-
1
-
-
0043269856
-
-
10.1103/PhysRevLett.90.254302
-
Oleg Lobkis and Richard Weaver, Phys. Rev. Lett. 90, 254302 (2003). 10.1103/PhysRevLett.90.254302
-
(2003)
Phys. Rev. Lett.
, vol.90
, pp. 254302
-
-
Lobkis, O.1
Weaver, R.2
-
2
-
-
28844485369
-
-
10.1103/PhysRevLett.95.184102
-
R. Schäfer, H.-J. Stöckmann, T. Gorin, and T. H. Seligman, Phys. Rev. Lett. 95, 184102 (2005). 10.1103/PhysRevLett.95.184102
-
(2005)
Phys. Rev. Lett.
, vol.95
, pp. 184102
-
-
Schäfer, R.1
Stöckmann, H.-J.2
Gorin, T.3
Seligman, T.H.4
-
4
-
-
23244443965
-
-
10.1088/1367-2630/7/1/152
-
R. Schafer, T. Gorin, H.-J. Stockmann, and T. H. Seligman, New J. Phys. 7, 152 (2005). 10.1088/1367-2630/7/1/152
-
(2005)
New J. Phys.
, vol.7
, pp. 152
-
-
Schafer, R.1
Gorin, T.2
Stockmann, H.-J.3
Seligman, T.H.4
-
8
-
-
0034299276
-
-
10.1006/jsvi.2000.3057
-
Oleg I. Lobkis, Richard L. Weaver, and Igor Rozhkov, J. Sound Vib. 237, 281 (2000) The number of channels and their coupling strengths are difficult to estimate from the data unless there are very few. If, however, one makes the assumption that all channels are equally coupled, one can often fit to a decay profile of the form E (t) = E0, [1+2σt]-M/2, where M is the number of channels and σ is the initial decay rate. 10.1006/jsvi.2000.3057
-
(2000)
J. Sound Vib.
, vol.237
, pp. 281
-
-
Lobkis, O.I.1
Weaver, R.L.2
Rozhkov, I.3
-
11
-
-
36549003614
-
-
10.1103/PhysRevE.76.051122
-
R. L. Weaver, Phys. Rev. E 76, 051122 (2007); 10.1103/PhysRevE.76.051122
-
(2007)
Phys. Rev. e
, vol.76
, pp. 051122
-
-
Weaver, R.L.1
-
12
-
-
0004451794
-
-
10.1006/jsvi.1999.2725
-
Richard L. Weaver and Oleg I. Lobkis, J. Sound Vib. 231, 1111 (2000). 10.1006/jsvi.1999.2725
-
(2000)
J. Sound Vib.
, vol.231
, pp. 1111
-
-
Weaver, R.L.1
Lobkis, O.I.2
-
15
-
-
0033899434
-
-
10.1016/S0041-624X(99)00047-5
-
Richard L. Weaver and Oleg I. Lobkis, Ultrasonics 38, 491 (2000). 10.1016/S0041-624X(99)00047-5
-
(2000)
Ultrasonics
, vol.38
, pp. 491
-
-
Weaver, R.L.1
Lobkis, O.I.2
-
16
-
-
34547346865
-
-
10.1103/RevModPhys.53.385
-
T. A. Brody, J. Flores, J. B. French, P. A. Mello, A. Pandey, and S. S. M. Wong, Rev. Mod. Phys. 53, 385 (1981). 10.1103/RevModPhys.53.385
-
(1981)
Rev. Mod. Phys.
, vol.53
, pp. 385
-
-
Brody, T.A.1
Flores, J.2
French, J.B.3
Mello, P.A.4
Pandey, A.5
Wong, S.S.M.6
-
17
-
-
0037720252
-
-
It is perhaps not widely appreciated that ostensibly regular elastodynamic bodies, when attention is confined to an irreducible symmetry class, exhibit what appear to be GOE level statistics unlike scalar waves [10.1103/PhysRevE.67.026213
-
It is perhaps not widely appreciated that ostensibly regular elastodynamic bodies, when attention is confined to an irreducible symmetry class, exhibit what appear to be GOE level statistics unlike scalar waves [K. Schaadt, A. P. B. Tufaile, and C. Ellegaard, Phys. Rev. E 67, 026213 (2003)]. This is in part due to mode conversion at free surfaces and in part to the strong diffraction at corners and edges. 10.1103/PhysRevE.67.026213
-
(2003)
Phys. Rev. e
, vol.67
, pp. 026213
-
-
Schaadt, K.1
Tufaile, A.P.B.2
Ellegaard, C.3
-
21
-
-
0001108748
-
-
10.1121/1.387816
-
R. Weaver, J. Acoust. Soc. Am. 71, 1608 (1982). 10.1121/1.387816
-
(1982)
J. Acoust. Soc. Am.
, vol.71
, pp. 1608
-
-
Weaver, R.1
|