JPH05307202A - Nonlinear optical element - Google Patents

Nonlinear optical element

Info

Publication number
JPH05307202A
JPH05307202A JP3327893A JP3327893A JPH05307202A JP H05307202 A JPH05307202 A JP H05307202A JP 3327893 A JP3327893 A JP 3327893A JP 3327893 A JP3327893 A JP 3327893A JP H05307202 A JPH05307202 A JP H05307202A
Authority
JP
Japan
Prior art keywords
light
nonlinear optical
reference light
polarization
optical
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.)
Granted
Application number
JP3327893A
Other languages
Japanese (ja)
Other versions
JP3214129B2 (en
Inventor
Yoshihiro Yokozawa
伊裕 横沢
Kazuhiro Morita
一弘 森田
Hidetomo Ashitaka
秀知 芦高
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.)
Ube Corp
Original Assignee
Ube Industries 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 Ube Industries Ltd filed Critical Ube Industries Ltd
Priority to JP03327893A priority Critical patent/JP3214129B2/en
Publication of JPH05307202A publication Critical patent/JPH05307202A/en
Application granted granted Critical
Publication of JP3214129B2 publication Critical patent/JP3214129B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To enable the taking out of a change in refractive index by a cubic nonlinear optical effect with a high sensitivity by forming a nonlinear optical material which has cubic nonlinearity and optical-rotatory dispersion characteristic. CONSTITUTION:This nonlinear optical material 21 has the cubic nonlinearity and optical- rotatory dispersion characteristic and its optical path length is set in such a manner that the plane of polarization rotates 90 deg. when reference light 22 of a wavelength lambda1 is transmitted therethrough as linearly polarized light in a perpendicular direction by a polarizer 24. Then, the reference light 23, the plane of polarization of which is rotated by 90 deg. to be in the horizontal direction is shut off by an analyzer 25 having the bearing in the perpendicular direction when control light 23 is not made incident. On the other hand, the control light 23 is strong light and, therefore, the light induces the nonlinear optical effect in the nonlinear optical material 21 when the control light 23 of a wavelength lambda2 is made incident as the linearly polarized light in the perpendicular direction on the nonlinear optical material 21 by the polarizer 24. Namely, the nonlinear optical effect is induced on the plane of polarization of the reference light 22 in the state where the plane of polarization of the reference light 22 inclines from the plane of polarization of the control light 23 and, therefore, the reference light 22 is eventually made into elliptically polarized light. A perpendicular component is, therefore, generated in the reference light 22 and is passed through an analyzer 25.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、オプトエレクトロニク
ス、光情報処理、光通信等の分野において用いられる非
線形光学材料に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a non-linear optical material used in the fields of optoelectronics, optical information processing, optical communication and the like.

【0002】[0002]

【従来の技術およびその問題点】非線形光学材料は、レ
ーザー光の強電界下、二次以上の非線形応答を示す材料
であって、周波数変換、発振、スイッチング等の光信号
処理において重要な素材である。特に、三次非線形光学
材料は、光が有する高速性、並列性という優れた特性を
十分に発揮させた次世代の光通信、情報処理における基
幹素材として注目されている。この三次非線形光学材料
を用いた非線形光学素子は、光の照射に対して屈折率が
変化することを利用しようとするものであり、例えば、
光カーシャッターが知られている。光カーシャッターは
非線形光学材料に強い制御光を照射して、非線形光学材
料を透過する参照光の偏光状態を変化させることによ
り、光−光スイッチング、光−光制御を行うものであ
る。
2. Description of the Related Art Nonlinear optical materials are materials that exhibit a second-order or higher nonlinear response under a strong electric field of laser light, and are important materials in optical signal processing such as frequency conversion, oscillation, and switching. is there. In particular, the third-order nonlinear optical material has been attracting attention as a basic material for next-generation optical communication and information processing, which fully exhibits the excellent characteristics of light such as high speed and parallelism. A non-linear optical element using this third-order non-linear optical material intends to utilize that the refractive index changes with the irradiation of light.
Optical car shutters are known. The optical Kerr shutter performs light-light switching and light-light control by irradiating the nonlinear optical material with strong control light and changing the polarization state of the reference light that passes through the nonlinear optical material.

