Fermi Transition
Fermi Transition is a type of beta decay process in nuclear physics wherein the emitted electron and antineutrino (or positron and neutrino) carry away no orbital angular momentum, characterized by the conservation of total angular momentum and parity with the nuclear spin transition occurring between states of the same orbital configuration and total angular momentum change ΔJ = 0, distinguishing it from Gamow-Teller transitions which involve spin-flip and allow ΔJ = 0, ±1 (excluding 0→0).
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Variants
Fermi-type Transition
Parents
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Model for modulation doped field effect transistor
T. J. Drummond, H. Morkoç̌, K. Lee et al. · IEEE Electron Device Letters · 1982 · 206 citations
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University of Washington Applied Physics Laboratory, United States
2 publications · 28 citations
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Centre National de la Recherche Scientifique
Paris, France
7 h-index
21 publications
1.3K citations

Universidad Nacional de La Plata
La Plata, Argentina
5 h-index
9 publications
249 citations

Oak Ridge National Laboratory
Oak Ridge, United States
4 h-index
8 publications
794 citations
Michigan State University
East Lansing, United States
4 h-index
26 publications
911 citations

Chinese Academy of Sciences
Beijing, China
4 h-index
27 publications
1K citations
Institute of Physics
Warsaw, Poland
4 h-index
7 publications
117 citations
California Institute of Technology
Pasadena, United States
3 h-index
7 publications
1K citations
The University of Osaka
Osaka, Japan
3 h-index
11 publications
137 citations
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PRC · 8 publications · 361 citations
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PRB · 5 publications · 338 citations
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5 publications · 180 citations
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4 publications · 103 citations
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4 publications · 175 citations
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