JPH03211535A - Organic nonlinear optical material - Google Patents

Organic nonlinear optical material

Info

Publication number
JPH03211535A
JPH03211535A JP776390A JP776390A JPH03211535A JP H03211535 A JPH03211535 A JP H03211535A JP 776390 A JP776390 A JP 776390A JP 776390 A JP776390 A JP 776390A JP H03211535 A JPH03211535 A JP H03211535A
Authority
JP
Japan
Prior art keywords
optical nonlinearity
optical
nonlinear optical
semiconductor laser
wavelength side
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.)
Pending
Application number
JP776390A
Other languages
Japanese (ja)
Inventor
Tetsuya Tsunekawa
哲也 恒川
Tetsuya Goto
哲哉 後藤
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
Original Assignee
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 Toray Industries Inc filed Critical Toray Industries Inc
Priority to JP776390A priority Critical patent/JPH03211535A/en
Publication of JPH03211535A publication Critical patent/JPH03211535A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain high optical nonlinearity, UV and visible ray absorption at a shorter wavelength side and high crystallinity by using a methyl-4- hydroxybenzoate crystal. CONSTITUTION:A methyl-4-hydroxybenzoate crystal has superior optical nonlinearity and crystallinity and the UV and visible ray absorption is at a shorter wavelength side than the second harmonic region of semiconductor laser light (lambda=0.83-0.9mum). Since the UV and visible ray absorption is at the shorter wavelength side, when the wavelength of the semiconductor laser light is transformed, the deterioration of the compd. and the lowering of the efficiency of transformation due to the reabsorption of second harmonics are not caused. High optical nonlinearity, high crystallinity and UV and visible ray absorption at a shorter wavelength side can be obtd.

Description

【発明の詳細な説明】 [産業上の利用分野コ 本発明は、光情報処理や光通信などで好適に用いられる
有機非線形光学材料に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an organic nonlinear optical material suitably used in optical information processing, optical communication, and the like.

[従来の技術] オプトエレクトロニクス分野の新素子として、非線形光
学素子の実現を目指した材料探索研究が数多くなされて
おり、近年、π電子共役系を有する有機化合物は、分子
自体の性能の大きさおよび高速の光応答性から注目され
ている。
[Prior Art] Many materials exploration studies have been conducted with the aim of realizing nonlinear optical elements as new elements in the field of optoelectronics.In recent years, organic compounds with π-electron conjugated systems have been It is attracting attention because of its fast photoresponsiveness.

特に、2次の光非線形性を有する材料については、種々
の化合物系で検討されており、また総説的な解説も数多
くある。(1) A CS  symposiumse
ries 233(1983)、 2)D、J、Wil
liams Angew、CbemInf、 Ed、 
Engl、 23 p690  (1984)、 3)
D、 S、 Chemlg  andJ、2yss、’
Non1inear optical propert
iea of organic molecules 
 and  crystals’  vol  1,2
 ^cademicpress (1987) など。
In particular, materials with second-order optical nonlinearity have been studied using various compound systems, and there are many general explanations. (1) A CS symposium
ries 233 (1983), 2) D. J. Wil.
liams Angew, CbemInf, Ed.
Engl., 23 p690 (1984), 3)
D, S, Chemlg and J, 2yss,'
Non1inear optical property
iea of organic molecules
and crystals' vol 1, 2
^cademicpress (1987) etc.

) π電子共役系を有する有機化合物の光非線形性は、レー
ザ光入射時のπ電子のゆらぎに起因するものとされてお
り、このゆらぎを大きくするため、π電子共役系にドナ
ー性、アクセプター性の置換基を導入することが従来の
分子設計指針であった。
) The optical nonlinearity of organic compounds with a π-electron conjugated system is said to be caused by the fluctuation of π-electrons when laser light is incident, and in order to increase this fluctuation, donor and acceptor properties are added to the π-electron conjugated system. The conventional molecular design guideline was to introduce substituents.

しかし、上記分子設計指針による化合物、すなわち、π
電子共役系にドナー性、アクセプター性の置換基を導入
した化合物は、分子間で強く双極子−双極子相互作用す
るため、多くの場合、2分子の双極子が打ち消し合う構
造である中心対称性の結晶を形成し、2次の光非線形性
を発現しない。
However, the compound according to the above molecular design guideline, i.e., π
Compounds in which donor and acceptor substituents are introduced into an electronically conjugated system have strong dipole-dipole interactions between molecules, so in many cases they have a central symmetry structure in which the dipoles of the two molecules cancel each other out. crystal, and does not exhibit second-order optical nonlinearity.

