1978
DOI: 10.1016/0038-1098(78)90785-8
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Interpretation of acceptor spectra in semiconductors

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Cited by 137 publications
(43 citation statements)
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“…A unique feature of the foregoing discussion is the assignment of the first excited state manifold of the exciton to an electron-hole pair involving a r7 hole. There is considerable theoretical support for the existence of a low-lying r: state for effective mass acceptors in silicon (Lipari and Baldereschi 1978). Raman scattering studies in boron-doped silicon by Wright and Mooradian (1967) and Cherlow et a1 (1973) and infrared absorption studies by Chandrasekhar etal (1973) provide experimental evidence for the existence of this state.…”
Section: Discussionmentioning
confidence: 96%
“…A unique feature of the foregoing discussion is the assignment of the first excited state manifold of the exciton to an electron-hole pair involving a r7 hole. There is considerable theoretical support for the existence of a low-lying r: state for effective mass acceptors in silicon (Lipari and Baldereschi 1978). Raman scattering studies in boron-doped silicon by Wright and Mooradian (1967) and Cherlow et a1 (1973) and infrared absorption studies by Chandrasekhar etal (1973) provide experimental evidence for the existence of this state.…”
Section: Discussionmentioning
confidence: 96%
“…Applying this classification scheme, all observed transitions originate from the P + acceptor ground state. The G-, D-and Blines were attributed to r s end states, whereas the C-line is due to two excited states, F s and P~-, being energetically very close [10]. The A-and/-lines are actually groups of 4 and 8 lines at B = 0 T, respectively.…”
Section: Resultsmentioning
confidence: 92%
“…The local symmetry of an acceptor on a Ge lattice site corresponds to the point group Td. In the effective mass approximation however, the small terms in the impurity potential being non-symmetric against inversion are neglected and the acceptor states are characterised by double group representation of the octahedral groups Oh, having definite parity [10]. Applying this classification scheme, all observed transitions originate from the P + acceptor ground state.…”
Section: Resultsmentioning
confidence: 99%
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“…1 (a) in a frequency range between 45 and 200 cm -1. The observed lines are due to photothermal ionization caused by transitions from the 1Sa/~ (F +) acceptor 18 ground state to excited states below the valence band edge [9]. The labelling of the lines in Fig.…”
Section: [8]mentioning
confidence: 97%