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Volumn 79, Issue 17, 2009, Pages

Comment on "low-temperature phonon thermal conductivity of single-crystalline Nd2 CuO4: Effects of sample size and surface roughness"

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EID: 65649092190     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.176501     Document Type: Article
Times cited : (18)

References (23)
  • 2
    • 32644483694 scopus 로고    scopus 로고
    • Electronic inhomogeneity and breakdown of the universal thermal conductivity of cuprate superconductors
    • DOI 10.1103/PhysRevLett.96.017008
    • X. F. Sun, S. Ono, Y. Abe, S. Komiya, K. Segawa, and Y. Ando, Phys. Rev. Lett. 96, 017008 (2006). 10.1103/PhysRevLett.96.017008 (Pubitemid 43248394)
    • (2006) Physical Review Letters , vol.96 , Issue.1 , pp. 017008
    • Sun, X.F.1    Ono, S.2    Abe, Y.3    Komiya, S.4    Segawa, K.5    Ando, Y.6
  • 4
    • 0037758325 scopus 로고
    • 10.1103/PhysRev.186.801
    • W. S. Hurst and D. R. Frankl, Phys. Rev. 186, 801 (1969). 10.1103/PhysRev.186.801
    • (1969) Phys. Rev. , vol.186 , pp. 801
    • Hurst, W.S.1    Frankl, D.R.2
  • 5
    • 0038772744 scopus 로고
    • 10.1103/PhysRevB.25.3608
    • R. O. Pohl and B. Stritzker, Phys. Rev. B 25, 3608 (1982). 10.1103/PhysRevB.25.3608
    • (1982) Phys. Rev. B , vol.25 , pp. 3608
    • Pohl, R.O.1    Stritzker, B.2
  • 6
    • 0001587261 scopus 로고
    • 10.1103/PhysRev.156.975
    • P. D. Thacher, Phys. Rev. 156, 975 (1967). 10.1103/PhysRev.156.975
    • (1967) Phys. Rev. , vol.156 , pp. 975
    • Thacher, P.D.1
  • 12
    • 65649141156 scopus 로고    scopus 로고
    • In Nd2 CuO4, one cannot use very low-temperature specific-heat data for analyzing the phonon term because of the appearance of a magnetic peak, so in Ref. the β value was obtained from the simple fitting of T3 to the data at intermediate temperature. It is known that in the temperature range 0.02
    • In Nd2 CuO4, one cannot use very low-temperature specific-heat data for analyzing the phonon term because of the appearance of a magnetic peak, so in Ref. the β value was obtained from the simple fitting of T3 to the data at intermediate temperature. It is known that in the temperature range 0.02
  • 14
    • 0033689586 scopus 로고    scopus 로고
    • This formula is commonly used for analyzing the phonon specific heat at this intermediate temperature range. [See, for example, the papers on the specific heat of La2 CuO4; 10.1103/PhysRevLett.84.5612;
    • This formula is commonly used for analyzing the phonon specific heat at this intermediate temperature range. [See, for example, the papers on the specific heat of La2 CuO4; C. F. Chang, J. Y. Lin, and H. D. Yang, Phys. Rev. Lett. 84, 5612 (2000) 10.1103/PhysRevLett.84.5612
    • (2000) Phys. Rev. Lett. , vol.84 , pp. 5612
    • Chang, C.F.1    Lin, J.Y.2    Yang, H.D.3
  • 16
    • 65649118103 scopus 로고    scopus 로고
    • It is important to recognize that the correction to the simple T3 analysis can decrease the β value, but it can never change the β value by as much as a factor of two, as can be seen in these reference papers. More importantly, if the specific-heat data in the intermediate temperature range can still be well fitted to the simple T3 law, which is actually the case for Nd2 CuO4, it means that the higher-power terms are effectively negligible in this material. (In Ref., the T3 law fits the data well from ∼15 to 25 K or even higher temperature.) This is not surprising, because the higher-power term β5 is usually found to be a small positive value in La2 CuO4, but it can even be a small negative value in some other materials [e.g., see the data for Nax CoO2;
    • It is important to recognize that the correction to the simple T3 analysis can decrease the β value, but it can never change the β value by as much as a factor of two, as can be seen in these reference papers. More importantly, if the specific-heat data in the intermediate temperature range can still be well fitted to the simple T3 law, which is actually the case for Nd2 CuO4, it means that the higher-power terms are effectively negligible in this material. (In Ref., the T3 law fits the data well from ∼15 to 25 K or even higher temperature.) This is not surprising, because the higher-power term β5 is usually found to be a small positive value in La2 CuO4, but it can even be a small negative value in some other materials [e.g., see the data for Nax CoO2
  • 17
    • 0001571997 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.60.10580;
    • Y. Ando, Phys. Rev. B 60, 10580 (1999)] 10.1103/PhysRevB.60.10580
    • (1999) Phys. Rev. B , vol.60 , pp. 10580
    • Ando, Y.1
  • 18
    • 65649154013 scopus 로고    scopus 로고
    • Also, it is useful to note that one can neglect the possibility that the β value determined at 15-25 K for Nd2 CuO4 might be enhanced by a magnon contribution, because it is established that in the Néel state of Nd2 CuO4, Cu magnons (which are the only possibility at 15-25 K) are gapped although it is still an open question whether the Nd magnons (which can only be relevant below 3 K) are gapped as well (Ref.).
    • Also, it is useful to note that one can neglect the possibility that the β value determined at 15-25 K for Nd2 CuO4 might be enhanced by a magnon contribution, because it is established that in the Néel state of Nd2 CuO4, Cu magnons (which are the only possibility at 15-25 K) are gapped although it is still an open question whether the Nd magnons (which can only be relevant below 3 K) are gapped as well (Ref.).
  • 19
    • 0001174548 scopus 로고
    • While the averaged sound velocity v̄ is a rather complicated average over all acoustic branches in all directions, this issue was carefully studied by Casimir and has been well sorted out; 10.1016/S0031-8914(38)80162-2
    • While the averaged sound velocity v̄ is a rather complicated average over all acoustic branches in all directions, this issue was carefully studied by Casimir and has been well sorted out; H. B. G. Casimir, Physica (Amsterdam) 5, 495 (1938). 10.1016/S0031-8914(38)80162-2
    • (1938) Physica (Amsterdam) , vol.5 , pp. 495
    • Casimir, H.B.G.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.