Journal of the Korean Physical Society

, Volume 63, Issue 3, pp 571–574 | Cite as

Specific-heat study on successive magnetic transitions in α-Dy2S3 single crystals under magnetic fields

Article

Abstract

Specific-heat measurements in magnetic fields have been performed on α-Dy2S3 single crystals and have shown successive magnetic transitions at \(T_{N_1 } = 11.4 K\) and \(T_{N_2 } = 6.4 K\). The specific heat in no magnetic field exhibits sharp peaks at both \(T_{N_1 }\) and \(T_{N_2 }\). The change in the magnetic entropy across each transition is estimated as Rln2/2 per mol-Dy, which suggests magnetic moments on only one Dy site between two crystallographically inequivalent Dy sites order at each transition temperature. When the magnetic field is applied along the b-axis of the orthorhombic system, the two peaks of the specific heat shift toward lower temperatures. On the other hand, a magnetic field perpendicular to the b-axis shifts the peaks toward higher temperatures. The \(T_{N_1 }\) shifts to 9.6 K (Hb) and 12.5 K (Hb) under a magnetic field of 2 T. The \(T_{N_2 }\) peak broadens gradually with increasing magnetic field for each direction; consequently, the peak is obscure under a field of 2 T.

Keywords

Rare-earth sulfides Specific heat Successive magnetc transitions Magnetic entropy 

Preview

Unable to display preview. Download preview PDF.

Unable to display preview. Download preview PDF.

References

  1. [1]
    S. Ebisu, Y. Iijima, T. Iwasa and S. Nagata, J. Phys. Chem. Solids 65, 1113 (2004).ADSCrossRefGoogle Scholar
  2. [2]
    A. Kikkawa, K. Katsumata, S. Ebisu and S. Nagata, J. Phys. Soc. Jpn. 73, 2955 (2004).ADSCrossRefGoogle Scholar
  3. [3]
    M. Matsuda, A. Kikkawa, K. Katsumata, S. Ebisu and S. Nagata, J. Phys. Soc. Jpn. 74, 1412 (2005).ADSCrossRefGoogle Scholar
  4. [4]
    K. Katsumata, A. Kikkawa, Y. Tanaka, S. Shimomura, S. Ebisu and S. Nagata, J. Phys. Soc. Jpn. 74, 1598 (2005).ADSCrossRefGoogle Scholar
  5. [5]
    S. Ebisu, M. Gorai, K. Maekawa and S. Nagata, AIP Conf. Proc. 850, 1237 (2006).ADSCrossRefGoogle Scholar
  6. [6]
    M. Matsuda, K. Kakurai, S. Ebisu and S. Nagata, J. Phys. Soc. Jpn. 75, 074710 (2006).ADSCrossRefGoogle Scholar
  7. [7]
    S. Ebisu, M. Narumi, M. Gorai and S. Nagata, J. Magn. Magn. Mater. 310, 1741 (2007).ADSCrossRefGoogle Scholar
  8. [8]
    S. Ebisu, M. Narumi and S. Nagata, J. Phys. Soc. Jpn. 75, 085002 (2006).ADSCrossRefGoogle Scholar
  9. [9]
    S. Ebisu, K. Koyama, H. Omote and S. Nagata, J. Phys.: Conf. Ser. 150, 042027 (2009).ADSCrossRefGoogle Scholar
  10. [10]
    S. Ebisu, H. Omote and S. Nagata, J. Phys.: Conf. Ser. 200, 092005 (2010).ADSCrossRefGoogle Scholar
  11. [11]
    C. T. Prewitt and A. W. Sleight, Inorg. Chem. 7, 1090 (1968).CrossRefGoogle Scholar
  12. [12]
    A. Aruga, S. Tsujimi and I. Nakai, Anal. Sci. 12, 151 (1996).CrossRefGoogle Scholar
  13. [13]
    K. A. Gschneidner, Jr., B. J. Beaudry, T. Takeshita and S. S. Eucker, Phys. Rev. B 24, 7187 (1981).ADSCrossRefGoogle Scholar
  14. [14]
    Details of the specific heat of α-R 2 S 3 (R = Sm and Tb) will be given elsewhere.Google Scholar

Copyright information

© The Korean Physical Society 2013

Authors and Affiliations

  1. 1.Division of Applied SciencesMuroran Institute of TechnologyMuroranJapan

Personalised recommendations