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JPH0660984B2 - Organic nonlinear optical material - Google Patents
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JPH0660984B2 - Organic nonlinear optical material - Google Patents

Organic nonlinear optical material

Info

Publication number
JPH0660984B2
JPH0660984B2 JP4871387A JP4871387A JPH0660984B2 JP H0660984 B2 JPH0660984 B2 JP H0660984B2 JP 4871387 A JP4871387 A JP 4871387A JP 4871387 A JP4871387 A JP 4871387A JP H0660984 B2 JPH0660984 B2 JP H0660984B2
Authority
JP
Japan
Prior art keywords
nonlinear optical
optical material
group
organic nonlinear
present
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 - Fee Related
Application number
JP4871387A
Other languages
Japanese (ja)
Other versions
JPS63216033A (en
Inventor
栗原  隆
俊邦 戒能
史朗 松元
哲哉 後藤
啓一 江川
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toray Industries Inc
NTT Inc
Original Assignee
Nippon Telegraph and Telephone Corp
Toray Industries Inc
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Nippon Telegraph and Telephone Corp, Toray Industries Inc filed Critical Nippon Telegraph and Telephone Corp
Priority to JP4871387A priority Critical patent/JPH0660984B2/en
Publication of JPS63216033A publication Critical patent/JPS63216033A/en
Publication of JPH0660984B2 publication Critical patent/JPH0660984B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • 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
    • G02F1/35Non-linear optics
    • G02F1/355Non-linear optics characterised by the materials used
    • G02F1/361Organic materials

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Organic Low-Molecular-Weight Compounds And Preparation Thereof (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、光双安定素子などの非線形光学素子用素材と
して有用な有機非線形光学材料に関する。
The present invention relates to an organic nonlinear optical material useful as a material for a nonlinear optical element such as an optical bistable element.

〔従来の技術〕[Conventional technology]

三次の非線形光学材料は、第三高調波発生(以下、TH
Gと略す)による周波数変換機能を有しているほか、光
双安定現象を利用した光スイッチ、光メモリへの応用な
どが可能であるため、将来の光素子の中心素材として、
活発な研究開発が進められている。なかでも、有機非線
形光学材料は、(1)KDP・LiNbOなどの無機強
誘電体結晶に比べ、非線形光学定数が大きい、(2)ガリ
ウム−ヒ素などの無機半導体に比べ応答速度が速い、
(3)高速応答・室温動作が確認されている塩化第一銅
(CuCl)では困難なμmオーダーの薄膜化が容易な
こと、など将来の材料では同時に満たされることのなか
つた要求条件をすべて満足する可能性を秘めており、活
発な材料探索が進められている。
The third-order nonlinear optical material is used for the third harmonic generation (hereinafter, TH
In addition to having a frequency conversion function by abbreviated as G), it can be applied to optical switches and optical memories using the optical bistable phenomenon.
Active research and development is underway. Among them, organic nonlinear optical materials have (1) larger nonlinear optical constants than inorganic ferroelectric crystals such as KDP / LiNbO 3 , (2) faster response speed than inorganic semiconductors such as gallium-arsenic,
(3) High-speed response · Room temperature operation has been confirmed. It is difficult to make thin films of the μm order, which is difficult with cuprous chloride (CuCl). There is a possibility of doing so, and active material search is underway.

現在、三次の効果の大きい有機非線形光学材料は、ポ
リジアセチレン〔特に、PTS:2,4−ヘキサジイン
−1,6−ビス(p−トルエンスルホナート)〕、ポリ
アセチレンに代表されるπ共役高分子系と、アミノニ
トロスチルベン(特に、DEANS:N,N−ジエチル
−4−アミノ−4′−ニトロスチルベン)に代表され
る、ドナー・アクセプターを非対称に置換した低分子系
の2種に分類できる。
At present, organic non-linear optical materials having a large third-order effect are polydiacetylene [particularly, PTS: 2,4-hexadiyne-1,6-bis (p-toluenesulfonate)], a π-conjugated polymer system represented by polyacetylene. And aminonitrostilbene (particularly, DEANS: N, N-diethyl-4-amino-4′-nitrostilbene), which is a low molecular weight system in which a donor / acceptor is asymmetrically substituted.

