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新型不对称酞菁的电致发光性质研究
作者姓名:Xia DC  Li WC  Han S  Cheng CH  Li QQ  Wang J  Zhang W  Li Z
作者单位:1. 运城学院化学系,山西,运城,044000;东北师范大学化学学院,吉林,长春,130012
2. 吉林大学集成光电子国家重点实验室,电子科学与工程学院,吉林,长春,130012
3. 运城学院化学系,山西,运城,044000
4. 大连理工大学物理与光电工程学院,辽宁,大连,116023
基金项目:国家自然科学基金项目,山西省青年基金项目,运城学院院级重点项目,东北师范大学校内博士后基金项目 
摘    要:制作了以3种新璎不对称酞菁铜为发光层的电致发光器件并研究了其电致发光性质.3种新型不对称酞菁铜为2(3)-(对叔丁基苯氧基)酞菁铜(1),2(3),9(10),16(17)-三-(对叔丁基苯氧基)酞菁铜(2)和2(3),16(17)-二-(对叔丁基苯氧基)酞菁铜(3).其中以(1)和(3)为发光层的器件结构ITO/NPB(40 nm)/Phthalocynine(Pc)(30 nm)/AlQ(43.8 nm)/LiF(0.5 nm)/Al(120 nm).其中以(2)为发光层的器件结构为:ITO/NPB(30 nm)/Pc(30 nm)/BCP(20 nm)/AlQ(30 nm)/LiF(0.5 nm)/Al(120 nm).以(1),(2)和(3)为发光层与Q带栩关联的发射波长分别出现在869和1 062 nm;1 050和1110 nm;和1 095和1 204 nm.上述发射波长的不同是因为取代基的数目和真空镀膜的分子聚集态不同造成的,所以3种不对称酞菁铜的发射峰值和半峰宽差别较大,而且由此也引起斯托克司位移的不同.

关 键 词:新型  酞菁  电致发光  性质

Electroluminescence character of novel unsymmetry substituted phthalocyanines
Xia DC,Li WC,Han S,Cheng CH,Li QQ,Wang J,Zhang W,Li Z.Electroluminescence character of novel unsymmetry substituted phthalocyanines[J].Spectroscopy and Spectral Analysis,2010,30(9):2335-2339.
Authors:Xia Dao-cheng  Li Wan-cheng  Han Shuang  Cheng Chuan-hui  Li Quan-quan  Wang Jin  Zhang Wei  Li Zhu
Institution:College of Chemistry, Yuncheng University, Yuncheng 044000, China. xiadaocheng@yahoo.com.cn
Abstract:The authors for the first time fabricated OLEDs employing novel phthalocynines: 2(3)-(p-tert-butylphenoxy) copper phthalocyanine(1), 2(3),16(17)-di(p-tert-butyl-phenoxy) copper phthalocyanine(2) and 2(3), 9(10), 16(17)-tri (p-tert-butylphenoxy) copper phthalocyanine(3) as light emitting layer, and their electroluminescence character was studied. The final structures of three-layer OLEDs based on copper 2(3)-(p-tert-butylphenoxy) copper phthalocyanine (1) and 2(3), 9(10), 16(17)-tri (p-tert-butylphenoxy) copper phthalocyanine(3) were ITO/NPB(40 nm)/Pc(30 nm)/AlQ(43.5 nm)/LiF (0.5 nm)/Al(120 nm). The structure of three-layer OLED based on 2(3), 9(10), 16(17)-tri (p-tert-butylphenoxy) copper phthalocyanine (3) was ITO/NPB(30 nm)/Pc(30 nm) /BCP(20 nm)/A1Q(30 nm)/LiF (0. 5 nm)/Al(120 nm). Room-temperature electroluminescence was observed at about 869 nmand 1 062 nm for 2(3)-(p-tert-butylphenoxy) copper phthalocyanine(1); room-temperature electroluminescence of 2(3),16(17) -di(p-tert-butyl-phenoxy) copper phthalocyanine(2) was found at about 1050 nm and 1110 nm; and room-temperature electroluminescence of 2(3), 9(10), 16( 17)-tri (p-tert-butylphenoxy) copper phthalocyanine(3) was studied at about 1095 and 1204 nm. The emission wavelengths and the half bandwidths were quite different for the phthalocyanine, which may be due to the differences in the number of substituted and the molecular aggregations in vacuum sublimed films. The difference in Stokes shift relaxation was also induced by the molecular aggregations.
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