Alkali-metal-atom polarization imaging in high-pressure optical-pumping cells

1998 ◽  
Vol 58 (3) ◽  
pp. 2282-2294 ◽  
Author(s):  
A. Ben-Amar Baranga ◽  
S. Appelt ◽  
C. J. Erickson ◽  
A. R. Young ◽  
W. Happer
Keyword(s):  
High Pressure ◽  
Alkali Metal ◽  
Metal Atom ◽  
Optical Pumping ◽  
Alkali Metal Atom ◽  
Polarization Imaging

Alkali metal atom adsorption on-top of the F s 0 defective center of MgO(001) surface

2011 ◽  
Vol 15 (3) ◽  
pp. 223-228 ◽  
Author(s):  
Xu Zhang ◽  
Run Xu ◽  
Lin-jun Wang ◽  
Feng Hong
Keyword(s):  
Alkali Metal ◽  
Metal Atom ◽  
Alkali Metal Atom

Collision-Induced Absorption in Alkali-Metal-Atom—Inert-Gas Mixtures

1973 ◽  
Vol 7 (5) ◽  
pp. 1606-1609 ◽  
Author(s):  
C. Bottcher ◽  
A. Dalgarno ◽  
E. L. Wright
Keyword(s):  
Alkali Metal ◽  
Metal Atom ◽  
Alkali Metal Atom ◽  
Gas Mixtures ◽  
Inert Gas ◽  
Induced Absorption

BONDING NATURE OF INTERCALATION COMPOUNDS M1/3TiS2 (M=TRANSITION-METAL ATOM, SILVER ATOM, ALKALI-METAL ATOM)

1993 ◽  
Vol 07 (01n03) ◽  
pp. 374-378 ◽  
Author(s):  
Naoshi SUZUKI ◽  
Tatsuya TESHIMA ◽  
Kazuko MOTIZUKI
Keyword(s):  
Transition Metal ◽  
Alkali Metal ◽  
Metal Atom ◽  
Silver Atom ◽  
Alkali Metal Atom ◽  
Intercalation Compounds ◽  
Energy Calculation ◽  
Covalent Bonds ◽  
Total Energy Calculation ◽  
Cohesive Properties

Self-consistent LAPW band calculations have been carried out systematically for intercalation compounds M 1/3 TiS 2 (M=transition metal, silver, alkali metal) in order to clarify bonding nature between the guest atoms and the host TiS 2. In transition-metal intercalates the guest 3d states hybridize with the S 3p states as well as the Ti 3d states. As the result covalent bonds are formed between the guest 3d and S 3p states, conserving the covalent bonds between the Ti 3d and S 3p states of the host. In Ag 1/3 TiS 2 the Ag 4d states hybridize strongly with the S 3p state and destroy the host covalent bonds between the Ti 3d and S 3p states. In Li 1/3 TiS 2 and K 1/3 TiS 2 there is little hybridization between the guest 2s or 4s states and the host Ti 3d or S 3p states. Cohesive properties of M 1/3 TiS 2 compounds, including stacking structures of the guest atoms, are discussed on the basis of the total energy calculation.

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