JP2729673B2 - Novel organic nonlinear optical material and method of converting light wavelength using the same - Google Patents

Novel organic nonlinear optical material and method of converting light wavelength using the same

Info

Publication number
JP2729673B2
JP2729673B2 JP1191626A JP19162689A JP2729673B2 JP 2729673 B2 JP2729673 B2 JP 2729673B2 JP 1191626 A JP1191626 A JP 1191626A JP 19162689 A JP19162689 A JP 19162689A JP 2729673 B2 JP2729673 B2 JP 2729673B2
Authority
JP
Japan
Prior art keywords
nonlinear optical
optical material
compound
same
light wavelength
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
JP1191626A
Other languages
Japanese (ja)
Other versions
JPH0355528A (en
Inventor
正樹 岡▲崎▼
暢彦 内野
康司 松尾
洋二 岡崎
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.)
Fujifilm Holdings Corp
Original Assignee
Fuji Photo Film Co Ltd
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 Fuji Photo Film Co Ltd filed Critical Fuji Photo Film Co Ltd
Priority to JP1191626A priority Critical patent/JP2729673B2/en
Publication of JPH0355528A publication Critical patent/JPH0355528A/en
Application granted granted Critical
Publication of JP2729673B2 publication Critical patent/JP2729673B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は波長変換素子等の非線形光学効果を利用する
各種素子に用いるに適した非線形光学材料に関する。ま
た、非線形光学材料を用いた光波長の変換方法に関す
る。
Description: TECHNICAL FIELD The present invention relates to a nonlinear optical material suitable for use in various devices utilizing a nonlinear optical effect such as a wavelength conversion device. Further, the present invention relates to a method for converting a light wavelength using a nonlinear optical material.

(従来の技術) 近年、非線形光学効果−レーザー光のような強い光電
界を与えたときに表われる、分極と電界との間の非線形
性−を有した材料が注目を集めている。
(Prior Art) In recent years, a material having a nonlinear optical effect-nonlinearity between polarization and an electric field, which appears when a strong optical electric field such as laser light is applied-has attracted attention.

かかる材料は、一般に非線形光学材料として知られて
おり、例えば次のものなどに詳しく記載されている。
“Nonliner Optical Properties of Organic and Polym
eric Material"ACS SYMPOSIUMSERIES 233 David J.Will
iams編(American Chemical Society、1983年刊)、
「有機非線形光学材料」加藤正雄、中西八郎監修(シー
・エム・シー社、1985年刊)。
Such materials are generally known as non-linear optical materials and are described in detail, for example, in:
“Nonliner Optical Properties of Organic and Polym
eric Material "ACS SYMPOSIUMSERIES 233 David J. Will
iams (American Chemical Society, 1983),
"Organic Nonlinear Optical Materials", edited by Masao Kato and Hachiro Nakanishi (CMC, 1985).

非線形光学材料の用途の1つに、2次の非線形効果に
基づいた第2高調波発生(SHG)および和周波、差周波
を用いた波長変換デバイスがある。これまで実用上用い
られているものは、ニオブ酸リチウムに代表される無機
質のペロブスカイト類である。しかし近年になり、電子
供与基および電子吸引基を有するπ電子共役系有機化合
物は前述の無機質を大きく上回る、非線形光学材料とし
ての諸性能を有していることが知られるようになった。
One of the applications of the nonlinear optical material is a second harmonic generation (SHG) based on a second-order nonlinear effect and a wavelength conversion device using a sum frequency and a difference frequency. Until now, inorganic perovskites represented by lithium niobate have been practically used. However, in recent years, it has become known that a π-electron conjugated organic compound having an electron donating group and an electron withdrawing group has various properties as a nonlinear optical material, which greatly exceeds the above-mentioned inorganic substances.

従って、この材料に用いるべき非線形光学応答を示す
有機化合物としては、まず分子状態での非線形感受率が
高いもの程望ましい。
Therefore, as an organic compound exhibiting a nonlinear optical response to be used for this material, a compound having a high nonlinear susceptibility in a molecular state is desirable.

