F-Center Formation in Mixed Crystals of Alkali Halides

1965 ◽  
Vol 10 (1) ◽  
pp. 105-112 ◽  
Author(s):  
J. Arends ◽  
H. W. den Hartog ◽  
A. J. Dekker
Keyword(s):  
Alkali Halides ◽  
Mixed Crystals ◽  
F Center

High-pressure optical studies of doped alkali halides. IV. Mixed crystals

1976 ◽  
Vol 13 (10) ◽  
pp. 4592-4596 ◽  
Author(s):  
W. D. Drotning ◽  
H. G. Drickamer
Keyword(s):  
High Pressure ◽  
Alkali Halides ◽  
Mixed Crystals ◽  
Optical Studies

FBands in Some Mixed Crystals of the Alkali Halides

1953 ◽  
Vol 21 (2) ◽  
pp. 323-330 ◽  
Author(s):  
Robert J. Gnaedinger
Keyword(s):  
Alkali Halides ◽  
Mixed Crystals

Lattice Matching and Relaxation of Vanadyl-Phthalocyanine Crystal Epitaxially Grown on Mixed Crystals of Alkali Halides

1997 ◽  
Vol 36 (Part 2, No. 5B) ◽  
pp. L622-L624 ◽  
Author(s):  
Satoru Nakao ◽  
Makoto Gomyou ◽  
Hajime Hoshi ◽  
Ken Ishikawa ◽  
Hideo Takezoe
Keyword(s):  
Alkali Halides ◽  
Mixed Crystals ◽  
Lattice Matching

Ab initio calculations of SrTiO3, BaTiO3, PbTiO3, CaTiO3, SrZrO3, PbZrO3 and BaZrO3 (001), (011) and (111) surfaces as well as F centers, polarons, KTN solid solutions and Nb impurities therein

2014 ◽  
Vol 28 (17) ◽  
pp. 1430009 ◽  
Author(s):  
R. I. Eglitis
Keyword(s):  
Ab Initio Calculations ◽  
Ab Initio ◽  
Solid Solutions ◽  
Alkali Halides ◽  
Shallow Donor ◽  
Surface Energies ◽  
F Center ◽  
Bonding Properties ◽  
Almost All ◽  
F Centers

In this paper, the review of recent results of calculations of surface relaxations, energetics, and bonding properties for ABO 3 perovskite (001), (011) and (111) surfaces using mostly a hybrid description of exchange and correlation is presented. Both AO and BO 2-terminations of the nonpolar (001) surface and A , BO , and O terminations of the polar (011) surface, as well as B and AO 3-terminations of the polar (111) surface were considered. On the AO -terminated (001) surface, all upper-layer A atoms relax inwards, while all second layer atoms relax outwards. For the BO 2-terminated (001) surface, in most cases, the largest relaxations are on the second-layer metal atoms. For almost all ABO 3 perovskites, the surface rumpling is much larger for the AO -terminated than for the BO 2-terminated (001) surface, but their surface energies are always quite similar. In contrast, different terminations of the (011) ABO 3 surface lead to very different surface energies for the O -terminated, A -terminated, and BO -terminated (011) surface, respectively. A considerable increase in the Ti – O or Zr – O , respectively, chemical bond covalency near the (011) surface as compared both to the bulk and to the (001) surface in ABO 3 perovskites were predicted. According to the results of ab initio calculations for Nb doped SrTiO 3, Nb is a shallow donor; six nearest O ions are slightly displaced outwards from the Nb ion. The F center in ABO 3 perovskites resembles electron defects in the partially-covalent SiO 2 crystal rather than usual F centers in ionic crystals like MgO and alkali halides. The results of calculations for several perovskite KNb x Ta 1-x O 3 (KTN) solid solutions, as well as hole and electron polarons in ABO 3 perovskites are analyzed.

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