The electronic structure of C60/ZnPc interface for organic photovoltaic device with blended layer architecture

被引:59
作者
Park, S. H. [1 ]
Jeong, J. G. [1 ]
Kim, Hyo-Jin [1 ]
Park, Seung-Han [1 ]
Cho, Mann-Ho [1 ]
Cho, Sang Wan [2 ]
Yi, Yeonjin [3 ]
Heo, Min Young [4 ]
Sohn, Hyunchul [4 ]
机构
[1] Yonsei Univ, Inst Phys & Appl Phys, Seoul 120749, South Korea
[2] Boston Univ, Dept Phys, Boston, MA 02215 USA
[3] KRISS, Div Ind Metrol, Taejon 305340, South Korea
[4] Yonsei Univ, Dept Ceram Engn, Seoul 120749, South Korea
关键词
charge exchange; electronic structure; fullerenes; interface states; multilayers; organic compounds; photoconductivity; photoelectric devices; ultraviolet photoelectron spectra; zinc compounds; PLASTIC SOLAR-CELLS; PHOTOELECTRON-SPECTROSCOPY; C-60;
D O I
10.1063/1.3285174
中图分类号
O59 [应用物理学];
学科分类号
摘要
The interfacial electronic structures of fullerene (C-60)/zinc-phthalocyanine (ZnPc) and C-60/ZnPc:C-60 (50 wt %) containing a blended layer were investigated by in situ ultraviolet photoelectron spectroscopy (UPS), in an attempt to understand the role of the blended layer in improving the performance of organic photovoltaic devices that contain such layers. From the UPS spectra, the band bending found to be 0.30 eV in the ZnPc layer and 0.43 eV in the C-60 layer at the C-60/ZnPc interface. On the other hand, the band bending was 0.25 eV in both of the organic layers at the ZnPc:C-60/ZnPc interface and no significant band bending in the C-60 layer at the C-60/ZnPc:C-60 interface was found. The observed interface dipole was 0.06 eV at the C-60/ZnPc interface and 0.26 eV at the ZnPc:C-60/ZnPc interface. The offset between the highest unoccupied molecular orbital of ZnPc and the lowest occupied molecular orbital of C-60 was 0.75 eV at C-60/ZnPc and was 1.04 eV at the ZnPc:C-60/ZnPc interface. The increased offset can be attributed to an increase in the interface dipole, caused by the blending donor and acceptor material. The blending facilitates charge transfer between the donor and acceptor, resulting in an increase in the interface dipole, resulting in a larger offset.
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页数:3
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共 21 条
  • [1] Hybrid polymer-metal oxide thin films for photovoltaic applications
    Boucle, Johann
    Ravirajan, Punniamoorthy
    Nelson, Jenny
    [J]. JOURNAL OF MATERIALS CHEMISTRY, 2007, 17 (30) : 3141 - 3153
  • [2] Brabec CJ, 2001, ADV FUNCT MATER, V11, P15, DOI 10.1002/1616-3028(200102)11:1<15::AID-ADFM15>3.0.CO
  • [3] 2-A
  • [4] Brabec CJ, 2001, ADV FUNCT MATER, V11, P374, DOI 10.1002/1616-3028(200110)11:5<374::AID-ADFM374>3.0.CO
  • [5] 2-W
  • [6] The polymer-fullerene interpenetrating network: one route to a solar cell approach
    Dyakonov, V
    [J]. PHYSICA E-LOW-DIMENSIONAL SYSTEMS & NANOSTRUCTURES, 2002, 14 (1-2) : 53 - 60
  • [7] Electronic structure and current injection in zinc phthalocyanine doped with tetrafluorotetracyanoquinodimethane: Interface versus bulk effects
    Gao, WY
    Kahn, A
    [J]. ORGANIC ELECTRONICS, 2002, 3 (02) : 53 - 63
  • [8] Electronic and chemical properties of tin-doped indium oxide (ITO) surfaces and ITO/ZnPc interfaces studied in-situ by photoelectron spectroscopy
    Gassenbauer, Y
    Klein, A
    [J]. JOURNAL OF PHYSICAL CHEMISTRY B, 2006, 110 (10) : 4793 - 4801
  • [9] THE ELECTRONIC-STRUCTURE OF FULLERENES AND FULLERENE COMPOUNDS FROM HIGH-ENERGY SPECTROSCOPY
    GOLDEN, MS
    KNUPFER, M
    FINK, J
    ARMBRUSTER, JF
    CUMMINS, TR
    ROMBERG, HA
    ROTH, M
    SING, M
    SCHMIDT, M
    SOHMEN, E
    [J]. JOURNAL OF PHYSICS-CONDENSED MATTER, 1995, 7 (43) : 8219 - 8247
  • [10] Electronic structure of lithium phthalocyanine studied by ultraviolet photoemission spectroscopy
    Kimura, T
    Sumimoto, M
    Sakaki, S
    Fujimoto, H
    Hashimoto, Y
    Matsuzaki, S
    [J]. CHEMICAL PHYSICS, 2000, 253 (01) : 125 - 131