しかしながら、2次の非線形光学材料として有用であ
るには、分子状態での性能のみでは不十分であり、集合
状態での分子配列に反転対称性の無いことが必須であ
る。しかるに現状では分子配列を予測することは極めて
困難であり、また全有機化合物中での存在確率も高いも
のではない。
However, to be useful as a second-order nonlinear optical material, performance in the molecular state alone is not sufficient, and it is essential that the molecular arrangement in the aggregated state has no inversion symmetry. However, at present, it is extremely difficult to predict the molecular arrangement, and the probability of existence in all organic compounds is not high.

(発明が解決しようとする課題) 従って本発明の第一の目的は、高い非線形応答性を示
す有機非線形光学材料を提供することにある。第二の目
的は非線形応答性のうち光波長の変換に関する応答性を
利用した方法を提供することにある。
(Problems to be Solved by the Invention) Accordingly, a first object of the present invention is to provide an organic nonlinear optical material exhibiting high nonlinear response. A second object is to provide a method that utilizes the response related to light wavelength conversion among the nonlinear responses.

(課題を解決するための手段) 本発明者らは、鋭意研究を重ねた結果、メソイオン化
合物又はその酸付加物、好ましくは下記一般式(I)で
表わされる化合物又はそれらの酸付加物を非線形光学応
答性化合物として用いることにより、本発明の目的が達
成可能なことを見出した。
(Means for Solving the Problems) As a result of intensive studies, the present inventors have found that a mesoionic compound or an acid adduct thereof, preferably a compound represented by the following general formula (I) or an acid adduct thereof is non-linearly converted. It has been found that the object of the present invention can be achieved by using the compound as an optically responsive compound.

一般式(I) (式中、Xはカルコゲン原子又はN−R4を表わす。
R1、R2、R3は水素原子、アルキル基、アリール基、を表
わし、R1とR2とで環を形成してもよい。R4はアリール基
を表わす。) メソイオン化合物は、シドノン(a)に代表される化
合物群であり シドノンなどのオキサジアゾール系化合物の他、オキ
サトリアゾール系化合物、チアゾール系化合物、ジチオ
ール系化合物などのオキソ型メソイオン化合物、シドノ
ンイミン系化合物、チアゾール系化合物、ジチオール系
化合物、などが知られており、これらに関しては、太田
正樹、加藤博著;日本化学雑誌、第86巻、第7号、661
〜673頁に詳しい。
General formula (I) (Wherein, X represents a chalcogen atom or N-R 4.
R 1 , R 2 and R 3 represent a hydrogen atom, an alkyl group or an aryl group, and R 1 and R 2 may form a ring. R 4 represents an aryl group. The mesoionic compounds are a group of compounds represented by sydnone (a) . In addition to oxadiazole compounds such as sydnones, oxatriazole compounds, thiazole compounds, oxo-type mesoionic compounds such as dithiol compounds, sydnonimine compounds, thiazole compounds, dithiol compounds, and the like are known. , By Masaki Ota and Hiroshi Kato; The Chemical Journal of Japan, Vol. 86, No. 7, 661
See page 673.

また一般式(I)で表わされるものの例を以下に示
す。
Examples of the compound represented by the general formula (I) are shown below.

これらの化合物の合成は、前記の太田らの文献を参照
して行なうことができる。
The synthesis of these compounds can be carried out with reference to the above-mentioned Ota et al.

後述の実施例より明らかなように、本発明の非線形光
学材料は波長変換用の材料として特に有用なものであ
る。しかしながら本発明の非線形光学材料の用途は波長
変換素子にかぎられるものではなく、非線形光学効果を
利用するものであればいかなる素子にも使用可能であ
る。本発明の非線形光学材料が用いられうる素子の具体
例として、波長変換素子以外に、光双安定素子(光記憶
素子、光パルス波形制御素子、光リミター、微分増幅素
子、光トランジスター、A/D変換素子、光論理素子、光
マルチバイブレーター、光フリップフロップ回路等)、
光変調素子および位相共役光学素子等が挙げられる。
As is clear from the examples described below, the nonlinear optical material of the present invention is particularly useful as a material for wavelength conversion. However, the application of the nonlinear optical material of the present invention is not limited to the wavelength conversion element, but can be used for any element utilizing the nonlinear optical effect. Specific examples of the device in which the nonlinear optical material of the present invention can be used include, in addition to the wavelength conversion device, optical bistable devices (optical storage device, optical pulse waveform control device, optical limiter, differential amplifier device, optical transistor, A / D Conversion element, optical logic element, optical multivibrator, optical flip-flop circuit, etc.),
An optical modulation element, a phase conjugate optical element, and the like can be given.

