scholarly journals Energy-level splitting of ground-states and Jahn-Teller effects in ruby crystal

2006 ◽  
Vol 55 (11) ◽  
pp. 6055
Author(s):  
Yin Chun-Hao ◽  
Zhang Lei ◽  
Zhao Ji-Ping ◽  
Jiao Yang ◽  
Song Ning ◽  
...  
2002 ◽  
Vol 731 ◽  
Author(s):  
R.A. Evarestov ◽  
R.I. Eglitis ◽  
S. Piskunov ◽  
E. A. Kotomin ◽  
G. Borstel

AbstractUsing the Unrestricted Hartree-Fock method and supercells containing up to 160 atoms, we calculated the energy level positions in the gap and atomic geometry for the Fe4+ impurity substituting for a host Ti atom in SrTiO3. In agreement with experiment, the high spin (S=2) state is much lower in energy than the zero-spin state. The energy level positions strongly depend on the asymmetric displacement mode of the six nearest O ions which is a combination of the Jahn-Teller and breathing modes. A considerable covalent bonding between the Fe ion and four nearest O ions takes place.


2018 ◽  
Vol 58 (2) ◽  
pp. 1058-1066 ◽  
Author(s):  
Meng Ju ◽  
MingMin Zhong ◽  
Cheng Lu ◽  
Yau-yuen Yeung

1982 ◽  
Vol 53 (3) ◽  
pp. 2107-2109 ◽  
Author(s):  
C. M. Srivastava ◽  
M. J. Patni ◽  
T. T. Srinivasan

1979 ◽  
Vol 16 (1) ◽  
pp. 17-25
Author(s):  
S. Middelhoek ◽  
W. S. M. Beke

A description is given of a lecture demonstration of energy level splitting in the hydrogen molecule. The demonstration is based on the electrical analogue of two coupled resonant circuits. Coupling occurs by mutual inductance. The relevant differential equations describing the hydrogen atom and the tuned circuits are also presented.


1985 ◽  
Vol 151 (2-3) ◽  
pp. L145-L152 ◽  
Author(s):  
M. Chiesa ◽  
L. Mattera ◽  
R. Musenich ◽  
C. Salvo

1979 ◽  
Vol 34 (12) ◽  
pp. 1500-1506
Author(s):  
P. Ganguli ◽  
K. M. Hasselbach

Abstract SCCEHMO calculations show that the ground state in [Fe(dtc)2X], X = Cl, Br, I and NCS, is 4A2: (x2 - y2)2(xz)1(yz)1(z2)1(xy)0 and for X = NO is 2A1: (xz)2(yz)2(x2-y2)2(z2)1(xy)0. The calculated quadrupole splittings of iron and iodine included the valence shell, overlap charge, and the ligand and lattice contributions to the EFG tensor at the nuclei. In addition, the elec-tron densities at the iron nucleus are compared with the measured isomer shifts. The spin densi-ties may be interpreted in terms of a π-delocalization. The results are discussed on the basis of the molecular orbital energy level schemes.


1999 ◽  
Vol 97 (1-2) ◽  
pp. 239-254 ◽  
Author(s):  
TIMOTHY A. BARCKHOLTZ ◽  
MIN-CHIEH YANG ◽  
TERRY A. MILLER
Keyword(s):  

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