the molecular arrangement of highly polar organic crystals tends to have inversion symmetry.
また、情報記録媒体の大容量化、高密度化の要求に応え
る形で光記録媒体の研究が盛んに行われているが、これ
ら光記録媒体の記録密度は光源の波長に依存するので(
記録密度限界は光源波長が短くなると、その2乗に反比
例して増大する。)、より短波な光源を得るなめに波長
変換素子への期待は大きいものがある。In addition, research into optical recording media is being actively conducted in response to demands for larger capacity and higher density information recording media, but since the recording density of these optical recording media depends on the wavelength of the light source (
As the light source wavelength becomes shorter, the recording density limit increases in inverse proportion to the square of the wavelength. ), there are great expectations for wavelength conversion elements in order to obtain shorter wavelength light sources.
しかしながら、既知の高SHG活性の化合物は、例えば
2−メチル−4−ニトロアニリン、m−ニトロアニリン
等のように黄色に着色しているため、短波光の透過率が
低く、波長変換で短波光を発生するには不利である。従
って、可視領域、特に短波光の透過率が高い非線形光学
材料が望まれている。However, known compounds with high SHG activity, such as 2-methyl-4-nitroaniline, m-nitroaniline, etc., are yellow-colored, so they have low transmittance to short-wave light, and they cannot be used for short-wave light by wavelength conversion. It is disadvantageous for this to occur. Therefore, a nonlinear optical material is desired that has high transmittance in the visible region, particularly in short-wavelength light.
[発明の目的]
従って、本発明の目的は、結晶、薄膜などバルク状態で
反転対称となり難く、かつ実質的に可視領域に吸収を持
たず、高い非線形光学効果を示す新規な有機非線形光学
材料及び有機非線形光学素子を提供することにある。[Objective of the Invention] Therefore, the object of the present invention is to provide a novel organic nonlinear optical material that is difficult to exhibit inversion symmetry in a bulk state such as a crystal or a thin film, has substantially no absorption in the visible region, and exhibits a high nonlinear optical effect. An object of the present invention is to provide an organic nonlinear optical element.
[発明の構成]
本発明の上記目的は、
(1) 下記一般式[11で表される化合物からなるこ
とを特徴とする非線形光学材料。[Structure of the Invention] The above objects of the present invention are as follows: (1) A nonlinear optical material characterized by comprising a compound represented by the following general formula [11].
一般式[11
(式中、Aは電子吸引性基、R1は置換アルキル基、R
2は一価の置換基を表す、nlよO〜3の整数を表す、
nが2以上のとき複数のR2は同じでも異なっていても
よく、また、隣接するR2が互いに連結して環を形成し
てもよい。)〈2) 上記(1)記載の非線形光学材料
からなる非線形光学素子。General formula [11 (wherein, A is an electron-withdrawing group, R1 is a substituted alkyl group, R
2 represents a monovalent substituent, nl represents an integer from O to 3,
When n is 2 or more, a plurality of R2s may be the same or different, or adjacent R2s may be linked to each other to form a ring. )<2) A nonlinear optical element made of the nonlinear optical material described in (1) above.
によって達成された。achieved by.
以下、本発明をより詳細に説明する。The present invention will be explained in more detail below.
上記一般式[I]において、Aで表される電子吸引性基
は、ハメットによって定義されるσp〉0の基であり、
例えばニトロ基、ホルミル基、カルバモイル基(例えば
メチルカルバモイル基、フェニルカルバモイル基等)、
カルボキシ基、スルファモイル基〈例えばメチルスルフ
ァモイル基等)、オキシカルボニル基(例えばメトキシ
カルボニル基、エトキシカルボニル基等)、シアノ基、
ジシアノビニル基等が挙げられる。In the above general formula [I], the electron-withdrawing group represented by A is a group with σp>0 defined by Hammett,
For example, nitro group, formyl group, carbamoyl group (e.g. methylcarbamoyl group, phenylcarbamoyl group, etc.),
Carboxy group, sulfamoyl group (e.g. methylsulfamoyl group, etc.), oxycarbonyl group (e.g. methoxycarbonyl group, ethoxycarbonyl group, etc.), cyano group,
Examples include dicyanovinyl group.
