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Volumn 60, Issue 4, 1999, Pages 2292-2298

Conductivity of metallic si:b near the metal-insulator transition: comparison between unstressed and uniaxially stressed samples

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EID: 4244186079     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.60.2292     Document Type: Article
Times cited : (5)

References (41)
  • 20
    • 0004032705 scopus 로고
    • C. N. Rao Taylor and Francis, London P. P. Edwards
    • For a review, see M. P. Sarachik, in Metal-Insulator Transitions Revisited, edited by P. P. Edwards and C. N. Rao (Taylor and Francis, London, 1995).
    • (1995) Metal-Insulator Transitions Revisited
    • Sarachik, M.P.1
  • 28
    • 85037913637 scopus 로고    scopus 로고
    • S. Bogdanovich, Ph.D. thesis, City College of CUNY, 1998.
    • S. Bogdanovich, Ph.D. thesis, City College of CUNY, 1998.
  • 31
    • 0021502767 scopus 로고
    • A (Formula presented) dependence of the conductivity at the critical value of the tuning parameter has been calculated for the case with strong spin-orbit scattering by C. Castellani, C. Di Castro, G. Forgacs, and S. Sorella, Solid State Commun. 52, 261 (1984).
    • (1984) Solid State Commun. , vol.52 , pp. 261
    • Castellani, C.1    Di Castro, C.2    Forgacs, G.3    Sorella, S.4
  • 32
    • 85037888135 scopus 로고    scopus 로고
    • Data for the stress closest to the critical value (Formula presented) were not included in the fit. The slope (Formula presented) for the (Formula presented) curve is smaller and atypical, due possibly to inhomogeneous distribution of stress resulting in insulating behavior for some regions of the sample.
    • Data for the stress closest to the critical value (Formula presented) were not included in the fit. The slope (Formula presented) for the (Formula presented) curve is smaller and atypical, due possibly to inhomogeneous distribution of stress resulting in insulating behavior for some regions of the sample.
  • 33
    • 85037890579 scopus 로고    scopus 로고
    • A somewhat better fit is obtained using (Formula presented) This represents the uncertainty associated with the present analysis.
    • A somewhat better fit is obtained using (Formula presented) This represents the uncertainty associated with the present analysis.
  • 38
  • 39
    • 4243944881 scopus 로고
    • ) and references to N. F. Mott and to A. B. Harris therein.
    • J. Chayes, L. Chayes, D. S. Fisher, and T. Spencer, Phys. Rev. Lett. 57, 2999 (1987) and references to N. F. Mott and to A. B. Harris therein.
    • (1987) Phys. Rev. Lett. , vol.57 , pp. 2999
    • Chayes, J.1    Chayes, L.2    Fisher, D.S.3    Spencer, T.4
  • 40
    • 85037880028 scopus 로고    scopus 로고
    • (private communication).
    • G. Zimanyi (private communication).
    • Zimanyi, G.1
  • 41
    • 4243611070 scopus 로고    scopus 로고
    • It should also be mentioned that the exponent for the Anderson localization transition for noninteracting electrons in three dimensions is also close to 1.6 [see, e.g., K. Slevin and T. Ohtsuki, Phys. Rev. Lett. 78, 4083 (1997)]. However, there is considerable evidence for electron interaction effects in both the insulating and metallic phases in Si:B; see, for example, Ref. 18.
    • (1997) Phys. Rev. Lett. , vol.78 , pp. 4083
    • Slevin, K.1    Ohtsuki, T.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.