〔発明が解決しようとする問題点〕 のπ共役高分子系の非線形性は、価電子帯の自由電子
の分極を根源としているため、無機半導体と極めて類似
した欠点、すなわち、狭いバンドギヤツプに基づいた共
鳴効果による応答速度の低下から逃れられない。ドナ
ー・アクセプター非対称置換低分子系は、現状(DEA
NS)以上に効果を大きくしようとすると分子内電荷移
動による吸収帯の長波長化によつて、と同様の欠点を
露呈する。更に、結晶が非対称中心構造をとるものの一
部は、二次効果の混在によつて、非線形動作の信頼性に
問題を生じる。
Since the non-linearity of the π-conjugated polymer system in [Problems to be solved by the invention] is rooted in the polarization of free electrons in the valence band, it is based on a drawback very similar to that of an inorganic semiconductor, that is, a narrow band gap. It cannot escape from the decrease in response speed due to the resonance effect. A donor-acceptor asymmetrically substituted small molecule system is currently in use (DEA
If it is attempted to increase the effect more than NS), the same drawback as in (1) is exposed due to the lengthening of the absorption band due to intramolecular charge transfer. Further, some of the crystals having an asymmetric center structure cause a problem in the reliability of nonlinear operation due to the mixing of secondary effects.

本発明の目的は、上記従来技術の欠点を克服し、高速・
高効率の光非線応答を示す有機非線形光学材料を提供す
ることにある。
The object of the present invention is to overcome the above-mentioned drawbacks of the prior art,
An object of the present invention is to provide an organic nonlinear optical material exhibiting highly efficient optical non-linear response.

〔問題点を解決するための手段〕[Means for solving problems]

本発明を概説すれば、本発明は有機非線形光学材料に関
する発明であつて、下記一般式I: (ただし、Dは電子供与性基を示す)で表されることを
特徴とする。
Briefly describing the present invention, the present invention relates to an organic nonlinear optical material, which is represented by the following general formula I: (Wherein D represents an electron-donating group).

本発明による有機非線形光学材料の主要な特徴は、吸収
の長波長化を抑制して応答速度の低下を防いでいる上
に、従来になく大きな三次の非線形光学効果を有する点
である。これは、非線形光学効果を大きくしようとする
と、π共役の拡大や電荷移動の増大による吸収の長波長
化を伴うという従来技術の欠点を、比較的長いπ共役系
(22π電子系のテレフタル−ビス−アニリン:TB
A)の分子両端に、ドナー性の強い分極基を対称置換す
ることによつて解決したものである。
The main characteristic of the organic nonlinear optical material according to the present invention is that it suppresses the absorption of a longer wavelength to prevent the response speed from lowering, and also has a larger third-order nonlinear optical effect than ever before. This is due to the disadvantage of the conventional technique that, when an attempt is made to increase the non-linear optical effect, the absorption wavelength becomes longer due to the expansion of π conjugation and the increase of charge transfer. -Aniline: TB
This is solved by symmetrically substituting a polarizing group having a strong donor property at both ends of the molecule A).

本発明の有機非線形光学材料は、従来から報告例のある
ようなドナー・アクセプターを非対称に置換した低分子
系とは異なり、基底状態での分極が小さい上、励起状態
の電子雲が対称中心構造をとることに特徴がある。した
がつて、本発明の有機非線形光学材料は本質的には二次
の非線形光学効果を発現しない材料であるから、二次の
非線形光学効果の混在によつて、非線形光学素子の動作
が影響を受けることもない。
The organic nonlinear optical material of the present invention has a small polarization in the ground state and has a symmetric center structure in the excited electron cloud, unlike a small molecule system in which a donor / acceptor is asymmetrically substituted, which has been reported in the past. It is characterized by taking. Therefore, since the organic nonlinear optical material of the present invention is essentially a material that does not exhibit the second-order nonlinear optical effect, the operation of the nonlinear optical element may be affected by the mixture of the second-order nonlinear optical effect. I do not receive it.

本発明の有機非線形光学材料は、前記一般式Iで示され
る。
The organic nonlinear optical material of the present invention is represented by the above general formula I.

ここで、基Dは、アミノ基、モノあるいはジアルキルア
ミノ基、モノあるいはジ(ヒドロキシアルキル)アミノ
基が代表的である。
Here, the group D is typically an amino group, a mono- or dialkylamino group, and a mono- or di (hydroxyalkyl) amino group.

