Ali Md Ehesan, Vyas Shubham, Datta Sambhu N
Department of Chemistry, Indian Institute of Technology-Bombay, Powai, Mumbai-400076, India.
J Phys Chem A. 2005 Jul 21;109(28):6272-8. doi: 10.1021/jp050282v.
The magnetic properties of the monoradicals 2-(4-phenyl acetylene)-4,4,5,5-tetramethyl-4,5-dihydro-1H-imidozolyl-oxyl (1) and 2-(4-phenyl acetylene)-4,4,5,5-tetramethyl-4,5-dihydro-1H-imidazole-1-oxyl-3-oxide (2) and the diradicals 2,2'-(1,2-ethynediyldi-4,1-phenylene)bis[4,4,5,5-tetramethyl-4,5-dihydro-1H-imidozolyl-oxyl] (3), 2,2'-(1,2-ethynediyldi-4,1 3,1-phenylene)bis[4,4,5,5-tetramethyl-4,5-dihydro-1H-imidozolyl-oxyl] (4), and 2,2'-(1,2-ethynediyldi-4,1 3,1-phenylene)bis[4,4,5,5-tetramethyl-4,5-dihydro-1H-imidazole-1-oxyl-3-oxide] (5) are investigated by ab initio quantum chemical methods. The rule of spin alternation in the unrestricted Hartree-Fock (UHF) method clearly shows that the radical sites are antiferromagnetically coupled in 3 and ferromagnetically coupled in 4 and 5, which is consistent with a previous experiment. The molecular geometries are optimized at Hartree-Fock levels. This is followed by single-point calculations using the density functional (UB3LYP) treatment and the multiconfigurational complete active space self-consistent field (CASSCF) methodology. Magnetic exchange coupling constants are determined from the broken-symmetry approach. The calculated J values, -3.60 cm(-1) for 3, 0.16 cm(-1) for 4, and 0.67 cm(-1) for 5, are in excellent agreement with the observed values. Because of the very large size of the diradicals 3-5, the CASSCF (10,10) calculations cannot yield realistic J values. Nevertheless, the CASSCF calculations support the antiferromagnetic nature of the magnetic coupling in 3 and the ferromagnetic nature of the coupling in 4 and 5. The existence of an intramolecular magnetic coupling in 3-5 is also confirmed through computations of the isotropic hyperfine coupling constants for monoradicals 1 and 2 as well as diradicals 3-5.
采用从头算量子化学方法研究了单自由基2-(4-苯基乙炔基)-4,4,5,5-四甲基-4,5-二氢-1H-亚氨基唑氧基(1)、2-(4-苯基乙炔基)-4,4,5,5-四甲基-4,5-二氢-1H-咪唑-1-氧基-3-氧化物(2)以及双自由基2,2'-(1,2-乙炔二基二-4,1-亚苯基)双4,4,5,5-四甲基-4,5-二氢-1H-亚氨基唑氧基、2,2'-(1,2-乙炔二基二-4,1 3,1-亚苯基)双4,4,5,5-四甲基-4,5-二氢-1H-亚氨基唑氧基和2,2'-(1,2-乙炔二基二-4,1 3,1-亚苯基)双4,4,5,5-四甲基-4,5-二氢-1H-咪唑-1-氧基-3-氧化物的磁性。在无限制哈特里-福克(UHF)方法中自旋交替规则清楚地表明,自由基位点在3中是反铁磁耦合的,而在4和5中是铁磁耦合的,这与先前的实验一致。分子几何结构在哈特里-福克水平上进行了优化。随后使用密度泛函(UB3LYP)处理和多组态完全活性空间自洽场(CASSCF)方法进行单点计算。磁交换耦合常数由破缺对称性方法确定。计算得到的J值,3为-3.60 cm(-1),4为0.16 cm(-1),5为0.67 cm(-1),与观测值非常吻合。由于双自由基3-5尺寸非常大,CASSCF(10,10)计算无法得出实际的J值。然而,CASSCF计算支持3中磁耦合的反铁磁性质以及4和5中耦合的铁磁性质。通过计算单自由基1和2以及双自由基3-5的各向同性超精细耦合常数,也证实了3-5中存在分子内磁耦合。