これらのうちで好ましいものは、ニトロ基、ホルミル基
、シアノ基、アルコキシカルボニル基である。Among these, preferred are a nitro group, a formyl group, a cyano group, and an alkoxycarbonyl group.
Aで表される電子吸引性基は、−OR,に対してパラ位
にあるのが好ましい。The electron-withdrawing group represented by A is preferably in the para position with respect to -OR.
R2で表される置換アルキル基の置換基とじては、ハロ
ゲン原子、アルコキシ基、シアン基、ニトロ基等を挙げ
ることができる。Examples of the substituent of the substituted alkyl group represented by R2 include a halogen atom, an alkoxy group, a cyan group, and a nitro group.
これらのうちで好ましいものはハロゲン原子であり、さ
らに好ましいものは臭素原子である。Among these, preferred is a halogen atom, and even more preferred is a bromine atom.
R2で表される一価の置換基としては、特に制限はなく
、電子供与性基、電子吸引性基のいずれでもよいが、π
電子共役系に大きな影響を与えない基が好ましい。The monovalent substituent represented by R2 is not particularly limited and may be either an electron-donating group or an electron-withdrawing group, but π
A group that does not significantly affect the electronic conjugation system is preferable.
上記電子吸引性基は、ハメットによって定義されるσp
>Oの基であり、例えばニトロ基、シアノ基、アルキル
スルホニル基(例えばメチルスルホニル基、エチルスル
ホニル基等)、ホルミル基、カルバモイル基(例えばメ
チルカルバモイル基、フェニルカルバモイル基等)、ス
ルファモイル基(例えばメチルスルファモイル基等)、
オキシカルボニル基(例えばメトキシカルボニル基、エ
トキシカルボニル基等)、ジシアノビニル基、カルボキ
シ基等が挙げられる。The electron-withdrawing group is σp defined by Hammett.
>O, such as nitro group, cyano group, alkylsulfonyl group (e.g. methylsulfonyl group, ethylsulfonyl group, etc.), formyl group, carbamoyl group (e.g. methylcarbamoyl group, phenylcarbamoyl group, etc.), sulfamoyl group (e.g. methylsulfamoyl group, etc.),
Examples thereof include oxycarbonyl group (eg, methoxycarbonyl group, ethoxycarbonyl group, etc.), dicyanovinyl group, and carboxy group.
上記電子供与性基は、ハロゲン原子またはハメットによ
って定義されるσp<Oの基であり、例えばアミノ基(
アミノ、メチルアミノ、ジメチルアミノ、L−2−ヒド
ロキシメチル−1−ピロリジニル等の基)、ヒドロキシ
ル基、アルコキシ基(メトキシ、エトキシ、ブトキシ等
の基)、アルキル基(メチル、エチル、プロピル等の基
)等が挙げられる。The electron donating group is a halogen atom or a group with σp<O defined by Hammett, for example, an amino group (
(groups such as amino, methylamino, dimethylamino, L-2-hydroxymethyl-1-pyrrolidinyl), hydroxyl groups, alkoxy groups (groups such as methoxy, ethoxy, butoxy), alkyl groups (groups such as methyl, ethyl, propyl, etc.) ) etc.
nが2以上のとき、隣接するR2が互いに連結して形成
される縮合環としては、例えばナフタレン、アントラセ
ン、インドール、キノリン、ベンゾイミダゾール等が挙
げられる。When n is 2 or more, examples of the condensed ring formed by connecting adjacent R2s include naphthalene, anthracene, indole, quinoline, benzimidazole, and the like.
以下に本発明に好ましく用いられる化合物の具体例を示
すが、これらに限定されない。Specific examples of compounds preferably used in the present invention are shown below, but the invention is not limited thereto.
以下余白
これらの化合物は、−数的合成法により、置換アルコキ
シベンゼン誘導体に、Aで表される電子吸引性基を導入
するか、フェノール誘導体に置換アルキルハライドを反
応させることにより容易に合成することができる。These compounds can be easily synthesized by introducing an electron-withdrawing group represented by A into a substituted alkoxybenzene derivative or by reacting a phenol derivative with a substituted alkyl halide using numerical synthesis methods. Can be done.
