-
3
-
-
84956071876
-
-
J.H. Hannay and M.V. Berry, Physica (Amsterdam)10.1016/0167-2789(80)90026-3 1D, 267–290 (1980).
-
(1980)
Physica (Amsterdam)
, vol.1D
, pp. 267-290
-
-
-
6
-
-
0040282818
-
-
A. Crisanti, M. Falcioni, G. Mantica, and A. Vulpiani, Phys. Rev. EPLEEE810.1103/PhysRevE.50.1959 50, 1959 (1994);
-
(1994)
Phys. Rev. E
, vol.50
, pp. 1959
-
-
Crisanti, A.1
Falcioni, M.2
Mantica, G.3
Vulpiani, A.4
-
7
-
-
0034207252
-
-
G. Mantica, Phys. Rev. EPLEEE810.1103/PhysRevE.61.6434 61, 6434 (2000).
-
(2000)
Phys. Rev. E
, vol.61
, pp. 6434
-
-
Mantica, G.1
-
9
-
-
51249182411
-
-
Originally, it was noticed that introducing a random component in the quantum evolution restores the diffusive properties of kicked rotors: see I. Guarneri, Lett. Nuovo Cimento 40, 171 (1984);
-
(1984)
Lett. Nuovo Cimento
, vol.40
, pp. 171
-
-
Guarneri, I.1
-
12
-
-
29444447839
-
-
The decoherent approach to quantum chaos flourished soon after: see, e.g., T. Dittrich and R. Graham, Phys. Rev. A10.1103/PhysRevA.42.4647 42, 4647 (1990);
-
(1990)
Phys. Rev. A
, vol.42
, pp. 4647
-
-
Dittrich, T.1
Graham, R.2
-
14
-
-
0000105932
-
-
W.H. Zurek and J.P. Paz, Physica (Amsterdam)10.1016/0167-2789(94)00271-Q 83D, 300 (1995);
-
Physica (Amsterdam)
, vol.83
, pp. 300
-
-
-
16
-
-
0037428573
-
-
and the recent A.K. Pattanayak, B. Sundaram, and B.J. Greenbaum, Phys. Rev. Lett.10.1103/PhysRevLett.90.014103 90, 14103 (2003). In many of these works, a randomly perturbed quantum cat plays a major role.
-
(2003)
Phys. Rev. Lett.
, vol.90
, pp. 14103
-
-
Pattanayak, A.K.1
Sundaram, B.2
Greenbaum, B.J.3
-
22
-
-
84956110264
-
-
Yu.�I. Kifer, Math. USSR Izv. 8, 1083 (1974).
-
(1974)
Math. USSR Izv.
, vol.8
, pp. 1083
-
-
-
23
-
-
48749145105
-
-
See, e.g., J.P. Crutchfield and N.H. Packard, Physica (Amsterdam)10.1016/0167-2789(83)90127-6 7D, 201–223 (1983);
-
(1983)
Physica (Amsterdam)
, vol.7D
, pp. 201-223
-
-
-
24
-
-
0034238980
-
-
and the more recent A. Ostruszka, P. Pakoński, W. Slomczyński, and K. Życzkowski, Phys. Rev. EPLEEE810.1103/PhysRevE.62.2018 62, 2018 (2000);
-
(2000)
Phys. Rev. E
, vol.62
, pp. 2018
-
-
Ostruszka, A.1
Pakoński, P.2
Slomczyński, W.3
Życzkowski, K.4
-
25
-
-
0000712133
-
-
G. Boffetta, M. Cencini, M. Falcioni, and A. Vulpiani, Phys. Rep.10.1016/S0370-1573(01)00025-4 356, 367 (2002).
-
(2002)
Phys. Rep.
, vol.356
, pp. 367
-
-
Boffetta, G.1
Cencini, M.2
Falcioni, M.3
Vulpiani, A.4
-
32
-
-
13844322865
-
-
P. Gaspard and X.-J. Wang, Phys. Rep.10.1016/0370-1573(93)90012-3 235, 291 (1993), and references therein.
-
(1993)
Phys. Rep.
, vol.235
, pp. 291
-
-
Gaspard, P.1
Wang, X.-J.2
-
33
-
-
0002367988
-
-
Y.E. Levy, Phys. Lett. A10.1016/0375-9601(82)90408-X 88, 1 (1982).
-
(1982)
Phys. Lett. A
, vol.88
, pp. 1
-
-
Levy, Y.E.1
-
34
-
-
85038330063
-
-
J. Coste and M. Hénon, in Disordered Systems and Biological Organization, edited by E. Bienestock et al, (Springer, Berlin, 1986), p.�360.
-
(1986)
, pp. 360
-
-
Coste, J.1
Hénon, M.2
-
37
-
-
0034227589
-
-
In M. Cencini, M. Falcioni, E. Olbrich, H. Kanz, and A. Vulpiani, Phys. Rev. EPLEEE810.1103/PhysRevE.62.427 62, 427 (2000) a similar situation was found: a nonchaotic continuous system, which can be regarded as an approximation, on large scales of resolution, of a chaotic system, can develop (on the same scales) the entropic behavior of the chaotic one, by virtue of an added random noise.
-
(2000)
Phys. Rev. E
, vol.62
, pp. 427
-
-
Cencini, M.1
Falcioni, M.2
Olbrich, E.3
Kanz, H.4
Vulpiani, A.5
|