Results 201 to 210 of about 1,763,432 (252)
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1976
We do not attempt in these two lectures to develop a coherent formalism of nuclear muon-capture, nor do we drive for completeness in the description of what the study of these processes may teach us about the basic interaction or the nuclear structure. The formalism may be consulted in ref. 1 (impulse approximation) or ref.
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We do not attempt in these two lectures to develop a coherent formalism of nuclear muon-capture, nor do we drive for completeness in the description of what the study of these processes may teach us about the basic interaction or the nuclear structure. The formalism may be consulted in ref. 1 (impulse approximation) or ref.
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Il Nuovo Cimento A, 1971
In this paper the partial-capture rates of muons in11B going to11Be(g.s.) and11Be (320 keV), as well as the hyperfine effect in the transition to11Be*, are studied. Comparing these results with the beta-decay of11Be and the electromagnetic transition11Be* →11Be, we can derive some conclusions on the nuclear structure of the bound states of11Be. We also
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In this paper the partial-capture rates of muons in11B going to11Be(g.s.) and11Be (320 keV), as well as the hyperfine effect in the transition to11Be*, are studied. Comparing these results with the beta-decay of11Be and the electromagnetic transition11Be* →11Be, we can derive some conclusions on the nuclear structure of the bound states of11Be. We also
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Nuclear Physics A, 1973
Abstract Excitation and decay of the giant resonance of 14 C in muon capture by 14 N are considered. A characteristic feature of this process is the large yield of two neutrons and the low yield of charged particles. The allowed transitions are included in the calculation and lead to noticeable neutron emission.
H.R. Kissener +3 more
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Abstract Excitation and decay of the giant resonance of 14 C in muon capture by 14 N are considered. A characteristic feature of this process is the large yield of two neutrons and the low yield of charged particles. The allowed transitions are included in the calculation and lead to noticeable neutron emission.
H.R. Kissener +3 more
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Physical Review C, 1980
It is shown by relating the transition amplitude of radiative muon capture to that of radiative pion capture, that the transition amplitude of radiative muon capture proposed recently by Hwang and Primakoff differs from the others mainly by Low's counter terms.
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It is shown by relating the transition amplitude of radiative muon capture to that of radiative pion capture, that the transition amplitude of radiative muon capture proposed recently by Hwang and Primakoff differs from the others mainly by Low's counter terms.
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Physical Review, 1959
The theory of radiative muon capture is developed. The discussion includes both parity conserving and nonconserving effects. The Gell-Mann weak magnetic term and the induced pseudoscalar are included, along with comparable relativistic effects in the nucleons.
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The theory of radiative muon capture is developed. The discussion includes both parity conserving and nonconserving effects. The Gell-Mann weak magnetic term and the induced pseudoscalar are included, along with comparable relativistic effects in the nucleons.
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Nuclear Physics A, 1975
Abstract The partial capture rates for μ − + 3 He → 3 H + ν, nd + ν and nnp + ν are calculated. The predictions of the impulse approximation and the elementary particle method for the 3 Hν channel are compared.
A.C. Phillips, F. Roig, J. Ros
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Abstract The partial capture rates for μ − + 3 He → 3 H + ν, nd + ν and nnp + ν are calculated. The predictions of the impulse approximation and the elementary particle method for the 3 Hν channel are compared.
A.C. Phillips, F. Roig, J. Ros
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Physical Review, 1963
To check the predictions of a universal Fermi interaction, negative muons were brought to rest in a 1\textonehalf{}-in. filament scintillator chamber and the rate for the reaction ${\ensuremath{\mu}}^{\ensuremath{-}}+{\mathrm{C}}^{12}\ensuremath{\rightarrow}{\mathrm{B}}^{12}+\ensuremath{\nu}$ was measured.
G. T. Reynolds +4 more
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To check the predictions of a universal Fermi interaction, negative muons were brought to rest in a 1\textonehalf{}-in. filament scintillator chamber and the rate for the reaction ${\ensuremath{\mu}}^{\ensuremath{-}}+{\mathrm{C}}^{12}\ensuremath{\rightarrow}{\mathrm{B}}^{12}+\ensuremath{\nu}$ was measured.
G. T. Reynolds +4 more
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MUON CAPTURE IN HYDROGEN ISOTOPES
Nuclear Physics A, 1981Abstract After a survey of the phenomenology of muonic hydrogen atoms and molecules recent experiments at SIN are discussed, dealing with muonic atoms and molecules in deuterium. These experiments could clarify the longstanding problem of hyperfine populations of muonic deuterium atoms.
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Physical Review, 1963
By exploiting the transfer process $({\ensuremath{\mu}}^{\ensuremath{-}}p)+\mathrm{Ne}\ensuremath{\rightarrow}p+({\ensuremath{\mu}}^{\ensuremath{-}}\mathrm{Ne})$, we have measured the disappearance rate of negative muons bound to neon nuclei. We find $\ensuremath{\lambda}=(0.658\ifmmode\pm\else\textpm\fi{}0.010)\ifmmode\times\else\texttimes\fi{}{10}^{6}
J. L. Rosen +6 more
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By exploiting the transfer process $({\ensuremath{\mu}}^{\ensuremath{-}}p)+\mathrm{Ne}\ensuremath{\rightarrow}p+({\ensuremath{\mu}}^{\ensuremath{-}}\mathrm{Ne})$, we have measured the disappearance rate of negative muons bound to neon nuclei. We find $\ensuremath{\lambda}=(0.658\ifmmode\pm\else\textpm\fi{}0.010)\ifmmode\times\else\texttimes\fi{}{10}^{6}
J. L. Rosen +6 more
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International Journal of Modern Physics E, 1999
Muon capture in deuterium, μ-+ D →νμ+n+n, is a weak process of fundamental importance. The capture rate depends critically on the spin configuration of the initial (μ D ) state, which is in turn related closely to the availability of having two nearby deuteron nuclei.
W.-Y. P. HWANG, B.-J. LIN
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Muon capture in deuterium, μ-+ D →νμ+n+n, is a weak process of fundamental importance. The capture rate depends critically on the spin configuration of the initial (μ D ) state, which is in turn related closely to the availability of having two nearby deuteron nuclei.
W.-Y. P. HWANG, B.-J. LIN
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