従来の研究では、結晶の中心対称性を崩し2次の光非線
形性を発現させるために、光学活性な置換基や水素結合
形成性の置換基をπ電子共役系に導入するという試みが
なされて来た。
In previous research, attempts have been made to introduce optically active substituents or hydrogen bond-forming substituents into the π-electron conjugated system in order to break the central symmetry of the crystal and develop second-order optical nonlinearity. It's here.

膨大な数の有機化合物について検討され、2−メチル−
4−ニトロアニリン(MNA) 、N、Nジメチル−2
−アセチルアミノ−4−ニトロアニリン(I)AN)、
N−(4−ニトロフェニル)−(L)−プロリノール(
NPP)などのベンゼン誘導体がNd:YAGレーザ波
長(λ=1.06μm)で比較的大きな光非線形性を発
現することが見い出された。
A huge number of organic compounds have been studied, and 2-methyl-
4-Nitroaniline (MNA), N,N dimethyl-2
-acetylamino-4-nitroaniline (I)AN),
N-(4-nitrophenyl)-(L)-prolinol (
It has been found that benzene derivatives such as NPP) exhibit relatively large optical nonlinearity at the Nd:YAG laser wavelength (λ = 1.06 μm).

しかし、これらのベンゼン誘導体はアミノ基とニトロ基
の様に強いドナー性基と強いアクセプター性基を有して
いるためNd : YAGレーザ波長での光非線形性は
比較的大きいが、紫外可視吸収が長波長まである。従っ
て、半導体レーザ光(λ・0.83〜0.9μm)を透
過型、すなわち基本波(半導体レーザ光)が材料中を伝
搬し、第二高調波も少なくとも材料を一部透過する構成
で波長変換する場合には、これらの化合物自身が第二高
調波を再吸収するため化合物劣化や変換効率の低下等の
問題が生じた。
However, since these benzene derivatives have strong donor groups and strong acceptor groups such as amino groups and nitro groups, their optical nonlinearity at the Nd:YAG laser wavelength is relatively large, but their ultraviolet-visible absorption is There are even long wavelengths. Therefore, the semiconductor laser light (λ 0.83 to 0.9 μm) is transmitted through the material, that is, the fundamental wave (semiconductor laser light) propagates through the material, and the second harmonic also transmits at least a portion of the material. When converting, these compounds themselves reabsorb the second harmonics, resulting in problems such as compound deterioration and reduction in conversion efficiency.

紫外可視吸収の短波長化を考慮し、分子設計されている
例としては、2−メチル−4−ニトロピリジン−N−オ
キシド(POM) 、N−[2(5−ニトロピリジル)
] −(L)−プロリノル(PNP) 、N−[4−ニ
トロフェニル]−2−エチルイミダゾール(NPEI)
、4−ヒドロキシ−3−メトキシベンズアルデヒド(V
AN)などが挙げられる。しかし、POM、NPEI、
PNPは短波長化が不十分であるため光非線形性が小さ
く、またVANは昇華性が高いため保存安定性に欠ける
という問題を有している。
Examples of molecules whose molecules have been designed with short wavelengths of UV-visible absorption in mind include 2-methyl-4-nitropyridine-N-oxide (POM) and N-[2(5-nitropyridyl).
] -(L)-prolinol (PNP), N-[4-nitrophenyl]-2-ethylimidazole (NPEI)
, 4-hydroxy-3-methoxybenzaldehyde (V
AN), etc. However, POM, NPEI,
PNP has a problem that optical nonlinearity is small because the wavelength is insufficiently shortened, and VAN lacks storage stability because it has high sublimation property.

以上の様に、材料探索は手広くなされており、Nd:Y
AGレーザを基本波とした場合には比較的大きな光非線
形性を発現する材料が見い出されているが、半導体レー
ザ(λ・0.83〜069μm)ヲ基本波とした場合で
も適用できる有望な材料は未だ見い出されていない状況
にある。
As mentioned above, material searches have been carried out extensively, and Nd:Y
Materials that exhibit relatively large optical nonlinearity have been found when the fundamental wave is an AG laser, but there are promising materials that can be applied even when the fundamental wave is a semiconductor laser (λ 0.83 to 069 μm). has not yet been discovered.