【0003】図1に従来の光カーシャッターの一例の概
略図を示す。11は非線形光学材料であり、CS2を光
学セルに入れたものである。14は方位を垂直方向に設
定した偏光子であり、波長λ1 の参照光12は偏光子1
4により垂直方向に偏光する。したがって、制御光13
が入射されていない時、参照光は、方位を水平方向に設
定した検光子15により遮断される。一方、波長λ2
制御光13を方位が45゜傾いた偏光子16により偏光
面が45゜傾いた直線偏光として、非線形光学材料11
に入射させると、制御光は強い光であるため非線形光学
材料11に非線形屈折率変化を引き起こす。この時、制
御光の偏光面は参照光の偏光面に対して傾いているた
め、参照光は楕円偏光となる。そのため、参照光に水平
成分が生じ、これが検光子15を透過する。このよう
に、従来、光−光スイッチングを実現するには、例えば
参照光に対して偏光面を傾けるといった工夫を制御光の
偏光に加えたり、さらに検光子も参照光の偏光子と直交
させる必要があるため、様々な方位の偏光子を準備しな
くてはならず、このために素子の構成が複雑になるとい
う問題があった。
FIG. 1 shows a schematic view of an example of a conventional optical car shutter. Reference numeral 11 is a non-linear optical material in which CS 2 is put in an optical cell. 14 is a polarizer setting the orientation in the vertical direction, the reference beam 12 with a wavelength lambda 1 is the polarizer 1
4 causes the light to be polarized in the vertical direction. Therefore, the control light 13
When is not incident, the reference light is blocked by the analyzer 15 whose azimuth is set to the horizontal direction. On the other hand, the control light 13 having the wavelength λ 2 is converted into linearly polarized light whose polarization plane is tilted by 45 ° by the polarizer 16 whose azimuth is tilted by 45 °, and the nonlinear optical material 11
When the light is incident on, the control light is a strong light and causes a nonlinear refractive index change in the nonlinear optical material 11. At this time, since the polarization plane of the control light is inclined with respect to the polarization plane of the reference light, the reference light becomes elliptically polarized light. Therefore, a horizontal component is generated in the reference light, which is transmitted through the analyzer 15. As described above, conventionally, in order to realize light-light switching, it is necessary to add a device such as tilting the polarization plane with respect to the reference light to the polarization of the control light, and also to make the analyzer orthogonal to the polarizer of the reference light. Therefore, it is necessary to prepare polarizers of various orientations, which causes a problem that the structure of the device is complicated.

【0004】[0004]

【問題点を解決するための手段】本発明の目的は、前記
問題点を解決し、旋光性物質の旋光分散特性を利用する
ことにより、三次非線形光学効果による屈折率変化を感
度良く取り出すことができる新規な非線形光学素子を提
供することである。本発明は、参照光の偏光状態を参照
光の波長と異なる波長の光で制御する非線形光学素子で
あって、非線形光学材料が三次非線形性と旋光分散特性
を有することを特徴とする非線形光学素子に関する。
SUMMARY OF THE INVENTION An object of the present invention is to solve the above-mentioned problems and to take out the change in refractive index due to the third-order nonlinear optical effect with high sensitivity by utilizing the optical rotatory dispersion characteristic of an optical rotatory substance. It is to provide a novel nonlinear optical element that can be used. The present invention is a non-linear optical element for controlling the polarization state of reference light with light having a wavelength different from the wavelength of reference light, wherein the non-linear optical material has third-order non-linearity and optical rotation dispersion characteristics. Regarding

