X-RAY STRUCTURE OF FAC-IMN(CO)(3)(BPY) AND ELECTRONIC-STRUCTURES AND TRANSITIONS OF THE COMPLEXES FAC-XMN(CO)(3)(BPY) (X=CL, I) AND MER-CLMN(CO)(3)(BPY)

被引:65
作者
STOR, GJ
STUFKENS, DJ
VERNOOIJS, P
BAERENDS, EJ
FRAANJE, J
GOUBITZ, K
机构
[1] UNIV AMSTERDAM,ANORGAN CHEM LAB,1018 WV AMSTERDAM,NETHERLANDS
[2] VRIJE UNIV AMSTERDAM,AFDELING THEORET CHEM,1081 HV AMSTERDAM,NETHERLANDS
[3] UNIV AMSTERDAM,KRISTALLOG LAB,1018 WV AMSTERDAM,NETHERLANDS
关键词
D O I
10.1021/ic00110a042
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
MO calculations have been performed on the complexes fac-XMn(CO)(3)(bpy) (X = Cl, I) and mer-ClMn(CO)(3)-(bpy) in order to establish the influence of X on the electronic transitions of the fac and mer isomers and to interpret the differences in photochemical behavior of the fac and mer complexes. SCF calculations were performed with the Amsterdam density-functional program package ADF. The structural data used for the calculations were partly derived from the X-ray structure of fac-IMn(CO)(3)(bpy) presented in the article. The theoretical data for the fac isomers show that the two highest occupied orbitals have metal-halide antibonding character and that the LUMO is a pi* (bpy) orbital. The first absorption band is therefore assigned to electronic transitions having mixed metal-halide to bpy CT character. The second absorption band is assigned to CT transitions from the corresponding metal-halide bonding orbitals to bpy. From a comparison of the theoretical and spectroscopic data, the intensities of these two absorption bands appear to depend on the metal character of the orbitals from which the electronic transitions originate. The main difference between the theoretical data of the fac- and mer-ClMn(CO)(3)(bpy) complexes is the higher energy of the highest filled orbitals in the case of the mer isomer. This difference is in accordance with the spectroscopic data and may also explain the differences in photochemistry between the two isomers.
引用
收藏
页码:1588 / 1594
页数:7
相关论文
共 54 条
[11]   PHOTOELECTRON-SPECTRA OF RHENIUM PENTACARBONYL HALIDES [J].
CEASAR, GP ;
MILAZZO, P ;
CIHONSKI, JL ;
LEVENSON, RA .
INORGANIC CHEMISTRY, 1974, 13 (12) :3035-3037
[12]  
COWLEY AH, 1979, PROG INORG CHEM, V26, P46
[13]   X-RAY SCATTERING FACTORS COMPUTED FROM NUMERICAL HARTREE-FOCK WAVE FUNCTIONS [J].
CROMER, DT ;
MANN, JB .
ACTA CRYSTALLOGRAPHICA SECTION A-CRYSTAL PHYSICS DIFFRACTION THEORETICAL AND GENERAL CRYSTALLOGRAPHY, 1968, A 24 :321-&
[14]  
CROMER DT, 1974, INT TABLES XRAY CRYS, V4, P55
[15]  
DANIEL CW, COMMUNICATION
[16]  
DEKOCK RL, 1977, ELECTRON SPECTROSCOP, V1, P294
[17]  
EVANS S, 1969, DISCUSS FARADAY SOC, V47, P112
[18]   ELECTRONIC STRUCTURE AND BONDING IN MANGANESE PENTACARBONYL HALIDES AND HYDRIDE [J].
FENSKE, RF ;
DEKOCK, RL .
INORGANIC CHEMISTRY, 1970, 9 (05) :1053-&
[19]  
Geoffroy G.L., 1979, ORGANOMETALLIC PHOTO
[20]   PHOTOSUBSTITUTION BEHAVIOR OF DICARBONYL(ETA-5-CYCLOPENTADIENYL) PYRIDINOMANGANESE AND PYRIDINORHENIUM AND RELATED COMPLEXES [J].
GIORDANO, PJ ;
WRIGHTON, MS .
INORGANIC CHEMISTRY, 1977, 16 (01) :160-166