-
1
-
-
0004185784
-
-
Cambridge University Press, Cambridge, England
-
U. Frisch, Turbulence (Cambridge University Press, Cambridge, England, 1995).
-
(1995)
Turbulence
-
-
Frisch, U.1
-
5
-
-
18144386182
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.94.065302
-
M. Kobayashi and M. Tsubota, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.94.065302 94, 065302 (2005).
-
(2005)
Phys. Rev. Lett.
, vol.94
, pp. 065302
-
-
Kobayashi, M.1
Tsubota, M.2
-
7
-
-
0036013593
-
-
RMPHAT. 0034-6861. 10.1103/RevModPhys.74.47
-
R. Albert and A. L. Barabási, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.74.47 74, 47 (2002).
-
(2002)
Rev. Mod. Phys.
, vol.74
, pp. 47
-
-
Albert, R.1
Barabási, A.L.2
-
8
-
-
0038483826
-
-
SCIEAS. 0036-8075. 10.1126/science.286.5439.509
-
A. L. Barabási and R. Albert, Science SCIEAS 0036-8075 10.1126/science.286.5439.509 286, 509 (1999).
-
(1999)
Science
, vol.286
, pp. 509
-
-
Barabási, A.L.1
Albert, R.2
-
9
-
-
32644489472
-
-
Nemirovskii recently discussed the same problem by formulating and analyzing the rate equation of the system [PRLTAO 0031-9007 10.1103/PhysRevLett. 96.015301
-
Nemirovskii recently discussed the same problem by formulating and analyzing the rate equation of the system [S. K. Nemirovskii, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.96.015301 96, 015301 (2006)]. The author succeeded in deriving the power law VLD with α=5 2 by considering only the situation in which there is no net flow of length in infinite l space. However, there must be net flow during the decay and the l space must be limited in real quantum turbulence. Therefore, more studies are eagerly anticipated to understand the emergence of the power-law VLD.
-
(2006)
Phys. Rev. Lett.
, vol.96
, pp. 015301
-
-
Nemirovskii, S.K.1
-
11
-
-
0242384605
-
-
For example, PRLTAO 0031-9007 10.1103/PhysRevLett.91.135301
-
For example, W. F. Vinen, M. Tsubota, and A. Mitani, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.91.135301 91, 135301 (2003).
-
(2003)
Phys. Rev. Lett.
, vol.91
, pp. 135301
-
-
Vinen, W.F.1
Tsubota, M.2
Mitani, A.3
-
12
-
-
0034818344
-
-
For example, PRLTAO 0031-9007 10.1103/PhysRevLett.86.1410
-
For example, M. Leadbeater, T. Winiecki, D. C. Samuels, C. F. Barenghi, and C. S. Adams, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.86.1410 86, 1410 (2001).
-
(2001)
Phys. Rev. Lett.
, vol.86
, pp. 1410
-
-
Leadbeater, M.1
Winiecki, T.2
Samuels, D.C.3
Barenghi, C.F.4
Adams, C.S.5
-
13
-
-
0037243703
-
-
PLRAAN 1050-2947 10.1103/PhysRevA.67.015601
-
M. Leadbeater, D. C. Samuels, C. F. Barenghi, and C. S. Adams, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.67.015601 67, 015601 (2003).
-
(2003)
Phys. Rev. a
, vol.67
, pp. 015601
-
-
Leadbeater, M.1
Samuels, D.C.2
Barenghi, C.F.3
Adams, C.S.4
-
14
-
-
25344474030
-
-
PRBMDO 0163-1829 10.1103/PhysRevB.38.2398
-
K. W. Schwarz, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.38.2398 38, 2398 (1988).
-
(1988)
Phys. Rev. B
, vol.38
, pp. 2398
-
-
Schwarz, K.W.1
-
17
-
-
22244471562
-
-
The polygons made by Eq. 1 tend to have more complex knots as N increases [JUPSAU 0031-9015
-
The polygons made by Eq. 1 tend to have more complex knots as N increases [K. Tsurusaki and T. Deguchi, J. Phys. Soc. Jpn. JUPSAU 0031-9015 64, 1506 (1995)]. However, vortex filament loops of various scales in actual turbulence should have statistically the same topology as long there is self-similarity over the scales. Hence, we opted to control not N but s.
-
(1995)
J. Phys. Soc. Jpn.
, vol.64
, pp. 1506
-
-
Tsurusaki, K.1
Deguchi, T.2
|