本発明の化合物は、例えば粉末の形、宿主格子(ポリ
マー、包接化合物、固溶体、液晶)中の分子の包有物の
形、支持体上に沈積した薄層の形(ラングミーア・ブロ
ジェット膜など)、単結晶の形、溶液の形等、種々の形
で非線形光学材料として用いることができる。
The compounds according to the invention can be used, for example, in the form of powder, in the form of inclusions of molecules in the host lattice (polymers, inclusion compounds, solid solutions, liquid crystals), in the form of thin layers deposited on supports (Langmea-Blodgett membranes). Etc.), a single crystal form, a solution form and the like can be used as a nonlinear optical material in various forms.

また本発明の化合物をペンダントの形でポリマー、ポ
リジアセチレンなどに結合させて用いることもできる。
Further, the compound of the present invention can be used by binding to a polymer, polydiacetylene or the like in a pendant form.

これらの方法について詳しくは前述のD.J.Williams編
の著作などに記載されている。
Details of these methods are described in the above-mentioned work by DJ Williams.

(実施例) 次に、本発明を実施例に基づいて詳しく説明する。(Examples) Next, the present invention will be described in detail based on examples.

実施例 第2高調波発生の測定をエス・ケー・クルツ(S.K.Ku
rtz)、ティー・ティー・ペリー(T.T.Perry)著、ジャ
ーナル オブ アプライド フィジックス(J.Appl.Phy
s.)39巻、3798頁(1968年刊)中に記載されている方法
に準じて、本発明の化合物の粉末に対して行なった。
Example 2nd harmonic generation measurement was performed by SKKu
rtz), TTPerry, Journal of Applied Physics (J. Appl. Phy)
s.) 39, p. 3798 (1968) was carried out on the powder of the compound of the present invention.

第1図に示した装置により測定を行った。 The measurement was performed using the apparatus shown in FIG.

すなわち、測定は、パルスYAGレーザー光(λ=1.064
μm、ビーム径≒1mmφ、ピークパワー≒10Mw/cm2)を
基本波に用い、第1図に示す評価装置にて、その第2高
調波の強度を測定した。測定は、尿素の第2高調波の強
度との相対比較で行った。また強度が弱い場合には目視
による観測を行った。特に、基本波の2光子吸収による
発光(おもに黄、赤の発光)と第2高調波とを区別する
ために、分光器を入れ、第2高調波のみを測定する様に
した。さらに粉末法の測定は、その物質の非線形性の有
無を判断することが主目的であり、その強度比は比線形
性の大きさの、参考値である。
That is, the measurement was performed using pulsed YAG laser light (λ = 1.064).
μm, a beam diameter of ≒ 1 mmφ, and a peak power of ≒ 10 Mw / cm 2 ) were used as fundamental waves, and the intensity of the second harmonic was measured by the evaluation apparatus shown in FIG. The measurement was performed by relative comparison with the intensity of the second harmonic of urea. When the intensity was low, visual observation was performed. In particular, in order to distinguish between the emission due to two-photon absorption of the fundamental wave (mainly yellow and red emission) and the second harmonic, a spectroscope was put in and only the second harmonic was measured. Further, the main purpose of the measurement by the powder method is to determine the presence or absence of nonlinearity of the substance, and the intensity ratio is a reference value of the magnitude of the specific linearity.

結果を表1に示した。 The results are shown in Table 1.

(発明の効果) これら粉末法により、SHG活性を示した化合物は下記
に示す方法により、波長変換素子としての使用が可能で
ある。
(Effect of the Invention) A compound exhibiting SHG activity by these powder methods can be used as a wavelength conversion element by the following method.