【0005】本発明の非線形光学材料の形態としては、
旋光分散性能を有する物質及び三次非線形性を有する物
質をポリマー中にドープしたものや、旋光分散性能を有
する物質を三次非線形性を有するポリマー中にドープし
たもの、逆に、三次非線形性を有する物質を旋光分散性
能を有するポリマー中にドープしたものが挙げられる。
あるいは、旋光分散性能を有する物質と三次非線形性を
有する物質の会合体でもよい。また、本発明の非線形光
学材料の他の形態としては、1つの物質が旋光分散性能
と三次非線形性を併せ持つものが挙げられ、例えば、ポ
リマーの側鎖に旋光分散性能を有する物質及び三次非線
形性を有する物質を導入したものや、旋光分散性能を有
するポリマーの側鎖に三次非線形性を有する物質を導入
したもの、逆に、三次非線形性を有するポリマーの側鎖
に旋光分散性能を有する物質を導入したものが挙げられ
る。もちろん、三次非線形性を有する物質自体が旋光分
散性能をもつものでもよく、この場合の三次非線形性と
旋光分散性能の起源は同一でも別々に存在してもよい。
さらに、本発明の非線形光学材料の他の形態としては、
旋光分散性能を有する物質を含有する層と三次非線形性
を有する物質を含有する層を交互に複数層積層したもの
でもよい。
The form of the nonlinear optical material of the present invention is as follows:
A substance doped with a substance having optical rotation dispersion property and a substance having third-order nonlinearity, a substance having a substance having optical rotation dispersion performance doped in a polymer having third-order nonlinearity, and conversely a substance having third-order nonlinearity And a polymer having optical rotatory dispersion performance.
Alternatively, it may be an aggregate of a substance having optical rotation dispersion performance and a substance having third-order nonlinearity. Another form of the nonlinear optical material of the present invention is one in which one substance has both optical rotatory dispersion performance and third-order nonlinearity. For example, a substance having optical rotatory dispersion performance in the side chain of a polymer and third-order nonlinearity. Introducing a substance having a compound having a third order non-linearity, or a substance having a third order nonlinearity in the side chain of a polymer having optical rotation dispersion performance, conversely, The ones introduced are listed. Of course, the substance itself having the third-order nonlinearity may have the optical rotation dispersion performance, and the origins of the third-order nonlinearity and the optical rotation dispersion performance in this case may be the same or different.
Furthermore, as another form of the nonlinear optical material of the present invention,
A plurality of layers including a layer containing a substance having optical rotation dispersion performance and a layer containing a substance having third-order nonlinearity may be alternately laminated.

【0006】旋光分散性能を有する物質としては、物質
自体が旋光分散性能を有するキラル化合物や、結晶化に
より旋光分散性能を示す物質、あるいは、外部の電場、
磁場、あるいは基板のラビング等により旋光分散性能を
示す物質などが挙げられる。例えば、アミノ酸、ポリペ
プチド、酒石酸、ヘリセン、水晶、コレステリック液
晶、ネマチック液晶等が挙げられる。また、三次非線形
性を有する物質としては、大きな非局在化π電子系を有
するものが挙げられ、例えば、DANSE(4−ジメチ
ルアミノ−4’−ニトロスチルベン)、テトラキス
(2,4−キシリル)ブタトリエン、9,10−ビス
(3,3−ジフェニル−3−ヒドロキシプロピニル)ア
ントラセン、2−(4−ニトロフェニル)−4,5−ジ
フェニルイミダゾール、2−(4−ニトロフェニル)−
4,5−ビス(4−メトキシフェニル)イミダゾール、
テトラチオテトラセン、3,6−ビス(4,5−ジフェ
ニル−2H−イミダゾール−2−イリデン)−1,4−
シクロヘキサジエン、2−(チオピラン−4−イリデ
ン)−1,3−ジチオール、1,1,6,6−テトラフ
ェニル−ヘキサ−1,5−ジエン−3イン、3,3’−
ジエチルオキサカルボシアニン、3,3’−ジエチルオ
キサジカルボシアニンが挙げられ、また励起子の効果に
よるCuCl、CdSe、ZnSe等が挙げられる。
Examples of the substance having the optical rotatory dispersion property include a chiral compound having the optical rotatory dispersion property, a substance exhibiting the optical rotatory dispersion property by crystallization, or an external electric field.
Examples thereof include substances exhibiting optical rotation dispersion performance due to a magnetic field or rubbing of a substrate. Examples thereof include amino acids, polypeptides, tartaric acid, helicene, crystals, cholesteric liquid crystals, nematic liquid crystals and the like. Examples of the substance having third-order nonlinearity include those having a large delocalized π-electron system, and examples thereof include DANSE (4-dimethylamino-4′-nitrostilbene) and tetrakis (2,4-xylyl). Butatriene, 9,10-bis (3,3-diphenyl-3-hydroxypropynyl) anthracene, 2- (4-nitrophenyl) -4,5-diphenylimidazole, 2- (4-nitrophenyl)-
4,5-bis (4-methoxyphenyl) imidazole,
Tetrathiotetracene, 3,6-bis (4,5-diphenyl-2H-imidazol-2-ylidene) -1,4-
Cyclohexadiene, 2- (thiopyran-4-ylidene) -1,3-dithiol, 1,1,6,6-tetraphenyl-hexa-1,5-diene-3yne, 3,3'-
Examples thereof include diethyloxacarbocyanine and 3,3′-diethyloxadicarbocyanine, and CuCl, CdSe, ZnSe and the like due to the effect of excitons.

