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Volumn 90, Issue 20, 2003, Pages

Observation of a liquid-gas-type transition in the pyrochlore spin ice compound Dy2Ti2O7 in a magnetic field

Author keywords

[No Author keywords available]

Indexed keywords

MAGNETIC FIELD EFFECTS; MAGNETIC HYSTERESIS; MAGNETIC VARIABLES MEASUREMENT; MAGNETIZATION; NUMERICAL ANALYSIS; PHASE DIAGRAMS; PHASE TRANSITIONS; SPECIFIC HEAT;

EID: 0037789426     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: None     Document Type: Article
Times cited : (173)

References (24)
  • 10
    • 0037750138 scopus 로고    scopus 로고
    • cond-mat/0107414
    • T. Fennell et al., cond-mat/0107414.
    • Fennell, T.1
  • 15
    • 0038426471 scopus 로고    scopus 로고
    • (to be published)
    • R. Higashinaka et al., (to be published).
    • Higashinaka, R.1
  • 19
    • 85088488245 scopus 로고    scopus 로고
    • note
    • cr becomes ∼ 0.18 K.
  • 20
    • 0037750137 scopus 로고    scopus 로고
    • note
    • At low temperatures, the magnetization is so large that we further made a demagnetizing field corection using a demagnetizing factor of -0.08 obtained for an oblate ellipsoid with the aspect ratio of 8 [R. M. Bozorth, Ferromagnetism (D. van Nostrand Co., New York, 1951).] The basic features of the present data are, however, free from this correction.
  • 22
    • 85088492519 scopus 로고    scopus 로고
    • note
    • c shown in Fig. 4 is slightly higher than those data in Fig. 3.
  • 23
    • 4243423438 scopus 로고
    • note
    • A phase transition that does not involve a symmetry change should always be of first order. In a magnetic system, the magnetization then becomes discontinuous and the differential susceptibility diverges as the critical point is approached from above [M. E. Fisher and A. N. Berker, Phys. Rev. B 26, 2507 (1982)].
    • (1982) Phys. Rev. B , vol.26 , pp. 2507
    • Fisher, M.E.1    Berker, A.N.2
  • 24
    • 0038764393 scopus 로고    scopus 로고
    • note
    • Ising ferromagnet is known to show a phase diagram of liquid-gas type, with a line of the first-order transition along the H = 0 line. In that case the analogy is purely on symmetry, and no latent heat is expected across the first-order transition because the phase boundary is parallel to the temperature axis.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.