The electronic structure of pentacene revisited

被引:18
|
作者
Berkebile, S. [1 ]
Koller, G. [1 ]
Fleming, A. J. [1 ]
Puschnig, P. [2 ]
Ambrosch-Draxl, C. [2 ]
Emtsev, K. [3 ]
Seyller, T. [3 ]
Riley, J. [4 ]
Ramsey, M. G. [1 ]
机构
[1] Karl Franzens Univ Graz, Inst Phys, A-8010 Graz, Austria
[2] Univ Leoben, Chair Atomist Modelling & Design Mat, A-8700 Leoben, Austria
[3] Univ Erlangen Nurnberg, Lehrstuhl Tech Phys, D-91058 Erlangen, Germany
[4] La Trobe Univ, Dept Phys, Bundoora, Vic 3086, Australia
关键词
Pentacene; Photoemission; Band dispersion; Electronic structure; INTERMOLECULAR BAND DISPERSION; ORGANIC THIN-FILMS; CHARGE-TRANSPORT; CU(110); SPECTROSCOPY;
D O I
10.1016/j.elspec.2009.04.001
中图分类号
O433 [光谱学];
学科分类号
0703 ; 070302 ;
摘要
Recently, there have been reports of the valence band photoemission of pentacene films grown on various substrates with particular emphasis on the highest occupied molecular orbital (HOMO) and its dispersion. In various works, evidence for HOMO band dispersion as high as 0.5 eV, even for polycrystalline films, has been presented. In apparent contradiction to these results, we have previously reported a band dispersion of only 50 meV. measured on a well characterised film with a single polymorph and single crystalline orientation. 5A(0 2 2). Here, we first present the two-dimensional momentum distribution of the HOMO of a 5A(0 2 2) film. Then the development of the valence band spectra for films grown at room temperature and low temperature are compared, and we show that morphological aspects can lead to the apparent observation of high HOMO dispersion. Finally, with the aid of the two-dimensional momentum distribution of the HOMO, we show that a reasonably large dispersion (0.25 eV) does indeed exist in 5A(0 2 2). (C) 2009 Elsevier B.V. All rights reserved.
引用
收藏
页码:22 / 27
页数:6
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