Synchrotron radiation studies of the orientation of thin silicon phthalocyanine dichloride film on HOPG substrate

  • Thin silicon phthalocyanine dichloride films on HOPG were prepared and the
    sample was heated in the vacuum with laser. The thickness of the thin sample
    on HOPG was checked by X-ray photoemission spectroscopy. The orientation of
    the molecules in respect to the substrate plane was investigated by measuring the silicon K-edge near edge X-ray absorption fine structure (NEXAFS). In the NEXAFS spectra of the thin sample, two clear peaks which were assigned to 1s→σSi-N* and 1s→σSi-Cl* appeared around 1847.2 eV and 1843.1 eV respectively. The intensities of the resonance peaks showed strong polarization dependence. A quantitative analysis of the polarization dependence revealed that the Si-N bond tended to lie down while the Si-Cl bond was out of the molecular plane.

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  • [1] . Friend R H, Gymer R W, Holmes A B et al. Nature(London), 1999, 121: 3972. Dimitrakopoulos C, Malenfant P R L. Adv. Mater (Weinheim,Ger.), 2002, 99: 143. Forrest S R. Chem. Rev., 1996, 97: 17934. Biswas I, Peisert H, Schwieger T et al. J. Chem. Phys.,2005, 122: 0647105. Miao P, Robinson A W, Palmer R E. J. Phys. D, 1998, 31:L376. Michaelis W, Wohrle D, Schlettwein D. J. Mater. Res.,2004, 19: 20407. Ostrick J R, Dodabalapur A, Torsi L et al. J. Appl. Phys.,1997, 81: 68048. Peisert H, Schwiegerm T J, Auerhammerm et al. J. Appl.Phys., 2001, 90: 4669. Vearey-Poberts A R, Steiner H J, Evans S et al. Appl. Surf.Sci., 2004, 234: 13110. Evans D A, Steiner H J, Vearey-Roberts A R et al. Nucl.Instrum. Methods Phys. Res. B, 2003, 199: 47511. Sekiguchi T, Baba Y, Shimoyama I et al. J. Phys.: Condens.Matter, 2005, 17: 545312. Moulder J F, Stichle W F, Sobol P E, Bomben K D. Handbookof X-ray Photoelectron Spectroscopy. Physical ElectronicsInc., Eden Prairie, USA, 199513. Sco eld J H. Physics, 1973, 45: UC-3414. Tanuma S, Powell C J, Penn D R. Surf. Interface Anal.,1994, 21: 16515. Stohr J. in: NEXAFS Spectroscopy. Ed. by G. Ertl, R.Gomer, D.L. Mills, H.K.V. Lotsch. Berlin: Springer-VerlagPress, 1992. 71, 27616. Boo B H, LIU Z Y, Koyano I. J. Phys. Chem. A, 2000, 104:147417. DENG J Z, Baba Y, Sekiguchi T, Hirao N, Honda M J.Phys.:Condens. Matter, 2007, 19: 1118. Outka D A, Stohr J. J. Chem. Phys., 1988, 88: 353919. Kitamura H. Synchrotron Radiation Calculation Programfor PC98, Version 2.3. 1993
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DENG Ju-Zhi, CHEN Rong, SEKIGUCHI Tetsuhiro, BABA Yuji, HIRAO Norie and HONDA Mitsunori. Synchrotron radiation studies of the orientation of thin silicon phthalocyanine dichloride film on HOPG substrate[J]. Chinese Physics C, 2008, 32(9): 769-772. doi: 10.1088/1674-1137/32/9/018
DENG Ju-Zhi, CHEN Rong, SEKIGUCHI Tetsuhiro, BABA Yuji, HIRAO Norie and HONDA Mitsunori. Synchrotron radiation studies of the orientation of thin silicon phthalocyanine dichloride film on HOPG substrate[J]. Chinese Physics C, 2008, 32(9): 769-772.  doi: 10.1088/1674-1137/32/9/018 shu
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Received: 2007-10-15
Revised: 2008-01-03
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Synchrotron radiation studies of the orientation of thin silicon phthalocyanine dichloride film on HOPG substrate

    Corresponding author: DENG Ju-Zhi,

Abstract: 

Thin silicon phthalocyanine dichloride films on HOPG were prepared and the
sample was heated in the vacuum with laser. The thickness of the thin sample
on HOPG was checked by X-ray photoemission spectroscopy. The orientation of
the molecules in respect to the substrate plane was investigated by measuring the silicon K-edge near edge X-ray absorption fine structure (NEXAFS). In the NEXAFS spectra of the thin sample, two clear peaks which were assigned to 1s→σSi-N* and 1s→σSi-Cl* appeared around 1847.2 eV and 1843.1 eV respectively. The intensities of the resonance peaks showed strong polarization dependence. A quantitative analysis of the polarization dependence revealed that the Si-N bond tended to lie down while the Si-Cl bond was out of the molecular plane.

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