[発明が解決しようとする課題] 本発明の課題は、透過型の半導体レーザ波長変換素子を
作製するための、■大きな光非線形性、■短波長側の紫
外可視吸収、および■高い結晶性を有する有機非線形光
学材料を提供することにある。
[Problems to be Solved by the Invention] The problems of the present invention are to achieve ■large optical nonlinearity, ■ultraviolet-visible absorption on the short wavelength side, and ■high crystallinity in order to produce a transmission type semiconductor laser wavelength conversion element. An object of the present invention is to provide an organic nonlinear optical material having the following properties.

[課題を解決するための手段] 上記目的を達成するため、本発明は、下記の構成を有す
る。
[Means for Solving the Problems] In order to achieve the above object, the present invention has the following configuration.

「メチル−4−ヒドロキシベンゾエートの結晶からなる
ことを特徴とする有機非線形光学材料。」すなわち、本
発明の要点は、メチル−4−ヒドロキシベンゾエート(
以下、MPHBと略す)結晶が、■光非線形性、■結晶
性、の点で優れており、しかも■紫外可視吸収は半導体
レーザ光(λ・0.83〜0.9μm)の第二高調波領
域より短波長側となることを見い出した点にある。紫外
可視吸収が半導体レーザ光の第二高調波領域より短波長
側にあるため、半導体レーザ光を波長変換する場合、第
二高調波の再吸収による化合物劣化や変換効率の低下な
どの問題を起こさない。
"An organic nonlinear optical material characterized by comprising crystals of methyl-4-hydroxybenzoate." That is, the gist of the present invention is that methyl-4-hydroxybenzoate (
The crystal (hereinafter abbreviated as MPHB) is excellent in terms of ■optical nonlinearity and ■crystallinity, and ■ultraviolet-visible absorption is the second harmonic of semiconductor laser light (λ 0.83 to 0.9 μm). The point is that it was discovered that the wavelength is shorter than the wavelength range. Since UV-visible absorption is on the shorter wavelength side than the second harmonic region of semiconductor laser light, when converting the wavelength of semiconductor laser light, problems such as compound deterioration and reduction in conversion efficiency due to reabsorption of the second harmonic do not occur. do not have.

本発明のM P HBを重水素化した場合、近赤外吸収
のシフト効果などがあるが、重水素化していない化合物
と同様の紫外可視吸収と非線形光学効果を有する。従っ
て、上記非線形光学化合物は、その一部または全ての水
素が重水素置換されていてもよい。
When the M P HB of the present invention is deuterated, there is a near-infrared absorption shift effect, but it has the same ultraviolet-visible absorption and nonlinear optical effect as a non-deuterated compound. Therefore, in the nonlinear optical compound, some or all of the hydrogens may be replaced with deuterium.

本発明化合物の結晶化の方法は、特に限定されるもので
はなく、溶液法、溶融法、気相法など従来公知の方法を
用いて、容易に良質のMP)(B単結晶を得ることがで
きる。
The method of crystallizing the compound of the present invention is not particularly limited, and it is possible to easily obtain a high-quality MP (B) single crystal using conventionally known methods such as a solution method, a melt method, and a gas phase method. can.

上記の様に、MPHB結晶は、波長変換素子を作製する
上で極めて有用な材料である。結晶性、加工性に優れて
いるため、平面導波路型、ファイバー型等、種々の形態
を有した波長変換素子の作製に有用である。
As mentioned above, MPHB crystal is an extremely useful material for producing wavelength conversion elements. Since it has excellent crystallinity and processability, it is useful for producing wavelength conversion elements having various forms such as planar waveguide type and fiber type.

[実施例コ 実施例I MPHBの光非線形性、紫外可視吸収、結晶性。[Example code] Example I Optical nonlinearity, UV-visible absorption, and crystallinity of MPHB.

まず市販(東京化成、特級)のM P HBをベンゼン
/クロロホルム(体積比 1/1)で2度再結晶した(
融点 127〜128℃)。
First, commercially available (Tokyo Kasei, special grade) M P HB was recrystallized twice with benzene/chloroform (volume ratio 1/1).
Melting point 127-128°C).