また、これらの化合物の一部は一般に市販されている試
薬(例えば、関東化学、東京化成、和光純薬、AIdr
ich社製品)として容易に入手できる。In addition, some of these compounds are generally available as commercially available reagents (e.g., Kanto Kagaku, Tokyo Kasei, Wako Pure Chemical, AIdr
It is easily available as a product of ich company).
合成例
(例示化合物1の合成)
20、のp−二トロフェノールナトリウムを 100m
1のジメチルホルムアミドに溶解し、これに26゜のジ
ブロムエタンを滴下し、室温にて10時間反応させた0
反応液を希塩酸中に注ぎ、析出した結晶をアセトニトリ
ルから再結晶し、目的物の結晶18gを得た。Synthesis Example (Synthesis of Exemplified Compound 1) 100 m of p-nitrophenol sodium of 20.
1 was dissolved in dimethylformamide, 26° dibromoethane was added dropwise thereto, and the mixture was reacted at room temperature for 10 hours.
The reaction solution was poured into dilute hydrochloric acid, and the precipitated crystals were recrystallized from acetonitrile to obtain 18 g of crystals of the desired product.
NMR,FD−マススペクトルにより構造を確認した。The structure was confirmed by NMR and FD-mass spectra.
融点:66〜67℃
本発明の化合物は、単結晶、粉末、溶液、支持体上に沈
積した薄膜(ラングミュア−プロジェット膜、蒸着膜な
ど)あるいはポリマーや液晶分子中にブレンドした形等
種々の形態で非線形光学素子とすることができる。また
、本発明の化合物をポリマーにペンダントしたり、包接
化合物あるいは付加物として用いることも可能である。Melting point: 66-67°C The compound of the present invention can be in various forms such as single crystal, powder, solution, thin film deposited on a support (Langmuir-Prodgett film, vapor deposited film, etc.), or blended into polymer or liquid crystal molecules. It can be made into a nonlinear optical element in the form of a nonlinear optical element. It is also possible to pendant the compound of the present invention to a polymer, or use it as an inclusion compound or adduct.
素子の形態は公知の導波路形状をとることができる0例
えば特開昭63−77035号公報で示されているよう
に、ファイバー形状、平板形状また単結晶の周囲をクラ
ツド材で囲んだ形状がある。The shape of the element can be a known waveguide shape. For example, as shown in Japanese Patent Application Laid-Open No. 63-77035, a fiber shape, a flat plate shape, or a shape in which a single crystal is surrounded by a cladding material are available. be.
本発明の非線形光学素子は、レーザー光の波長変jA(
高調波の発生等)、強度変調、スイッチング等に用いる
ことができる。The nonlinear optical element of the present invention has a wavelength change jA(
It can be used for harmonic generation, etc.), intensity modulation, switching, etc.
[実施例]
以下、実施例を示すが、本発明の実施態様はこれらに限
定されない。[Example] Examples will be shown below, but the embodiments of the present invention are not limited thereto.
実施例l
5HG効果を判定するのに一敗的に行われている粉末法
(S、に、Kurtz、 T、T、Perry ;
J、AOOI。Example 1 Powder method that has been unsuccessfully used to determine the effect of 5HG (S., Kurtz, T., T. Perry;
J.AOOI.
Phys、、 39.3798 (1968) )を用
いて本発明の化合物を評価した。Phys., 39.3798 (1968)) was used to evaluate the compounds of the present invention.
光源としてビーム径2市、繰り返し10pps 、パル
ス幅1Qns 、パルスエネルギー201JのQスイッ
チNd : YAGレーザ−(米国Quantel
Inter−rlatiOna1社 Y G 660
A、波長1064nrx)を使用して、ガラスセル中に
充填した粉末のサンプルに照射し、発生したSHG光(
532ni緑色光)をフィルターおよびモノクロメータ
−で分光し光電子増倍管で検知し、尿素を1とした時の
相対値を求めた。As a light source, a Q-switched Nd:YAG laser (manufactured by Quantel, USA) with a beam diameter of 2 cm, repetition rate of 10 pps, pulse width of 1 Qns, and pulse energy of 201 J was used.
