TY - JOUR
T1 - Formation and characterization of epitaxial phthalocyanine and perylene monolayers and bilayers on Cu(100)
T2 - Low-energy electron diffraction and thermal desorption mass spectrometry studies
AU - Schueriein, T. J.
AU - Armstrong, N. R.
PY - 1994/7
Y1 - 1994/7
N2 - Ordered monolayer and multilayer thin films of copper phthalocyanine (CuPc) and perylene dicarboxylic di anhydride (PTCDA) have been grown on Cu(100) single crystals. CuPc grows in a commensurate square lattice configuration, with two equivalent domains consisting of closest packed, flat lying Pc rings, rotated at ±21.8° from the principle Cu(iOO) axes. The dimensions of these square lattices (bl = b2 = 13J A) are comparable to those observed using other substrates which interact weakly with the Pc overlayer (layered metal dichalocogenides, cleavage faces of single-crystal salts). PTCDA grows in a commensurate rectangular lattice (5yߢ2X4v’2)-/? = 45 whose dimensions (Z — 14.5 A, b2 = lS.1 A) are significantly different than those seen on weakly interacting substrates. Low-energy electron diffraction (LEED), x-ray photoelectron spectroscopy, and thermal desorption mass spectroscopy (TDMS) data for the adsorption of this molecule strongly suggest that the first monolayer is dissociatively adsorbed to the Cu(100) surface. Growth of ordered layers of PTCDA has also been carried out on a Cu(100) surface modified with 1 -2 ML (monolayers) of an ordered CuPc film. LEED and TDMS data indicate the formation of a new commensurate rectangular unit cell (ftj = 13.7 A, b2—20.5 A) for these PTCDA/CuPc/Cu(100) overlayers, which suggest that the CuPc layer controls the architecture of the subsequent PTCDA layers. The formation of a wide range of highly ordered organic heterojunctions appears to be possible, starting with a strongly adsorbed first layer, on surfaces such as single-crystal metals.
AB - Ordered monolayer and multilayer thin films of copper phthalocyanine (CuPc) and perylene dicarboxylic di anhydride (PTCDA) have been grown on Cu(100) single crystals. CuPc grows in a commensurate square lattice configuration, with two equivalent domains consisting of closest packed, flat lying Pc rings, rotated at ±21.8° from the principle Cu(iOO) axes. The dimensions of these square lattices (bl = b2 = 13J A) are comparable to those observed using other substrates which interact weakly with the Pc overlayer (layered metal dichalocogenides, cleavage faces of single-crystal salts). PTCDA grows in a commensurate rectangular lattice (5yߢ2X4v’2)-/? = 45 whose dimensions (Z — 14.5 A, b2 = lS.1 A) are significantly different than those seen on weakly interacting substrates. Low-energy electron diffraction (LEED), x-ray photoelectron spectroscopy, and thermal desorption mass spectroscopy (TDMS) data for the adsorption of this molecule strongly suggest that the first monolayer is dissociatively adsorbed to the Cu(100) surface. Growth of ordered layers of PTCDA has also been carried out on a Cu(100) surface modified with 1 -2 ML (monolayers) of an ordered CuPc film. LEED and TDMS data indicate the formation of a new commensurate rectangular unit cell (ftj = 13.7 A, b2—20.5 A) for these PTCDA/CuPc/Cu(100) overlayers, which suggest that the CuPc layer controls the architecture of the subsequent PTCDA layers. The formation of a wide range of highly ordered organic heterojunctions appears to be possible, starting with a strongly adsorbed first layer, on surfaces such as single-crystal metals.
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U2 - 10.1116/1.578995
DO - 10.1116/1.578995
M3 - Article
AN - SCOPUS:21344490081
SN - 0734-2101
VL - 12
SP - 1992
EP - 1997
JO - Journal of Vacuum Science and Technology A: Vacuum, Surfaces and Films
JF - Journal of Vacuum Science and Technology A: Vacuum, Surfaces and Films
IS - 4
ER -