【0007】本発明においては、非線形光学素子に入射
する参照光の偏光状態を参照光の波長と異なる波長の光
で制御する。即ち、同一偏光面で入射した波長の異なる
参照光と制御光は、非線形材料の持つ旋光分散により、
材料内部で参照光と制御光の偏光面間に角度を生じるの
で、制御光によって参照光の偏光変化を引き起こすこと
ができる。したがって、簡単な偏光子の構成で光−光制
御素子を得ることができる。さらに、参照光に対する旋
光角が90°+n×180°(nは整数)となるように
光路長や濃度を設定することにより、全て同一方位の偏
光子だけで、光−光スイッチング素子を構成することが
できる。
In the present invention, the polarization state of the reference light incident on the nonlinear optical element is controlled by the light having a wavelength different from the wavelength of the reference light. That is, the reference light and the control light having different wavelengths incident on the same plane of polarization are rotatively dispersed by the nonlinear material.
Since an angle is generated between the polarization planes of the reference light and the control light inside the material, the control light can cause the polarization change of the reference light. Therefore, the light-light control element can be obtained with a simple polarizer configuration. Further, by setting the optical path length and the concentration so that the optical rotation angle with respect to the reference light is 90 ° + n × 180 ° (n is an integer), the optical-optical switching element is configured only by the polarizers in the same direction. be able to.

【0008】[0008]

【実施例】以下に、実施例を示して本発明を具体的に説
明する。 実施例1 図2は、本発明の非線形光学素子を用いた光−光スイッ
チング装置の概略図である。21は非線形光学材料であ
り、ポリ−L−グルタミン酸とDANSEをジクロロエ
タンに溶解し、キャスト後、溶媒を除去して得られたフ
ィルムである。24及び25は方位を垂直方向に設定し
た偏光子であり、24は偏光子として、25は検光子と
して働く。非線形光学材料21は、波長λ1 の参照光2
2を偏光子24により垂直方向の直線偏光として透過さ
せると、偏光面が90°回転するように光路長を設定し
ている。したがって、制御光が入射されていない時、偏
光面が90°回転して水平方向となった参照光は、方位
が垂直方向の検光子25により遮断される。
EXAMPLES The present invention will be specifically described below with reference to examples. Example 1 FIG. 2 is a schematic diagram of an optical-optical switching device using the nonlinear optical element of the present invention. Reference numeral 21 denotes a non-linear optical material, which is a film obtained by dissolving poly-L-glutamic acid and DANSE in dichloroethane, casting, and removing the solvent. Reference numerals 24 and 25 denote polarizers whose azimuths are set in the vertical direction, where 24 serves as a polarizer and 25 serves as an analyzer. The nonlinear optical material 21 uses the reference light 2 having the wavelength λ 1 .
The optical path length is set so that the plane of polarization is rotated by 90 ° when 2 is transmitted as vertical linearly polarized light by the polarizer 24. Therefore, when the control light is not incident, the reference light whose polarization plane is rotated by 90 ° and becomes horizontal is blocked by the analyzer 25 whose azimuth is vertical.

