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Volumn 39, Issue 12, 1989, Pages 8169-8174

Nonlocal resistance and magnetoresistance in bulk metals

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EID: 35949011334     PISSN: 01631829     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevB.39.8169     Document Type: Article
Times cited : (3)

References (36)
  • 6
    • 0000252640 scopus 로고
    • Examples of weak localization and Aharanov Bohm oscillations in metallic cylinders are found in D. Yu Sharvin and, JETP Lett., 34, 272, 8, 718, N. B. Brandt, et al., Fiz. Nizk. Temp.
    • (1981) Pis'ma Zh. Eksp. Teor. Fiz. , vol.34 , pp. 285
    • Sharvin, Yu V.1
  • 15
    • 0000238514 scopus 로고
    • Universal conductance fluctuations in silicon inversion-layer nanostructures
    • Finally, see also the excellent review by, 26, 1926, R. A. Webb, et al., Jpn. J Appl. Phys.
    • (1986) Physical Review Letters , vol.56 , pp. 2865
    • Skoçpol, W.J.1
  • 19
    • 84931517994 scopus 로고    scopus 로고
    • Commercial SQUID from B.T.I.
  • 20
    • 84931517993 scopus 로고    scopus 로고
    • Empirical values of ρb lb for aluminum, taken from size effect experiments, vary from 5 times 10-12 to 14 times 10-12 Ω ^ cm2. We have chosen a typical value, in the middle of the range. See Jack Bass, Landolt-Börnstein, Numerical Data and Functional Relationships in Science and Technology, Group III (Springer-Verlag, Berlin, 1982), Vol. 15a;
  • 24
    • 84931517992 scopus 로고    scopus 로고
    • Data represented in Figs. 2(a) and 3(c) had larger baseline deviations, on a day-to-day basis, of a few nOMEGA.
  • 25
    • 84931517999 scopus 로고    scopus 로고
    • The amplitude can vary by a factor of 3 over the full angular range of 180degr. The amplitudes presented in Fig. 4(a) are from orientations within 20degr of perpendicular field.
  • 26
    • 84931517983 scopus 로고
    • We have used ρb lb = 9 times 10-12 Ω ^ cm2, and Fickett's measured values of ρb (T) for bulk aluminum with an RRR of 2000, which is essentially the same as the deduced value of RRR (1900) for our aluminum (after processing). Between data points, ρb (T) is fit to the form ρ (T) = ρ0 + ρ1 T3, as suggested by the author. See
    • (1971) Phys. Rev. B , vol.2 , pp. 1943
    • Fickett, F.R.1
  • 28
    • 84931517982 scopus 로고    scopus 로고
    • see Table IV.
  • 29
    • 84931517989 scopus 로고    scopus 로고
    • See, for example, D. A. Wharam et al. in Ref. 1.
  • 32
    • 84931517988 scopus 로고    scopus 로고
    • see Fig. 5.
  • 36
    • 84931517991 scopus 로고    scopus 로고
    • Mark Johnson, Ph.D. dissertation, Cornell University, Ithaca, NY (1986).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.