Novel organic ions of high-spin state. 2. Determination of the spin multiplicity of the ground state and 1H-ENDOR study of the monoanion of m-phenylenebis(phenylmethylene)

1992 ◽  
Vol 114 (19) ◽  
pp. 7470-7475 ◽  
Author(s):  
Michio Matsushita ◽  
Toshihiro Nakamura ◽  
Takamasa Momose ◽  
Tadamasa Shida ◽  
Yoshio Teki ◽  
...  
2006 ◽  
Vol 527-529 ◽  
pp. 523-526 ◽  
Author(s):  
Adam Gali ◽  
M. Bockstedte ◽  
Nguyen Tien Son ◽  
T. Umeda ◽  
Junichi Isoya ◽  
...  

Only recently the well-resolved hyperfine structure of the P6/P7 EPR center has been experimentally observed. Based on the calculated hyperfine tensors we assign the P6/P7 center to the high spin state neutral divacancy, which is the ground state in agreement with the experiment. We propose a mechanism to explain the loss of divacancy signal at high tem- perature annealing in semi-insulating SiC samples. We discuss the possible correlation between the divacancy and some photoluminescence centers.


2013 ◽  
Vol 87 (21) ◽  
Author(s):  
Pradip Chakraborty ◽  
Antoine Tissot ◽  
Lisa Peterhans ◽  
Laure Guénée ◽  
Céline Besnard ◽  
...  

2013 ◽  
Vol 2013 ◽  
pp. 1-4
Author(s):  
Jillian Lennartz ◽  
Eric Dumas ◽  
Lennie Ramirez ◽  
John Morrison Galbraith

The lowest energy geometric structures and electronic spin states of first row transition metal (TM) dioxygen dication molecules ([TM–O2]2+; TM = Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, and Zn) have been determined at the B3LYP/LANL2DZ level of theory (along with an extra d-type polarization function added to the O atoms). In order to further verify the spin states, CASSCF(6 + n, 9) energy points were determined (n = number of TM d electrons). It has been found that with the exception of [Sc–O2]2+, [V–O2]2+, [Co–O2]2+, and [Ni–O2]2+, all [TM–O2]2+ molecules take on a high-spin state. [Sc–O2]2+ adopts a trigonal structure, while [Ti–O2]2+-[Mn–O2]2+ are essentially linear and [Fe–O2]2+-[Zn–O2]2+ are bent. It is further noted that the O–O bond decreases from 130.0 pm to 118.1 pm as the TM changes from Sc to Zn. However, the TM–O2 bond lengths fluctuate between values of 182.2 pm for [Ni–O2]2+ and 232.2 pm for [Zn–O2]2+.


Energy ◽  
2019 ◽  
Vol 189 ◽  
pp. 116286 ◽  
Author(s):  
Hai Zhang ◽  
Lei Luo ◽  
Jiaxun Liu ◽  
Anyao Jiao ◽  
Jianguo Liu ◽  
...  

2007 ◽  
Vol 63 (a1) ◽  
pp. s202-s202
Author(s):  
U. Pietsch ◽  
M. Lommel ◽  
Y. Bodethin ◽  
D. Kurth ◽  
G. Schwarzl ◽  
...  

Author(s):  
Guangxin Song ◽  
Rui Gao ◽  
Zhao Zhao ◽  
Yujun Zhang ◽  
Huaqiao Tan ◽  
...  

1998 ◽  
Vol 53 (9) ◽  
pp. 755-765
Author(s):  
Christian Kollma ◽  
Sighart F. Fischer ◽  
Michael C. Böhm

AbstractThe origin of the displacement of the Fe atom in deoxymyoglobin with respect to the porphyrin plane in the high-spin state is examined by a qualitative molecular orbital (MO) analysis on the extended Hückel level. We find that attachment of a fifth ligand (imidazole in our model complex) to Fe(II)porphyrin favors the out-of-plane shift due to a strengthening of the bonding interaction between Fe and the nitrogen of the imidazole ligand. This results in a high-spin (5 = 2) ground state with Fe shifted out-of-plane for the five-coordinate complex instead of an intermediate spin ground state (5 = 1) with Fe lying in the plane for four-coordinate Fe(II)porphyrin. The relative energies of the different spin states as a function of the distance between Fe and the porphyrin plane are evaluated using an ROHF (restricted open shell Hartree-Fock) version of an INDO (intermediate neglect of differential overlap) method. We observe a level crossing between high-spin and intermediate spin states whereas the low-spin (5 = 0) state remains always higher in energy.


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