【0009】一方、波長λ2 の制御光23を偏光子24
により垂直方向の直線偏光として、非線形光学材料21
に入射させると、制御光は強い光であるため非線形光学
材料21に非線形光学効果を引き起こす。この時、制御
光と参照光は波長が異なるため、旋光分散により偏光面
の回転角度が異なっている。即ち、参照光の偏光面が制
御光の偏光面に対して傾いた状態で、非線形光学効果が
誘起されるので、その結果、参照光は楕円偏光となる。
そのため、参照光に垂直成分が生じ、これが検光子25
を透過する。以上のように、本発明によれば、参照光と
制御光が同一の偏光面であっても、参照光と制御光の波
長を変えて非線形光学材料に入射させることにより、旋
光分散性能と三次非線形性を利用して光−光スイッチン
グ装置を実現できる。 実施例2 非線形光学材料として(+)−ヘキサヘリセンの4%C
2溶液を用い、図2と同様の装置において、440n
mの参照光と535nmの制御光を同一偏光面で入射さ
せ、制御光の強度と検出光の強度の関係を調べた。その
結果は図3に示すように、制御光の強度の2乗に比例し
た検出光が得られ、カーシャッターが動作していること
が確認された。
On the other hand, the control light 23 having the wavelength λ 2 is supplied to the polarizer 24.
As a linearly polarized light in the vertical direction, the nonlinear optical material 21
When the light is incident on, the control light is a strong light and causes a nonlinear optical effect in the nonlinear optical material 21. At this time, since the control light and the reference light have different wavelengths, the rotation angle of the polarization plane is different due to the optical rotation dispersion. That is, the nonlinear optical effect is induced in the state where the polarization plane of the reference light is inclined with respect to the polarization plane of the control light, and as a result, the reference light becomes elliptically polarized light.
Therefore, a vertical component is generated in the reference light, which is the analyzer 25.
Through. As described above, according to the present invention, even if the reference light and the control light have the same polarization plane, by changing the wavelengths of the reference light and the control light to enter the nonlinear optical material, the optical rotatory dispersion performance and the third order An optical-optical switching device can be realized by utilizing the non-linearity. Example 2 4% C of (+)-hexahelicene as a nonlinear optical material
In an apparatus similar to that of FIG. 2 using S 2 solution, 440n
The reference light of m and the control light of 535 nm were made incident on the same polarization plane, and the relationship between the intensity of the control light and the intensity of the detection light was investigated. As a result, as shown in FIG. 3, detection light proportional to the square of the intensity of the control light was obtained, and it was confirmed that the car shutter was operating.

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

【図1】図1は、従来の光−光スイッチング装置の概略
図である。
FIG. 1 is a schematic diagram of a conventional optical-optical switching device.

【図2】図2は、本発明の一実施例の光−光スイッチン
グ装置の概略図である。
FIG. 2 is a schematic diagram of an optical-optical switching device according to an embodiment of the present invention.

【図3】図3は、実施例2における制御光の強度と検出
光の強度の関係を示す図である。
FIG. 3 is a diagram showing a relationship between the intensity of control light and the intensity of detection light in the second embodiment.

【符号の説明】[Explanation of symbols]

11 非線形光学材料 12 参照光 13 制御光 14,16 偏光子 15 検光子 21 非線形光学材料 22 参照光 23 制御光 24 偏光子 25 検光子 11 Nonlinear Optical Material 12 Reference Light 13 Control Light 14, 16 Polarizer 15 Analyzer 21 Nonlinear Optical Material 22 Reference Light 23 Control Light 24 Polarizer 25 Analyzer