Inter-rlatiOna1 YG 660
The generated SHG light (
532ni green light) was separated using a filter and a monochromator, detected using a photomultiplier tube, and the relative value when urea was taken as 1 was determined.
更に、メタノール中での可視領域の吸収も測定しな、結
果を併せて表1に示す。Furthermore, absorption in the visible region in methanol was also measured, and the results are also shown in Table 1.
表1
表1から明らかなように、本発明の化合物はSHG強度
ら強く、可視吸収も実質的にないことから、より短波光
にも使用できる優れた非線形光学材料であることが判る
。Table 1 As is clear from Table 1, the compound of the present invention has a strong SHG intensity and substantially no visible absorption, which indicates that it is an excellent nonlinear optical material that can be used even with shorter wavelength light.
実施例2
光源としてビーム径2關、繰り返し10ppS、パルス
幅7 ns 、パルスエネルギー201Jの色素レーザ
ー(米1Spectra Physics社 PDL−
2。Example 2 As a light source, a dye laser (USA 1 Spectra Physics PDL-
2.
1DS−867波長862nn )を使用し、実施例1
と同様にして 431n11の青色光強度を測定し、2
−メチル−4−ニトロアニリン(MNA)を1とした時
の相対値を求めた。結果を表2に示す。Example 1
Measure the blue light intensity of 431n11 in the same way as 2.
The relative value when -methyl-4-nitroaniline (MNA) is set to 1 was determined. The results are shown in Table 2.
色光発生に特に優れた非線形光学材料であることが判る
。It can be seen that this is a nonlinear optical material that is particularly excellent in generating colored light.
実施例3
実施例1で使用した本発明の化合物を、中空ファイバー
内に形成させて、非線形光学素子を作成した。ファイバ
ーの端面より波長11064nのYAGレーザー光を入
射すると、532nn+の第二高調波が観測された。Example 3 The compound of the present invention used in Example 1 was formed in a hollow fiber to create a nonlinear optical element. When a YAG laser beam with a wavelength of 11064n was input from the end face of the fiber, a second harmonic of 532nn+ was observed.
[発明の効果コ
本発明によれば、実質的に可視領域に吸収を持たず、使
用形態で反転対称となり難く、高いSHGが得られる有
機非線形光学材料及び有機非線形光学素子を提供するこ
とができる。[Effects of the Invention] According to the present invention, it is possible to provide an organic nonlinear optical material and an organic nonlinear optical element that have substantially no absorption in the visible region, are unlikely to exhibit inversion symmetry in the form of use, and can provide high SHG. .
Claims (2)
とを特徴とする非線形光学材料。 一般式[ I ] ▲数式、化学式、表等があります▼ (式中、Aは電子吸引性基、R_1は置換アルキル基、
R_2は一価の置換基を表す。nは0〜3の整数を表す
。nが2以上のとき複数のR_2は同じでも異なってい
てもよく、また、隣接するR_2が互いに連結して環を
形成してもよい。)(1) A nonlinear optical material comprising a compound represented by the following general formula [I]. General formula [I] ▲There are mathematical formulas, chemical formulas, tables, etc.▼ (In the formula, A is an electron-withdrawing group, R_1 is a substituted alkyl group,
R_2 represents a monovalent substituent. n represents an integer of 0 to 3. When n is 2 or more, a plurality of R_2 may be the same or different, or adjacent R_2 may be connected to each other to form a ring. )
形光学素子。(2) A nonlinear optical element made of the nonlinear optical material according to claim (1).
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19101988A JPH0240633A (en) | 1988-07-30 | 1988-07-30 | Nonlinear optical material and nonlinear optical element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19101988A JPH0240633A (en) | 1988-07-30 | 1988-07-30 | Nonlinear optical material and nonlinear optical element |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0240633A true JPH0240633A (en) | 1990-02-09 |
Family
ID=16267534
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19101988A Pending JPH0240633A (en) | 1988-07-30 | 1988-07-30 | Nonlinear optical material and nonlinear optical element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0240633A (en) |
-
1988
- 1988-07-30 JP JP19101988A patent/JPH0240633A/en active Pending
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