The two possible schemes of inversionless amplification of resonant (gamma) -radiation with radiofrequency pumping have been analyzed by making use of the effective model of nuclear states.© (2000) COPYRIGHT SPIE--The International Society for Optical Engineering. Downloading of the abstract is permitted for personal use only.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIEJan 14, 20001 citation

Structure of magnetic resonance in 87Rb atoms

Andrey Nikolaevich Kozlov, Sergei A. Zibrov, Alexander S. Zibrov +7 more

Magnetic resonance at the F g = 1 $$ \rightleftarrows $$ F e = 1 transition of the D 1 line in 87Rb has been studied with pumping and detection by linearly polarized radiation and detection at the double frequency of the radiofrequency field. The intervals of allowed values of the static and alternating magnetic fields in which magnetic resonance has a single maximum have been found. The structure appearing beyond these intervals has been explained. It has been shown that the quadratic Zeeman shift is responsible for the three-peak structure of resonance; the radiofrequency shift results in the appearance of additional extrema in resonance, which can be used to determine the relaxation constant Γ2. The possibility of application in magnetometry has been discussed.

Journal of Experimental and Theoretical PhysicsMay 1, 20164 citations

Il Nuovo Cimento

Interference effects of radiofrequency fields in resonance radiation

M. N. Hack

Published Oct 1, 1961• 1 citation

Publisher

DOI: 10.1007/bf02829003

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Structure of magnetic resonance in 87Rb atoms

Andrey Nikolaevich Kozlov, Sergei A. Zibrov, Alexander S. Zibrov +7 more

Magnetic resonance at the F g = 1 $\rightleftarrows$ F e = 1 transition of the D 1 line in 87Rb has been studied with pumping and detection by linearly polarized radiation and detection at the double frequency of the radiofrequency field. The intervals of allowed values of the static and alternating magnetic fields in which magnetic resonance has a single maximum have been found. The structure appearing beyond these intervals has been explained. It has been shown that the quadratic Zeeman shift is responsible for the three-peak structure of resonance; the radiofrequency shift results in the appearance of additional extrema in resonance, which can be used to determine the relaxation constant Γ2. The possibility of application in magnetometry has been discussed.Magnetic resonance at the F g = 1 $$ \rightleftarrows $$ F e = 1 transition of the D 1 line in 87Rb has been studied with pumping and detection by linearly polarized radiation and detection at the double frequency of the radiofrequency field. The intervals of allowed values of the static and alternating magnetic fields in which magnetic resonance has a single maximum have been found. The structure appearing beyond these intervals has been explained. It has been shown that the quadratic Zeeman shift is responsible for the three-peak structure of resonance; the radiofrequency shift results in the appearance of additional extrema in resonance, which can be used to determine the relaxation constant Γ2. The possibility of application in magnetometry has been discussed.

Journal of Experimental and Theoretical PhysicsMay 1, 20164 citations

Magnetic resonance at the F g = 1

\rightleftarrows

F e = 1 transition of the D 1 line in 87Rb has been studied with pumping and detection by linearly polarized radiation and detection at the double frequency of the radiofrequency field. The intervals of allowed values of the static and alternating magnetic fields in which magnetic resonance has a single maximum have been found. The structure appearing beyond these intervals has been explained. It has been shown that the quadratic Zeeman shift is responsible for the three-peak structure of resonance; the radiofrequency shift results in the appearance of additional extrema in resonance, which can be used to determine the relaxation constant Γ2. The possibility of application in magnetometry has been discussed.