ここで得た白色の結晶をさらに窒素雰囲気下、スローエ
バポレーション法により結晶化させるとメチルエチルケ
トン溶液から透明性の良い大型角状品(5mmx 7 
mmx 3 mm)か得られた。結晶化溶媒を醋酸エチ
ル、エタノールとしても同様に透明性の良い大型角状品
が得られ、本発明のM P HBは極めて結晶性に優れ
ていることがわかった。
The white crystals obtained here are further crystallized by slow evaporation in a nitrogen atmosphere, resulting in a large square crystal with good transparency (5 mm x 7 mm) from a methyl ethyl ketone solution.
mm x 3 mm) was obtained. Even when ethyl acetate or ethanol was used as the crystallization solvent, large angular products with good transparency were similarly obtained, and it was found that the M P HB of the present invention has extremely excellent crystallinity.

次に、化合物の光非線形性を調へるためにS HG(第
2高調波発生)を粉末法(S、 K、 Kurlx、 
T、 T。
Next, in order to investigate the optical nonlinearity of the compound, SHG (second harmonic generation) was performed using a powder method (S, K, Kurlx,
T, T.

Pet+y、J、Appl、Phys 393798 
(1966))により測定した。ここで用いたレーザ光
源は、Nd:YAGレーザの第2高調波励起の色素レー
ザ(波長0゜83f1m)で、また試料はメチルエチル
ケトン溶液から得た角状結晶を乳鉢により10μm以下
に粉砕したものを使用した。
Pet+y, J, Appl, Phys 393798
(1966)). The laser light source used here was a dye laser (wavelength: 0°83f1m) with second harmonic excitation of an Nd:YAG laser, and the sample was a square crystal obtained from a methyl ethyl ketone solution that was crushed to 10 μm or less in a mortar. used.

紫外可視吸収スペクトルの測定は、拡散反射法により行
った。測定用サンプルは、臭化カリウム/MPHBを重
量比10/1で混合し、ディスク成型することにより作
製した。
The measurement of the ultraviolet-visible absorption spectrum was performed by the diffuse reflection method. A sample for measurement was prepared by mixing potassium bromide/MPHB at a weight ratio of 10/1 and molding the mixture into a disk.

S T−I Gおよび紫外可視吸収の吸収端の測定結果
を表1に示す。
Table 1 shows the measurement results of S T-I G and the absorption edge of ultraviolet-visible absorption.

本発明によるM P )(Bは標準的な非線形光学化合
物であるウレアの3倍の光非線形性を有し、しかも吸収
端が半導体レーザの第2高調波波長より短波長側にあり
、従って半導体レーザの透過型波長変換素子用材料とし
て好適であることがわかった。
M P ) (B according to the present invention) has an optical nonlinearity three times that of urea, which is a standard nonlinear optical compound, and has an absorption edge on the shorter wavelength side than the second harmonic wavelength of a semiconductor laser. It was found that this material is suitable as a material for a transmission type wavelength conversion element of a laser.

比較例1 3−メチル−4−ニトロピリジン−N−オキシド(PO
M)の光非線形性と紫外可視吸収。
Comparative Example 1 3-Methyl-4-nitropyridine-N-oxide (PO
M) Optical nonlinearity and UV-visible absorption.

市販品(ランカスター社)をアセトン/ベンゼン(体積
比 1/1)で再結晶すると、薄黄色の角状結晶が得ら
れた。
When a commercial product (Lancaster) was recrystallized with acetone/benzene (volume ratio 1/1), pale yellow angular crystals were obtained.

次に、化合物の光非線形性と紫外可視吸収スペクトルの
測定を実施例1と同様の方法により行った。
Next, the optical nonlinearity and ultraviolet-visible absorption spectrum of the compound were measured in the same manner as in Example 1.

S HGおよび紫外可視吸収の吸収端の測定結果を表1
に示す。
Table 1 shows the measurement results of the absorption edges of SHG and UV-visible absorption.
Shown below.