例えば、ドナー(D)がジアルキルアミノ基である場
合、ジエチルアミノ基とジメチルアミノ基とでは、ドナ
ー性に優り、平面共役構造をとりやすいジエチルアミノ
基のほうが、大きな非線形光学効果を発現する。更に、
フレキシビリテイの増大により、溶解性が高く、溶融結
晶化に適した融点を示す。エチル−ヒドロキシエチルア
ミノ基ドナーにすると、溶解性は、更に向上する。Dが
ジメチルアミノ基の材料をDM−TBA、ドナーDがジ
エチルアミノ基の材料をDE−TBA、Dがエチレン−
ヒドロキシエチルアミノ基の材料をEOE−TBAと略
称する。
For example, in the case where the donor (D) is a dialkylamino group, the diethylamino group and the dimethylamino group are more excellent in the donor property, and the diethylamino group, which easily takes a plane conjugated structure, exhibits a larger nonlinear optical effect. Furthermore,
Due to the increased flexibility, it has a high solubility and a melting point suitable for melt crystallization. The solubility is further improved by using an ethyl-hydroxyethylamino group donor. D-dimethylamino group material is DM-TBA, donor D is diethylamino group material is DE-TBA, D is ethylene-
The hydroxyethylamino group material is abbreviated as EOE-TBA.

以下、前記一般式Iで表される化合物の製造例を示す
が、これらに限定されない。
The production examples of the compound represented by the general formula I are shown below, but the invention is not limited thereto.

製造例1、DE−TBAの合成 N,N−ジエチル−p−フエニレンジアミン(3.6
g、22mmol)のベンゼン−エタノール(1:1)溶
液に、テレフタルアルデヒド(1.3g、10mmolの
エタノール溶液と触媒量のベンゼンスルホン酸を加え、
室温で1時間かくはんした。更に、油浴上で、3時間、
加熱還流しした。反応液を室温まで冷し、生成物を完全
に析出させた後、これをろ取、冷エタノールにて充分洗
浄した。メチルシクロヘキサン:o−ジクロロベンゼン
(1:1)混合溶媒を用いて再結晶し、橙色うろこ状結
晶(2.6g)を得た。融点:227℃。第1図に、溶
融結晶化薄膜のUV−VISスペクトルを示す。すなわ
ち第1図は本発明による有機非線形光学材料:DE−T
BAの溶融結晶化薄膜のUV−VISスペクトルを波長
(nm、横軸)と吸光度(任意単位、縦軸)との関係で
示したグラフである。第1図から明らかなように、上記
薄膜は長波長領域(約700nm以上)に吸収を持たな
い。
Production Example 1, Synthesis of DE-TBA N, N-diethyl-p-phenylenediamine (3.6
g, 22 mmol of benzene-ethanol (1: 1) solution, terephthalaldehyde (1.3 g, 10 mmol of ethanol solution and catalytic amount of benzenesulfonic acid were added,
Stir at room temperature for 1 hour. Furthermore, on an oil bath for 3 hours,
Heated to reflux. The reaction solution was cooled to room temperature to completely precipitate the product, which was collected by filtration and sufficiently washed with cold ethanol. Recrystallization was performed using a mixed solvent of methylcyclohexane: o-dichlorobenzene (1: 1) to obtain orange scaly crystals (2.6 g). Melting point: 227 ° C. FIG. 1 shows the UV-VIS spectrum of the melt-crystallized thin film. That is, FIG. 1 shows an organic nonlinear optical material according to the present invention: DE-T.
It is the graph which showed the UV-VIS spectrum of the melt-crystallized thin film of BA with the relationship of wavelength (nm, abscissa) and light absorbency (arbitrary unit, ordinate). As is clear from FIG. 1, the thin film has no absorption in the long wavelength region (about 700 nm or more).

