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Volumn 10, Issue C, 1975, Pages 1-89

Chapter 1 Low-Field Electron Transport

(1)  Rode, D L a  

a NONE

Author keywords

[No Author keywords available]

Indexed keywords

ELECTRON TRANSPORT; LOW FIELD;

EID: 0002531092     PISSN: 00808784     EISSN: None     Source Type: Book Series    
DOI: 10.1016/S0080-8784(08)60331-2     Document Type: Article
Times cited : (320)

References (245)
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    • Anisotropy of the Shubnikov-deHaas frequency has been applied for this purpose by
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    • One of the more careful experimental tests of Eq. (22) can be found in the following reference, which, although it does not confirm the dilatation model rigorously, indicates only small departures for our present purposes, See also Part V.
    • Eaves, L., Stradling, R.A., Askenazy, S., Leotin, J., Portal, J.C., Ulmet, J.P., J. Phys. C Solid State Phys., 4, 1971, L42 One of the more careful experimental tests of Eq. (22) can be found in the following reference, which, although it does not confirm the dilatation model rigorously, indicates only small departures for our present purposes, See also Part V.
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    • personal communication. Note the insensitivity of high-field electron transport to the assumed value of the γ1c to L1c separation.
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    • 150 these results are not extended above room temperature where satisfactory agreement is more difficult to achieve.
    • 150 these results are not extended above room temperature where satisfactory agreement is more difficult to achieve.
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    • unpublished.
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    • 160 in Table I. For example, the effective mass and polaron mass are found to be 0.2 m and 0.216 m, whereas the polaron mass estimated in Table I is 0.218 m.
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    • 15 indicates agreement between experimental and theoretical Hall factor to within 1% when nonuniformities are minimized.
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    • 2/V-sec for mag netic fields from 0.1 to 7.0 kG on their highest purity sample. These results are consistent with the assumption of uniform doping.
    • 2/V-sec for mag netic fields from 0.1 to 7.0 kG on their highest purity sample. These results are consistent with the assumption of uniform doping.
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    • Values quoted in the former work are questioned but seemingly unresolved in the latter.
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    • 215 in terms of intervalley scattering by emission of a 59-meV TO phonon near X rather than a 47.4-meV phonon. Use of the TO phonon in the present work would shift the knee of the curve in Fig. 29 from near 130 to near 160°K. High-purity mobility given here agrees within a few percent with Fig. 29.
    • 215 in terms of intervalley scattering by emission of a 59-meV TO phonon near X rather than a 47.4-meV phonon. Use of the TO phonon in the present work would shift the knee of the curve in Fig. 29 from near 130 to near 160°K. High-purity mobility given here agrees within a few percent with Fig. 29.
    • (1973) Phys. Rev. B , vol.8 , pp. 5632
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    • private communication.
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    • also report mobility in highpurity Ge.
    • Norton, P., Levinstein, H., Phys. Rev. B, 6, 1972, 470 also report mobility in highpurity Ge.
    • (1972) Phys. Rev. B , vol.6 , pp. 470
    • Norton, P.1    Levinstein, H.2


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