1988
DOI: 10.1007/bf01318307
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Integrable and nonintegrable classical spin clusters

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Cited by 27 publications
(27 citation statements)
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“…If it weren't for the slow convergence of the time averages along chaotic trajectories due to low-flux cantori [18][19][20], the entire chaotic region would be represented by a single isolated point in the constant-energy section of the invariant-surface. In the full ( M 2 x , M 2 z , E)-space, the points associated with chaotic regions form string-like objects.…”
Section: B Nonanalytic Invariantsmentioning
confidence: 99%
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“…If it weren't for the slow convergence of the time averages along chaotic trajectories due to low-flux cantori [18][19][20], the entire chaotic region would be represented by a single isolated point in the constant-energy section of the invariant-surface. In the full ( M 2 x , M 2 z , E)-space, the points associated with chaotic regions form string-like objects.…”
Section: B Nonanalytic Invariantsmentioning
confidence: 99%
“…In a diagram I λ versus E λ , the array of (2σ + 1) 2 points form a regular pattern, which, however, is likely to be visually distorted due to the generally complicated nonlinear dependence of E and I on J 1 , J 2 . But we do not, in fact, need to know the 2 nd integral of the motionÎ explicitly to carry out this scheme; we can, following an idea of Peres [24], always construct it via time averages similar to the procedure previously employed for the classical model [18]: Take any operator with [Â,Ĥ] = 0, which represents a dynamical variable independent ofĤ, and consider the matrix elementsÂ(t) in the energy representation,…”
Section: Quantum Invariantsmentioning
confidence: 99%
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