製造例2、DM−TBAの合成 N,N−ジメチル−p−フエニレンジアミン(3.0
g、22mmol)のエタノール溶液に、テレフタルアル
デヒド(1.3g、10mmol)のエタノール溶液と触
媒量のベンゼンスルホン酸を加え、室温で1時間かくは
んした。更に、油浴上で、3時間、加熱還流した。析出
物をろ取、冷エタノールにて充分洗浄したのち、o−ジ
クロロベンゼンより再結晶し橙色の結晶(2.2g)を
得た。融点:300℃以上。
Production Example 2, Synthesis of DM-TBA N, N-dimethyl-p-phenylenediamine (3.0
g, 22 mmol) in ethanol solution, terephthalaldehyde (1.3 g, 10 mmol) in ethanol solution and catalytic amount of benzenesulfonic acid were added, and stirred at room temperature for 1 hour. Furthermore, the mixture was heated under reflux on an oil bath for 3 hours. The precipitate was collected by filtration, washed thoroughly with cold ethanol, and recrystallized from o-dichlorobenzene to obtain orange crystals (2.2 g). Melting point: 300 ° C or higher.

製造例3、EOE−TBAの合成 硫酸−4−アミノ−N−(β−ヒドロキシエチル)−N
−エチルアニリン(9.3g、33mmol)のエタノー
ル−水(1:1)溶液に、水酸化ナトリウム水溶液を加
え、弱酸性にすると均一溶液となるから、この溶液にテ
レフタルアルデヒド(2.2g、16mmol)のエタノ
ール溶液を加え室温で3時間、更に、油浴上で1時間加
熱還流した。反応液を室温まで冷却し、生成物を析出さ
せ、これをろ取、冷エタノール−水(1:4)混合媒更
に冷水で充分洗浄した。得られた粗結晶はエタノール−
水(1:1)混合溶媒から再結晶し、橙色結晶5.5g
を得た。融点113〜115℃。
Production Example 3, Synthesis of EOE-TBA Sulfuric acid-4-amino-N- (β-hydroxyethyl) -N
-Ethylaniline (9.3 g, 33 mmol) was added to an ethanol-water (1: 1) solution, and an aqueous solution of sodium hydroxide was added to the solution to make it weakly acidic to give a homogeneous solution. The ethanol solution of 1) was added, and the mixture was heated under reflux for 3 hours at room temperature and further for 1 hour on an oil bath. The reaction solution was cooled to room temperature to precipitate a product, which was collected by filtration and thoroughly washed with a cold ethanol-water (1: 4) mixed medium and cold water. The crude crystals obtained were ethanol-
Recrystallized from water (1: 1) mixed solvent, orange crystals 5.5 g
Got Melting point 113-115 [deg.] C.

〔実施例〕〔Example〕

以下、本発明を実施例により更に具体的に説明するが、
本発明はこれら実施例に限定されない。
Hereinafter, the present invention will be described in more detail with reference to Examples.
The present invention is not limited to these examples.

実施例1〜3 製造例1〜3で得られた化合物について非線形光学特性
を測定した。
Examples 1 to 3 Nonlinear optical characteristics of the compounds obtained in Production Examples 1 to 3 were measured.

THG測定の方法は、以下に述べる通りである。光源に
は、Nd:YAGレーザー(波長1.06μm、10H
z、50MW/cm2)を用い、可視光をカツトした後、レ
ンズで集光したビームを試料に照射し、試料より放射さ
れた光をモノクロメータに通して、THG光(0.35
μm)のみの強度をホトマルで検知した。測定試料は、
DM−TBA、DE−TBA、EOE−TBAを105
〜120μmの粒径に粉砕したものを用いた。更に、観
測されるTHG光が、尿素やMNA(2−メチル−4−
ニトロアニリン)に見られるような二次のカスケード効
果〔基本波(ω)と第二高調波(2ω)の和周波による
3ωの発生〕ではなく、純粋に三次の効果のみによるこ
とを観認するために、同一試料の第二高調波発生(以
下、SHGと略す)についても測定した。その結果を下
記表1に示す。なお、比較資料として、尿素、MNA及
びDEANSの結果を併記した。
The method of THG measurement is as described below. Nd: YAG laser (wavelength 1.06 μm, 10H
z, 50 MW / cm 2 ) and cut visible light, irradiate the sample with the beam condensed by the lens, and let the light emitted from the sample pass through a monochromator to produce THG light (0.35
The intensity of only (μm) was detected by Photomal. The measurement sample is
DM-TBA, DE-TBA, EOE-TBA 105
What was pulverized to a particle size of 120 μm was used. Furthermore, the THG light observed is urea or MNA (2-methyl-4-).
Recognize that the effect is purely the third-order effect, not the second-order cascade effect [Nitroaniline] [generation of 3ω by the sum frequency of the fundamental wave (ω) and the second harmonic (2ω)]. Therefore, the second harmonic generation (hereinafter abbreviated as SHG) of the same sample was also measured. The results are shown in Table 1 below. As comparative data, the results of urea, MNA and DEANS are also shown.

