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Volumn 59, Issue 5, 1999, Pages 3385-3387

Pressure effect on quasi-one-dimensional charge transport in (formula presented) magnetotransport study

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EID: 16644393665     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.3385     Document Type: Article
Times cited : (1)

References (17)
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    • Y. Yamada, et al., Physica C 231, 131 (1994).
    • (1994) Physica C , vol.231 , pp. 131
    • Yamada, Y.1
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    • (unpublished)
    • T. Tatsumi et al., (unpublished).
    • Tatsumi, T.1
  • 11
    • 85038950891 scopus 로고    scopus 로고
    • For a review, S. Kagoshima, H. Nagasawa, and T. Sambongi, One-Dimensional Conductors (Springer-Verlag, Berlin, 1988)
    • For a review, S. Kagoshima, H. Nagasawa, and T. Sambongi, One-Dimensional Conductors (Springer-Verlag, Berlin, 1988).
  • 14
    • 85038920058 scopus 로고    scopus 로고
    • To our knowledge, no one has succeeded in preparing single crystals of Pr124 at present
    • To our knowledge, no one has succeeded in preparing single crystals of Pr124 at present.
  • 15
    • 85038961297 scopus 로고    scopus 로고
    • We also measured MR in a longitudinal configuration (Formula presented) to check whether MR is isotropic or not and found that longitudinal MR is smaller in magnitude than transverse MR. This indicates MR is anisotropic, which is consistent with our assignment that the observed MR is classical
    • We also measured MR in a longitudinal configuration (Formula presented) to check whether MR is isotropic or not and found that longitudinal MR is smaller in magnitude than transverse MR. This indicates MR is anisotropic, which is consistent with our assignment that the observed MR is classical.
  • 17
    • 85038895177 scopus 로고    scopus 로고
    • One may notice that for the MR data at 5 and 10 K shown in Figs. 33(a) and 33(b), there is a sharp raise of MR near (Formula presented) followed by an (Formula presented) law. This may arise from the AF order of Pr moments because it is not observed for the data above 20 K
    • One may notice that for the MR data at 5 and 10 K shown in Figs. 33(a) and 33(b), there is a sharp raise of MR near (Formula presented) followed by an (Formula presented) law. This may arise from the AF order of Pr moments because it is not observed for the data above 20 K.


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