1.ファイバーのコア部分に上記化合物を単結晶化し、ク
ラッド材料としてガラスを用いた波長変換素子を作成
し、YAGレーザー光を入力しその第二高調波の発生が可
能である。さらに、他の方法として同様にして、導波路
型の波長変換素子を作成し、第二高調波の発生が可能で
ある。この時の位相整合方法には、チエレンコフ放射方
式を用いた。ただし、これらに限定されるだけでなく、
導波−導波の位相整合も可能である。波長変換波は第二
高調波に限定されるでけでなく、第三高調波、和および
差周波発生にも用いられる。
1. The above compound is monocrystallized in the core of the fiber, and a wavelength conversion device using glass as a cladding material is prepared. The second harmonic can be generated by inputting a YAG laser beam. Further, as another method, similarly, a waveguide type wavelength conversion element can be prepared to generate the second harmonic. At this time, the Cherenkov radiation method was used as the phase matching method. However, it is not limited to these,
Waveguide-waveguide phase matching is also possible. Wavelength-converted waves are not limited to second harmonics, but are also used for third harmonic, sum and difference frequency generation.

2.次に上記化合物を単結晶化し、そこからバルクの単結
晶を切り出し、YAGレーザー光を入力しその第二高調波
の発生が可能である。この時の位相整合方法には角度位
相整合を用いた。これらの、バルク単結晶はレーザーの
キャビティ外で用いられるだけでなく、LD励起固体レー
ザー等の固体レーザーのキャビティ内で用いる事で、波
長変換効率を高めることが出来る。さらには、外部共振
器型のLDの共振器内に配置することでも、波長変換効率
を高めることが出来る。
2. Next, the above compound is converted into a single crystal, and a bulk single crystal is cut out from the compound, and a second harmonic can be generated by inputting a YAG laser beam. At this time, an angle phase matching was used as a phase matching method. The wavelength conversion efficiency can be increased by using these bulk single crystals not only outside the laser cavity but also inside a solid laser cavity such as an LD pumped solid laser. Furthermore, the wavelength conversion efficiency can be increased by arranging it in the resonator of the external resonator type LD.

以上の単結晶化には、ブリッジマン法、溶媒蒸発法等
が用いられる。
For the above-mentioned single crystallization, a Bridgman method, a solvent evaporation method, or the like is used.

波長変換波は第二高調波に限定されるだけでなく、第
三高調波、和差周波発生にも用いられる。
The wavelength-converted wave is used not only for the second harmonic, but also for the generation of the third harmonic and the sum difference frequency.

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

第1図に粉末法の測定装置を示すが、図中の番号は下記
を示す。 1:粉末試料、2:基本波カットフィルター 3:分光器、4:フォトマル、5:アンプ (11):波長1.064μm、(12):0.532μm
FIG. 1 shows a measuring apparatus of the powder method, and the numbers in the figure indicate the following. 1: powder sample, 2: fundamental wave cut filter 3: spectroscope, 4: photomultiplier, 5: amplifier (11): wavelength 1.064 μm, (12): 0.532 μm

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】メソイオン化合物又はその酸付加物から成
る非線形光学材料。
1. A nonlinear optical material comprising a mesoionic compound or an acid adduct thereof.
【請求項2】メソイオン化合物又はその酸付加物が下記
の一般式(I)で表わされる化合物又はその酸付加物で
ある請求項(1)記載の非線形光学材料。 一般式(I) (式中、Xはカルコゲン原子又はN−R4を表わす。R1
R2、R3は水素原子、アルキル基、アリール基、を表わ
し、R1とR2とで環を形成してもよい。R4はアリール基を
表わす。)
2. The nonlinear optical material according to claim 1, wherein the mesoionic compound or an acid adduct thereof is a compound represented by the following general formula (I) or an acid adduct thereof. General formula (I) (Wherein, X represents a chalcogen atom or N-R 4 .R 1,
R 2 and R 3 represent a hydrogen atom, an alkyl group or an aryl group, and R 1 and R 2 may form a ring. R 4 represents an aryl group. )
【請求項3】レーザー光と非線形光学材料とを用いて光
波長の変換を行なう際に、非線形光学材料として請求項
(1)記載の有機非線形光学材料を用いる光波長の変換
方法。
3. A method for converting an optical wavelength using the organic nonlinear optical material according to claim 1, wherein the conversion of the optical wavelength using the laser light and the nonlinear optical material is performed.
JP1191626A 1989-07-25 1989-07-25 Novel organic nonlinear optical material and method of converting light wavelength using the same Expired - Fee Related JP2729673B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1191626A JP2729673B2 (en) 1989-07-25 1989-07-25 Novel organic nonlinear optical material and method of converting light wavelength using the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1191626A JP2729673B2 (en) 1989-07-25 1989-07-25 Novel organic nonlinear optical material and method of converting light wavelength using the same