〔発明の効果〕 以上説明したように、本発明の有機非線形光学材料は、
従来になく大きな三次の非線光学効果を有するので、こ
れを利用した光学素子、例えば光双安定性素子、光スイ
ツチ、光メモリなど将来の光通信用光集積素子の中心素
材として利用できる。
As described above, the organic nonlinear optical material of the present invention is
Since it has a larger third-order nonlinear optical effect than ever before, it can be used as a central material for future optical integrated devices for optical communication, such as optical devices using this, such as optical bistable devices, optical switches, and optical memories.

【図面の簡単な説明】[Brief description of drawings]

第1図は、本発明による有機非線形光学材料:DE−T
BAの溶融結晶化薄膜のUV−VISスペクトル図であ
る。
FIG. 1 shows an organic nonlinear optical material according to the present invention: DE-T
It is a UV-VIS spectrum figure of the melt-crystallized thin film of BA.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 松元 史朗 茨城県那珂郡東海村大字白方字白根162番 地 日本電信電話株式会社茨城電気通信研 究所内 (72)発明者 後藤 哲哉 滋賀県大津市園山1丁目1番1号 東レ株 式会社滋賀事業場内 (72)発明者 江川 啓一 滋賀県大津市園山1丁目1番1号 東レ株 式会社滋賀事業場内 (56)参考文献 特開 昭61−78748(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Shiro Matsumoto, Tokai-mura, Naka-gun, Ibaraki 162 Shirahane, Shirahata, Nippon Telegraph and Telephone Corporation Ibaraki Telecommunications Research Institute (72) Inventor Tetsuya Goto Otsu, Shiga Prefecture 1-11 Sonoyama Toray Co., Ltd. Shiga Plant (72) Inventor Keiichi Egawa 1-1-1 Sonoyama, Otsu City, Shiga Toray Co. Ltd. Shiga Plant (56) Reference JP 61-78748 (JP, A)

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】下記一般式I: (ただし、Dは電子供与性基を示す)で表されることを
特徴とする有機非線形光学材料。
1. The following general formula I: (However, D shows an electron-donating group), The organic nonlinear optical material characterized by the above-mentioned.
【請求項2】該基Dが、アミノ基である特許請求の範囲
第1項記載の有機非線形光学材料。
2. The organic nonlinear optical material according to claim 1, wherein the group D is an amino group.
【請求項3】該基Dが、モノ又はジアルキルアミノ基で
ある特許請求の範囲第1項又は第2項記載の有機非線形
光学材料。
3. The organic nonlinear optical material according to claim 1 or 2, wherein the group D is a mono- or dialkylamino group.
【請求項4】該基Dが、モノ又はジ(ヒドロキシアルキ
ル)アミノ基である特許請求の範囲第1項又は第2項記
載の有機非線形光学材料。
4. The organic nonlinear optical material according to claim 1 or 2, wherein the group D is a mono- or di (hydroxyalkyl) amino group.
JP4871387A 1987-03-05 1987-03-05 Organic nonlinear optical material Expired - Fee Related JPH0660984B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4871387A JPH0660984B2 (en) 1987-03-05 1987-03-05 Organic nonlinear optical material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4871387A JPH0660984B2 (en) 1987-03-05 1987-03-05 Organic nonlinear optical material

Publications (2)

Publication Number Publication Date
JPS63216033A JPS63216033A (en) 1988-09-08
JPH0660984B2 true JPH0660984B2 (en) 1994-08-10

Family

ID=12810946

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4871387A Expired - Fee Related JPH0660984B2 (en) 1987-03-05 1987-03-05 Organic nonlinear optical material

Country Status (1)

Country Link
JP (1) JPH0660984B2 (en)

Also Published As

Publication number Publication date
JPS63216033A (en) 1988-09-08

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