Spin-flip acceptor scattering in ZnTe

Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Toms, D. J. Helms, C. A. Scott, J. F.

Format:	E-Artikel

Erschienen:	1978

Umfang:	Online-Ressource 4

Reproduktion:	APS Digital Backfile Archive 1893-2003
Übergeordnetes Werk:	Enthalten in: Physical review / B - College Park, Md. : APS, 1970, 18(1978), 2, Seite 871-874
Übergeordnetes Werk:	volume:18 ; year:1978 ; number:2 ; pages:871-874 ; extent:4

Links:	Link aufrufen

Katalog-ID:	NLEJ249604183

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520			\|a Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center.
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allfields	(DE-627)NLEJ249604183 (DE-601)aps:dcb18713d5d8553609b774d9bcf7c55152a73235 DE-627 ger DE-627 rakwb Spin-flip acceptor scattering in ZnTe 1978 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center. APS Digital Backfile Archive 1893-2003 Toms, D. J. oth Helms, C. A. oth Scott, J. F. oth Enthalten in Physical review / B College Park, Md. : APS, 1970 18(1978), 2, Seite 871-874 Online-Ressource (DE-627)NLEJ248237845 (DE-600)1473011-X 1550-235X nnns volume:18 year:1978 number:2 pages:871-874 extent:4 https://www.tib.eu/de/suchen/id/aps%3Adcb18713d5d8553609b774d9bcf7c55152a73235 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 18 1978 2 871-874 4
spelling	(DE-627)NLEJ249604183 (DE-601)aps:dcb18713d5d8553609b774d9bcf7c55152a73235 DE-627 ger DE-627 rakwb Spin-flip acceptor scattering in ZnTe 1978 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center. APS Digital Backfile Archive 1893-2003 Toms, D. J. oth Helms, C. A. oth Scott, J. F. oth Enthalten in Physical review / B College Park, Md. : APS, 1970 18(1978), 2, Seite 871-874 Online-Ressource (DE-627)NLEJ248237845 (DE-600)1473011-X 1550-235X nnns volume:18 year:1978 number:2 pages:871-874 extent:4 https://www.tib.eu/de/suchen/id/aps%3Adcb18713d5d8553609b774d9bcf7c55152a73235 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 18 1978 2 871-874 4
allfields_unstemmed	(DE-627)NLEJ249604183 (DE-601)aps:dcb18713d5d8553609b774d9bcf7c55152a73235 DE-627 ger DE-627 rakwb Spin-flip acceptor scattering in ZnTe 1978 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center. APS Digital Backfile Archive 1893-2003 Toms, D. J. oth Helms, C. A. oth Scott, J. F. oth Enthalten in Physical review / B College Park, Md. : APS, 1970 18(1978), 2, Seite 871-874 Online-Ressource (DE-627)NLEJ248237845 (DE-600)1473011-X 1550-235X nnns volume:18 year:1978 number:2 pages:871-874 extent:4 https://www.tib.eu/de/suchen/id/aps%3Adcb18713d5d8553609b774d9bcf7c55152a73235 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 18 1978 2 871-874 4
allfieldsGer	(DE-627)NLEJ249604183 (DE-601)aps:dcb18713d5d8553609b774d9bcf7c55152a73235 DE-627 ger DE-627 rakwb Spin-flip acceptor scattering in ZnTe 1978 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center. APS Digital Backfile Archive 1893-2003 Toms, D. J. oth Helms, C. A. oth Scott, J. F. oth Enthalten in Physical review / B College Park, Md. : APS, 1970 18(1978), 2, Seite 871-874 Online-Ressource (DE-627)NLEJ248237845 (DE-600)1473011-X 1550-235X nnns volume:18 year:1978 number:2 pages:871-874 extent:4 https://www.tib.eu/de/suchen/id/aps%3Adcb18713d5d8553609b774d9bcf7c55152a73235 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 18 1978 2 871-874 4
allfieldsSound	(DE-627)NLEJ249604183 (DE-601)aps:dcb18713d5d8553609b774d9bcf7c55152a73235 DE-627 ger DE-627 rakwb Spin-flip acceptor scattering in ZnTe 1978 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center. APS Digital Backfile Archive 1893-2003 Toms, D. J. oth Helms, C. A. oth Scott, J. F. oth Enthalten in Physical review / B College Park, Md. : APS, 1970 18(1978), 2, Seite 871-874 Online-Ressource (DE-627)NLEJ248237845 (DE-600)1473011-X 1550-235X nnns volume:18 year:1978 number:2 pages:871-874 extent:4 https://www.tib.eu/de/suchen/id/aps%3Adcb18713d5d8553609b774d9bcf7c55152a73235 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 18 1978 2 871-874 4
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title_sort	spin-flip acceptor scattering in znte
title_auth	Spin-flip acceptor scattering in ZnTe
abstract	Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center.
abstractGer	Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center.
abstract_unstemmed	Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center.
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up_date	2024-07-06T05:08:25.266Z
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fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">NLEJ249604183</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20231114102310.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">231114s1978 xx \|\|\|\|\|o 00\| \|\|und c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ249604183</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-601)aps:dcb18713d5d8553609b774d9bcf7c55152a73235</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Spin-flip acceptor scattering in ZnTe</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1978</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">4</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Two transitions have been observed in ZnTe: As and in ZnTe: P. These are interpreted as the -32→-12 and -32→+12 transitions of holes bound to the shallow arsenic and phosphorous acceptors. The deduced bound-hole gyromagnetic ratio is similar in each case: g12=0.61±0.04; g32=0.63±0.04 for ZnTe: P and g12=0.37±0.04 and g32=0.39±0.04 for ZnTe: As. These ZnTe: P values are in excellent agreement with the shallow acceptor g value gh=0.59±0.05 obtained by Dean et al. from luminescence Zeeman studies, but both As and P values are significantly smaller than the values for free holes obtained from theory (0.92 ± 0.15, Hollis) and experiment (0.9-1.1, Hollis and Scott, spin-flip scattering; 0.89 ± 0.10, Venghaus et al., magnetoreflectivity). The difference between free- and bound-hole g values is interpreted in terms of Hollis's valence-band theory for ZnTe, which shows that gh decreases with increasing wave vector near the Brillouin-zone center.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">APS Digital Backfile Archive 1893-2003</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Toms, D. J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Helms, C. A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Scott, J. F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Physical review / B</subfield><subfield code="d">College Park, Md. : APS, 1970</subfield><subfield code="g">18(1978), 2, Seite 871-874</subfield><subfield code="h">Online-Ressource</subfield><subfield code="w">(DE-627)NLEJ248237845</subfield><subfield code="w">(DE-600)1473011-X</subfield><subfield code="x">1550-235X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:18</subfield><subfield code="g">year:1978</subfield><subfield code="g">number:2</subfield><subfield code="g">pages:871-874</subfield><subfield code="g">extent:4</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://www.tib.eu/de/suchen/id/aps%3Adcb18713d5d8553609b774d9bcf7c55152a73235</subfield><subfield code="x">Verlag</subfield><subfield code="z">Deutschlandweit zugänglich</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-APS</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">18</subfield><subfield code="j">1978</subfield><subfield code="e">2</subfield><subfield code="h">871-874</subfield><subfield code="g">4</subfield></datafield></record></collection>
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Spin-flip acceptor scattering in ZnTe

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