Nuclear Quadrupole Interaction of Alkali-Metal Atoms Adsorbed on Metal Surfaces

1986 ◽  
Vol 41 (1-2) ◽  
pp. 113-117
Author(s):  
D. Fick ◽  
B. Horn ◽  
E. Koch ◽  
U. Memmert

A new technique is discussed for probing microscopic details o f surface charge distributionsusing beams o f thermal-velocity nuclear-spin-polarized atoms. The technique has made possibleone o f the first spin-relaxation and the first nuclear-spin-resonance experiments on single-crystalmetal surfaces.

1989 ◽  
Vol 39 (11) ◽  
pp. 5613-5623 ◽  
Author(s):  
S. R. Schaefer ◽  
G. D. Cates ◽  
Ting-Ray Chien ◽  
D. Gonatas ◽  
W. Happer ◽  
...  

1996 ◽  
Vol 51 (8) ◽  
pp. 898-904 ◽  
Author(s):  
Axel H. Saleck ◽  
Thomas Klaus ◽  
Sergei P. Belov ◽  
Gisbert Winnewisser

Abstract We have observed the pure rotational spectra of HBr isotopomers in their υ = 0 and υ = 1 states between 0.97 and 1.02 THz. i. e. the HBr Ј = 2-1 and the DBr Ј =4 - 3 transitions, respectively. In the analysis, all presently available rotational transitions of all isotopomers have been fitted to a Dunham-type Hamiltonian to obtain the isotopically invariant parameters, including vibrational and rotational expansion coefficients for the hyperfine constants. In the analysis, the vibrational expansion coefficients of the nuclear quadrupole interaction are determined up to second order, and up to first order for the nuclear spin-rotation interaction.


Author(s):  
M. M. Glazov

This chapter is devoted to one of key phenomena in the field of spin physics, namely, resonant absorption of electromagnetic waves under conditions where the Zeeman splitting of spin levels in magnetic field is equal to photon energy. This method is particularly important for identification of nuclear spin effects, because resonance spectra provide fingerprints of different involved spin species and make it possible to distinguish different nuclear isotopes. As discussed in this chapter the nuclear magnetic resonance provides also an access to local magnetic fields acting on nuclear spins. These fields are caused by the magnetic interactions between the nuclei and by the quadrupole splittings of nuclear spin states in anisotropic crystalline environment. Manifestations of spin resonance in optical responses of semiconductors–that is, optically detected magnetic resonance–are discussed.


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