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 参照光の偏光状態を参照光の波長と異な
る波長の光で制御する非線形光学素子であって、非線形
光学材料が三次非線形性と旋光分散特性を有することを
特徴とする非線形光学素子。
1. A non-linear optical element for controlling the polarization state of reference light with light having a wavelength different from that of the reference light, wherein the non-linear optical material has third-order non-linearity and optical rotation dispersion characteristics. element.
JP03327893A 1992-03-03 1993-02-23 Nonlinear optical element Expired - Fee Related JP3214129B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP03327893A JP3214129B2 (en) 1992-03-03 1993-02-23 Nonlinear optical element

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP8029292 1992-03-03
JP4-80292 1992-03-03
JP03327893A JP3214129B2 (en) 1992-03-03 1993-02-23 Nonlinear optical element

Publications (2)

Publication Number Publication Date
JPH05307202A true JPH05307202A (en) 1993-11-19
JP3214129B2 JP3214129B2 (en) 2001-10-02

Family

ID=26371954

Family Applications (1)

Application Number Title Priority Date Filing Date
JP03327893A Expired - Fee Related JP3214129B2 (en) 1992-03-03 1993-02-23 Nonlinear optical element

Country Status (1)

Country Link
JP (1) JP3214129B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7835643B2 (en) 2005-01-17 2010-11-16 Fujitsu Limited Optical waveform measuring apparatus and optical waveform measuring method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7835643B2 (en) 2005-01-17 2010-11-16 Fujitsu Limited Optical waveform measuring apparatus and optical waveform measuring method

Also Published As

Publication number Publication date
JP3214129B2 (en) 2001-10-02

Similar Documents

Publication Publication Date Title
US5847790A (en) Liquid crystal devices using a linear electro-optic effect
Kolinsky New materials and their characterization for photonic device applications
Ono et al. Photorefractive Bragg diffraction in high-and low-molar-mass liquid crystal mixtures
Meijer et al. Second-harmonic generation in centrosymmetric crystals of chiral molecules
Zhang et al. Homogeneous photorefractive polymer/nematogen composite
JP2772582B2 (en) Optical modulator
KR100213178B1 (en) Optical alignment composition, alignment layer formed therefrom, liquid crystal device employing the alignment layer
JPH0135325B2 (en)
Hu et al. The crystal growth and nonlinear optical properties of K2Al2B2O7
JPH05307202A (en) Nonlinear optical element
Mircea et al. Tuning NLO susceptibility in functionalized DNA
Kawatsuki Photothermal response characteristics of host-guest liquid crystals
US4093344A (en) Infrared polarization rotator and optical switch
JP3214128B2 (en) Optical signal processing method
US3957347A (en) Selectively variable circularly dichroic filtering method
JP2780180B2 (en) Light modulation element
Utsumi et al. Electrically controlled second-harmonic generation in ferroelectric liquid crystal
JP3324231B2 (en) Optical operation element
Park et al. Nonlinear optical anisotropy associated with polar ordering in ferroelectric liquid crystals
JP3651917B2 (en) Optical angle modulation-intensity modulation conversion method
JP3365004B2 (en) Light angle modulation-intensity modulation conversion method
JP2988574B2 (en) Wavelength selection method for optical signal processor
JPH08274401A (en) Total optical signal processing device
JP3003819B2 (en) Nonlinear optical element and optical signal processing device
Nakayama et al. Second‐order nonlinearity of nonpoled polymeric thin films doped with pyrylium salts with blue window characteristics

Legal Events

Date Code Title Description
S111 Request for change of ownership or part of ownership

Free format text: JAPANESE INTERMEDIATE CODE: R313115

R360 Written notification for declining of transfer of rights

Free format text: JAPANESE INTERMEDIATE CODE: R360

S111 Request for change of ownership or part of ownership

Free format text: JAPANESE INTERMEDIATE CODE: R313115

R370 Written measure of declining of transfer procedure

Free format text: JAPANESE INTERMEDIATE CODE: R370

R350 Written notification of registration of transfer

Free format text: JAPANESE INTERMEDIATE CODE: R350

FPAY Renewal fee payment (prs date is renewal date of database)

Year of fee payment: 8

Free format text: PAYMENT UNTIL: 20090727

LAPS Cancellation because of no payment of annual fees