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Volumn 145, Issue 1-4, 2006, Pages 209-218

Decay of quantized vortices in quantum turbulence

Author keywords

[No Author keywords available]

Indexed keywords

ENERGY DISSIPATION; LOW TEMPERATURE EFFECTS; NUMERICAL ANALYSIS; QUANTUM THEORY; VORTEX FLOW;

EID: 33845770734     PISSN: 00222291     EISSN: 15737357     Source Type: Journal    
DOI: 10.1007/s10909-006-9245-1     Document Type: Article
Times cited : (9)

References (23)
  • 2
    • 0003190105 scopus 로고
    • ibid. A 240, 128 (1957); ibid. A 240, 493 (1957)
    • Vinen W.F., Proc. Roy. Soc. A 240, 114 (1957); ibid. A 240, 128 (1957); ibid. A 240, 493 (1957).
    • (1957) Proc. Roy. Soc. A , vol.240 , pp. 114
    • Vinen, W.F.1
  • 3
    • 77956959547 scopus 로고
    • in C. J. Gorter (ed.), North-Holland, Ameterdam
    • Tough J.T., in Progress in Low Temperature Physics, Vol. VIII, C. J. Gorter (ed.), North-Holland, Ameterdam (1955), p. 133.
    • (1955) Progress in Low Temperature Physics , vol.8 , pp. 133
    • Tough, J.T.1
  • 6
    • 0004185784 scopus 로고
    • Cambridge University Press, Cambridge
    • Frisch U., (1995). Turbulence. Cambridge University Press, Cambridge
    • (1995) Turbulence
    • Frisch, U.1
  • 8
    • 33845747900 scopus 로고    scopus 로고
    • Equation (1) neglects the intermittency of turbulence. In this work, we does not discuss the intermittency in both classical and quantum turbulence
    • Equation (1) neglects the intermittency of turbulence. In this work, we does not discuss the intermittency in both classical and quantum turbulence.
  • 22
    • 45849155586 scopus 로고    scopus 로고
    • The proportional coefficient α(ζ) is closely related with the vortex length distribution n (ζ) throughout α(ζ) = ζ n (ζ) / L and ∫ d ζ: α(ζ) = 1. The behavior of n (ζ) in quantum turbulence was already discussed by Araki et al. in with using the vortex-filament model. They reported n (ζ) to be some power-law functions of ζ because of the self-similarity, and we can, therefore, expect some power-low structure of α(ζ) from the above equations
    • The proportional coefficient α(ζ) is closely related with the vortex length distribution n (ζ) throughout α(ζ) = ζ n (ζ) / L and ∫ d ζ: α(ζ) = 1. The behavior of n (ζ) in quantum turbulence was already discussed by Araki et al. in T. Araki, M. Tsubota and S. Nemirovskii, Phys. Rev. Lett. 89 145301 (2002) with using the vortex-filament model. They reported n (ζ) to be some power-law functions of ζ because of the self-similarity, and we can, therefore, expect some power-low structure of α(ζ) from the above equations.
    • (2002) Phys. Rev. Lett. , vol.89 , pp. 145301
    • Araki, T.1    Tsubota, M.2    Nemirovskii, S.3


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.