P OMは標準的な非線形光学化合物であるウレアの1
.1倍の光非線形性しか示さなかった。また、吸収端の
測定結果より、POMは第2高調波領域に紫外可視吸収
を有しているため半導体レーザの透過型波長変換素子用
材料として好ましくないことか明らかとなった。
P OM is one of the standard nonlinear optical compounds, urea.
.. It showed only 1x optical nonlinearity. In addition, the absorption edge measurement results revealed that POM is not preferable as a material for a transmission type wavelength conversion element of a semiconductor laser because it has ultraviolet-visible absorption in the second harmonic region.

比較例2 N−[2−(5−ニトロピリジル)コー(I、)プロリ
ノール(PNP)の光非線形性、紫外可視吸収、結晶性
Comparative Example 2 Optical nonlinearity, ultraviolet-visible absorption, and crystallinity of N-[2-(5-nitropyridyl)co(I,)prolinol (PNP).

1) N Pは、文献記載(R1,Twieg et 
al、、J、 Chem、  Phys、、 85(6
)、 3537(1986))の方法により合成し t
こ。
1) NP is as described in the literature (R1, Twieg et al.
al., J. Chem, Phys., 85(6
), 3537 (1986)).
child.

得られた粗結晶は、ベンゼンにより2度再結晶した。The obtained crude crystals were recrystallized twice from benzene.

PNPは、クロロホルム/シクロヘキサン(体積比 1
:1)の混合溶媒により再結晶すると、比較的透明性の
良い、薄黄色の角状晶(5mmx4mmx 4 mm)
となった。しかし、この結晶は数日間室温に放置してお
くと失透した。
PNPs were prepared using chloroform/cyclohexane (volume ratio 1
: When recrystallized with a mixed solvent of 1), pale yellow angular crystals (5 mm x 4 mm x 4 mm) with relatively good transparency are obtained.
It became. However, this crystal devitrified when left at room temperature for several days.

次に、化合物の光非線形性と紫外可視吸収スペクトルの
測定を実施例1の方法により行った。
Next, the optical nonlinearity and ultraviolet-visible absorption spectrum of the compound were measured by the method of Example 1.

S TI Gおよび紫外可視吸収の吸収端の測定結果を
表1に示す。
Table 1 shows the measurement results of STI G and the absorption edge of ultraviolet-visible absorption.

PNPは標準的な非線形光学化合物であるウレアの0.
2倍の光非線形性しか示さなかった。また、吸収端の測
定結果より、PNPは第2高調波領域に紫外可視吸収を
有しているため半導体レーザの透過型波長変換素子用材
料として好ましくないことか明らかとなった。
PNP is a standard nonlinear optical compound, 0.0.
It showed only twice as much optical nonlinearity. Furthermore, the absorption edge measurement results revealed that PNP is not preferable as a material for a transmission type wavelength conversion element of a semiconductor laser because it has ultraviolet-visible absorption in the second harmonic region.

表1.有機非線形光学化合物のSHGとUVcuiof
f  (λ:0.83μm) [発明の効果コ 大きな光非線形性、高結晶性および短波長側の紫外可視
吸収を有し、半導体レーザの波長変換を透過型で可能と
する高性能の有機非線形光学材料を提供できる。
Table 1. Organic nonlinear optical compounds SHG and UV cuiof
f (λ: 0.83 μm) [Effects of the invention] High-performance organic nonlinearity that has large optical nonlinearity, high crystallinity, and ultraviolet-visible absorption on the short wavelength side, and enables wavelength conversion of semiconductor lasers in a transmission type. We can provide optical materials.

Claims (1)

【特許請求の範囲】[Claims] (1)メチル−4−ヒドロキシベンゾエートの結晶から
なることを特徴とする有機非線形光学材料。
(1) An organic nonlinear optical material comprising crystals of methyl-4-hydroxybenzoate.
JP776390A 1990-01-16 1990-01-16 Organic nonlinear optical material Pending JPH03211535A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP776390A JPH03211535A (en) 1990-01-16 1990-01-16 Organic nonlinear optical material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP776390A JPH03211535A (en) 1990-01-16 1990-01-16 Organic nonlinear optical material

Publications (1)

Publication Number Publication Date
JPH03211535A true JPH03211535A (en) 1991-09-17

Family

ID=11674729

Family Applications (1)

Application Number Title Priority Date Filing Date
JP776390A Pending JPH03211535A (en) 1990-01-16 1990-01-16 Organic nonlinear optical material

Country Status (1)

Country Link
JP (1) JPH03211535A (en)

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