Carbon-13 hyperfine constants, g-factors and electronic structure of m-benzosemiquinone radical anions

1982 ◽  
Vol 86 (15) ◽  
pp. 2926-2929 ◽  
Author(s):  
Keith P. Madden ◽  
Hugh J. McManus ◽  
Robert H. Schuler
1979 ◽  
Vol 172 (4) ◽  
pp. C63-C65 ◽  
Author(s):  
R.S. Dickson ◽  
B.M. Peake ◽  
P.H. Rieger ◽  
B.H. Robinson ◽  
J. Simpson

1970 ◽  
Vol 39 (7) ◽  
pp. 591-608 ◽  
Author(s):  
Stanislav P Solodovnikov ◽  
Alexandr I Prokof'ev

2003 ◽  
Vol 07 (12) ◽  
pp. 801-806 ◽  
Author(s):  
Dmitri V. Konarev ◽  
Salavat S. Khasanov ◽  
Gunzi Saito ◽  
Rimma N. Lyubovskaya

The complexes of cobalt(II) tetraphenylporphyrin ( Co II TPP ) with fullerenes C 60, C 70 and C 60( CN )2 are presented. It is shown that Co II TPP forms complexes with fullerenes in different solvents: [ Co II TPP •fullerene•solvent] ( solvent = C 6 H 6, C 6 H 5 Me , C 6 H 4 Cl 2, CS 2, CHCl 3). The use of additional donors ( Cp 2 Fe , Cr 0( C 6 H 6)2, and TDAE ) in the synthesis of Co II TPP /fullerene complexes allows one to obtain multi-component complexes ranging from neutral [( Co II TPP • Py )2• Cp 2 Fe • fullerene • solvent ] to ionic [ Co II TPP •( D 2•+)•( fullerene •−)• solvent ] ( D 2 = Cr I( C 6 H 6)2, TDAE ). The interaction of Co II TPP with neutral and negatively charged fullerenes is considered. The neutral Co II TPP /fullerene complexes are characterized by a secondary M…C(fullerene) bonding with the shortest Co … C contacts in the 2.69-2.82 Å range and noticeable changes in the electronic structure of the parent components. At the same time, σ-bonding is observed in ionic complexes between Co II TPP and fullerene radical anions with the shortened Co … C contacts being in the 2.28-2.32 Å range. The resulting ( Co II TPP •fullerene−) anions are diamagnetic. The σ-bonding is relatively weak and the ( Co II TPP •fullerene−) anions begin to dissociate above 200 K.


1978 ◽  
Vol 56 (7) ◽  
pp. 827-837 ◽  
Author(s):  
C. W. T. Chien ◽  
F. W. Dalby ◽  
J. Van Der Linde

Accurate experimental radiative lifetimes, disalignment cross sections, hyperfine constants, and Zeeman g factors are reported for a number of rotational levels of the 3d electronic complex and the nearby doubly excited K1Σg+ state of molecular hydrogen. The 3d complex of states is not a complete basis for calculation of the above molecular properties. A theory of the Hanle effect in the presence of hyperfine structure is presented.


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