Results 301 to 310 of about 3,259,463 (359)
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Nature, 1932
As a possible explanation of the anomalous g(I) factors of nuclear magnetic moments found in heavy and in light elements respectively by McLennan, McLay, and Crawford,1 and by me,2 it was suggested in both these papers that an orbital motion of some of the nuclear protons might fit the observed facts.
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As a possible explanation of the anomalous g(I) factors of nuclear magnetic moments found in heavy and in light elements respectively by McLennan, McLay, and Crawford,1 and by me,2 it was suggested in both these papers that an orbital motion of some of the nuclear protons might fit the observed facts.
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Modern Physics Letters A, 2005
Finite neutrino magnetic moments are consequences of nonzero neutrino masses. The particle physics aspects of the neutrino electromagnetic interactions are reviewed. The astrophysical bounds and the results from recent direct experiments are reviewed, with emphasis on the reactor neutrino experiments. Future projects and prospects are surveyed.
HENRY T. WONG, HAU-BIN LI
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Finite neutrino magnetic moments are consequences of nonzero neutrino masses. The particle physics aspects of the neutrino electromagnetic interactions are reviewed. The astrophysical bounds and the results from recent direct experiments are reviewed, with emphasis on the reactor neutrino experiments. Future projects and prospects are surveyed.
HENRY T. WONG, HAU-BIN LI
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Journal of Magnetism and Magnetic Materials, 1992
Abstract Magnetic properties of rough Fe(110) films have been investigated by Torsion Oscillation Magnetometry (TOM). It is found that the magnetic moment of a single Fe-atom on a step edge is increased by (0.7±0.4) μ B to (3.4±0.4) μ b , compared to a surface moment of (2.7±0.2) μ B . The result is roughly in accordance with values obtained from
M. Albrecht +3 more
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Abstract Magnetic properties of rough Fe(110) films have been investigated by Torsion Oscillation Magnetometry (TOM). It is found that the magnetic moment of a single Fe-atom on a step edge is increased by (0.7±0.4) μ B to (3.4±0.4) μ b , compared to a surface moment of (2.7±0.2) μ B . The result is roughly in accordance with values obtained from
M. Albrecht +3 more
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Hyperfine Interactions, 1993
The magnetic moment of the23Mg (Iπ=3/2+, T1/2=11.3 s), has been determined as |μ(23Mg)|=0.5364±0.003 µN by use of β-NMR detection with the recoil polarization obtained through a low energy nuclear reaction.
M. Fukuda +8 more
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The magnetic moment of the23Mg (Iπ=3/2+, T1/2=11.3 s), has been determined as |μ(23Mg)|=0.5364±0.003 µN by use of β-NMR detection with the recoil polarization obtained through a low energy nuclear reaction.
M. Fukuda +8 more
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Hyperfine Interactions, 1983
Properties of the [512] 5/2−, [633] 7/2+ and [514] 7/2− bands have been studied by experiments on the magnetic moments of the [512] 5/2− 7/2− (79 keV; g=0.058(19)), [512] 5/2− 9/2− (179 keV; g=+0.06(8)) and [633] 7/2 7/2 (351 keV; g=−0.13(13)) states.
G. Carlsson +4 more
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Properties of the [512] 5/2−, [633] 7/2+ and [514] 7/2− bands have been studied by experiments on the magnetic moments of the [512] 5/2− 7/2− (79 keV; g=0.058(19)), [512] 5/2− 9/2− (179 keV; g=+0.06(8)) and [633] 7/2 7/2 (351 keV; g=−0.13(13)) states.
G. Carlsson +4 more
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Nuclear Physics, 1966
Abstract Expressions for the nuclear magnetic moments are given accurately taking into account the nucleon-nucleon interaction. Comparison with experiment makes it possible to determine the constants introduced in the theory and in particular the constant of the spin-spin interaction between the constituent nucleons; the value of this constant is in ...
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Abstract Expressions for the nuclear magnetic moments are given accurately taking into account the nucleon-nucleon interaction. Comparison with experiment makes it possible to determine the constants introduced in the theory and in particular the constant of the spin-spin interaction between the constituent nucleons; the value of this constant is in ...
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1984
Consideration of core polarization, isobar currents and meson-exchange processes gives a satisfactory understanding of the ground-state magnetic moments in closed-shell-plus (or minus)-one nuclei, A = 3, 15, 17, 39 and 41.
I. S. Towner, F. C. Khanna
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Consideration of core polarization, isobar currents and meson-exchange processes gives a satisfactory understanding of the ground-state magnetic moments in closed-shell-plus (or minus)-one nuclei, A = 3, 15, 17, 39 and 41.
I. S. Towner, F. C. Khanna
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Nuclear Physics A, 1980
Abstract Exchange magnetic moments are investigated by adopting a phenomenological approach and a field theoretical model. Their contributions are estimated for nuclei with a particle or hole outside a closed shell. They are expressed in terms of corrections of gyromagnetic factors.
H. Hyuga, A. Arima, K. Shimizu
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Abstract Exchange magnetic moments are investigated by adopting a phenomenological approach and a field theoretical model. Their contributions are estimated for nuclei with a particle or hole outside a closed shell. They are expressed in terms of corrections of gyromagnetic factors.
H. Hyuga, A. Arima, K. Shimizu
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JOM, 1965
Experimental facts; a discussion of theory; and answers to such questions as: Why do local moments appear in some solid solutions and not in others? And, how has the understanding of these moments cast new light on the general phenomenon of magnetism in such metals as chromium and iron?
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Experimental facts; a discussion of theory; and answers to such questions as: Why do local moments appear in some solid solutions and not in others? And, how has the understanding of these moments cast new light on the general phenomenon of magnetism in such metals as chromium and iron?
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2001
Abstract In this chapter the properties of isolated magnetic moments will be examined. At this stage, interactions between magnetic moments on different atoms, or between magnetic moments and their immediate environments, are ignored. All that remains is therefore just the physics of isolated atoms and their interaction with an applied ...
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Abstract In this chapter the properties of isolated magnetic moments will be examined. At this stage, interactions between magnetic moments on different atoms, or between magnetic moments and their immediate environments, are ignored. All that remains is therefore just the physics of isolated atoms and their interaction with an applied ...
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