TY - JOUR
T1 - Chaos and quantum mechanics
AU - Habib, Salman
AU - Bhattacharya, Tanmoy
AU - Greenbaum, Benjamin
AU - Jacobs, Kurt
AU - Shizume, Kosuke
AU - Sundaram, Bala
PY - 2005
Y1 - 2005
N2 - The relationship between chaos and quantum mechanics has been somewhat uneasy-even stormy, in the minds of some people. However, much of the confusion may stem from inappropriate comparisons using formal analyses. In contrast, our starting point here is that a complete dynamical description requires a full understanding of the evolution of measured systems, necessary to explain actual experimental results. This is of course true, both classically and quantum mechanically. Because the evolution of the physical state is now conditioned on measurement results, the dynamics of such systems is intrinsically nonlinear even at the level of distribution functions. Due to this feature, the physically more complete treatment reveals the existence of dynamical regimes-such as chaos-that have no direct counterpart in the linear (unobserved) case. Moreover, this treatment allows for understanding how an effective classical behavior can result from the dynamics of an observed quantum system, both at the level of trajectories as well as distribution functions. Finally, we have the striking prediction that time-series from measured quantum systems can be chaotic far from the classical regime, with Lyapunov exponents differing from their classical values. These predictions can be tested in next-generation experiments.
AB - The relationship between chaos and quantum mechanics has been somewhat uneasy-even stormy, in the minds of some people. However, much of the confusion may stem from inappropriate comparisons using formal analyses. In contrast, our starting point here is that a complete dynamical description requires a full understanding of the evolution of measured systems, necessary to explain actual experimental results. This is of course true, both classically and quantum mechanically. Because the evolution of the physical state is now conditioned on measurement results, the dynamics of such systems is intrinsically nonlinear even at the level of distribution functions. Due to this feature, the physically more complete treatment reveals the existence of dynamical regimes-such as chaos-that have no direct counterpart in the linear (unobserved) case. Moreover, this treatment allows for understanding how an effective classical behavior can result from the dynamics of an observed quantum system, both at the level of trajectories as well as distribution functions. Finally, we have the striking prediction that time-series from measured quantum systems can be chaotic far from the classical regime, with Lyapunov exponents differing from their classical values. These predictions can be tested in next-generation experiments.
KW - Chaos
KW - Quantum mechanics
UR - http://www.scopus.com/inward/record.url?scp=23744508299&partnerID=8YFLogxK
U2 - 10.1196/annals.1350.026
DO - 10.1196/annals.1350.026
M3 - Article
AN - SCOPUS:23744508299
SN - 0077-8923
VL - 1045
SP - 308
EP - 332
JO - Annals of the New York Academy of Sciences
JF - Annals of the New York Academy of Sciences
ER -