无机化学学报
無機化學學報
무궤화학학보
JOURNAL OF INORGANIC CHEMISTRY
2001年
2期
269-274
,共6页
陈鹏磊%王东军%王小兵%刘鸣华%甄珍%刘新厚%王文军%陆兴泽
陳鵬磊%王東軍%王小兵%劉鳴華%甄珍%劉新厚%王文軍%陸興澤
진붕뢰%왕동군%왕소병%류명화%견진%류신후%왕문군%륙흥택
对称萘酞菁%LB膜%二阶非线性%二次谐波
對稱萘酞菁%LB膜%二階非線性%二次諧波
대칭내태정%LB막%이계비선성%이차해파
用水平提拉法制备了四叔丁基萘酞菁锌的LB膜。利用表面压-面积曲线、紫外-可见吸收光谱、小角X-射线衍射等表征了LB膜的结构,结果表明该化合物可以形成较高质量的具有很好层状结构的多层LB膜,在膜中分子大环平面垂直于基片平面并且以分子平面并不完全重合的H-聚集体存在。采用透射SHG方法测量了相应LB膜的二阶非线性光学性质,结果显示在实验条件下该化合物LB膜的宏观二阶非线性系数以及分子超极化率分别为:X(2)=1.1~2.5×10-9esu,β=2.1~4.7×10-31esu。这一研究为开发二阶非线性光学材料提出了更宽广的领域。
用水平提拉法製備瞭四叔丁基萘酞菁鋅的LB膜。利用錶麵壓-麵積麯線、紫外-可見吸收光譜、小角X-射線衍射等錶徵瞭LB膜的結構,結果錶明該化閤物可以形成較高質量的具有很好層狀結構的多層LB膜,在膜中分子大環平麵垂直于基片平麵併且以分子平麵併不完全重閤的H-聚集體存在。採用透射SHG方法測量瞭相應LB膜的二階非線性光學性質,結果顯示在實驗條件下該化閤物LB膜的宏觀二階非線性繫數以及分子超極化率分彆為:X(2)=1.1~2.5×10-9esu,β=2.1~4.7×10-31esu。這一研究為開髮二階非線性光學材料提齣瞭更寬廣的領域。
용수평제랍법제비료사숙정기내태정자적LB막。이용표면압-면적곡선、자외-가견흡수광보、소각X-사선연사등표정료LB막적결구,결과표명해화합물가이형성교고질량적구유흔호층상결구적다층LB막,재막중분자대배평면수직우기편평면병차이분자평면병불완전중합적H-취집체존재。채용투사SHG방법측량료상응LB막적이계비선성광학성질,결과현시재실험조건하해화합물LB막적굉관이계비선성계수이급분자초겁화솔분별위:X(2)=1.1~2.5×10-9esu,β=2.1~4.7×10-31esu。저일연구위개발이계비선성광학재료제출료경관엄적영역。
Langmuir-Blodgett films of tetra-tert-butyl naphthalocyaninatozinc(ttb-Nc), which is a novel symmetrically substituted naphthalocyanine derivative, have been fabricated by horizontal lifting technique and their structures have been characterized by the π-A isotherm, electronic absorption spectra, small-angle X-ray diffraction, coupled with the information deduced from the second-order nonlinear optical properties of the compound in the LB films. It concludes that LB films with good layer structure have came into being with the ttb-Nc molecules arranged themselves with H-aggregation, which is different from the conventional type one due to the macrocyclic planes of the ttb-Nc molecules in the aggregations have an incomplete overlapped configuration. Namely, the angle between the axis of this column-like H-aggregation of the ttb-Nc molecules and the macrocyclic planes of the compound is not just 90°. A staggered process for the ttb-Nc molecules to take this form of H-aggregation has been found after its solution spread onto the subphase surface. Particularly,second harmonic generation (SHG) from the LB films has also been detected. The macroscopic second-order susceptibility (X(2)) as well as the molecular hyperpolarizability (β) of the LB films for the compound under the experimental condition were estimated to be X(2) = 1.1 ~ 2.5 × 10 -9esu and β=2.1~4.7×10-31esu, respectively. In spite of the moderate high values of these two data, the research work expands the investigation field for the SHG materials.