Publications (2)

Publication Number Publication Date
JPH0355528A JPH0355528A (en) 1991-03-11
JP2729673B2 true JP2729673B2 (en) 1998-03-18

Family

ID=16277774

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1191626A Expired - Fee Related JP2729673B2 (en) 1989-07-25 1989-07-25 Novel organic nonlinear optical material and method of converting light wavelength using the same

Country Status (1)

Country Link
JP (1) JP2729673B2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01185527A (en) * 1988-01-19 1989-07-25 Ricoh Co Ltd Nonlinar optical material

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3808309A1 (en) * 1988-03-12 1989-09-21 Merck Patent Gmbh TWITTERIONIC NLO CHROMOPHORE

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01185527A (en) * 1988-01-19 1989-07-25 Ricoh Co Ltd Nonlinar optical material

Also Published As

Publication number Publication date
JPH0355528A (en) 1991-03-11

Similar Documents

Publication Publication Date Title
WO1980001225A1 (en) 2-methyl-4-nitro-aniline nonlinear optical devices
Cao et al. Recovery of second-order optical nonlinearity in annealed proton-exchanged LiNbO/sub x
Bechthold et al. Linear and nonlinear optical properties of Ca3 (VO4) 2
US4879479A (en) Poly-yne nonlinear optical materials
Zyss et al. Optical parametric interactions in 3-methyl-4-nitropyridine-1-oxide (POM) single crystals
US4756598A (en) Second harmonic generation with 5-chloro-2-nitroaniline
JP2729673B2 (en) Novel organic nonlinear optical material and method of converting light wavelength using the same
JPH04121717A (en) Novel organic nonlinear optical material and method for converting light wavelength by using this material
US5220451A (en) Second-order nonlinear optical device
US5072451A (en) Molecular crystal and method for converting light wavelength by use thereof
JPH03164722A (en) Organic nonlinear optical material and method for converting wavelength of light with same
US5080832A (en) Optically nonlinear aromatic carboxylic acid complexes
JPH021831A (en) Waveguide type wavelength conversion element
JP2694562B2 (en) Novel organic nonlinear optical material and method of converting light wavelength using the same
US3982136A (en) Ternary ferroelectric fluoride nonlinear devices
JPH0355527A (en) Novel organic nonlinear optical material and method for converting light wavelength by using this material
JP2574697B2 (en) Novel organic nonlinear optical material and method of converting light wavelength using the same
JPH06128234A (en) Compound having asymmetric carbon atom and non-linear optical material composed of the compound
US4992214A (en) Optically nonlinear aromatic carboxylic acid complexes
Sutter et al. Linear and nonlinear optical properties of 2-(N-prolinol)-5-nitropyridine (pnp
JPH06118462A (en) Organic nonlinear optical material
JPH0355526A (en) Novel organic nonlinear optical material and method for converting light wavelength by using this material
JP2723797B2 (en) Wavelength conversion element and laser device using the same
JP2871202B2 (en) Nonlinear optical element
JPH03194519A (en) Nonlinear optical material

Legal Events

Date Code Title Description
R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

LAPS Cancellation because of no payment of annual fees
S111 Request for change of ownership or part of ownership

Free format text: JAPANESE INTERMEDIATE CODE: R313111

R370 Written measure of declining of transfer procedure

Free format text: JAPANESE INTERMEDIATE CODE: R370