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Semi-classics for non-integrable systems. Lecture 8 of “Introduction to Quantum Chaos”. Kicked oscillator: a model of Hamiltonian chaos. Cantorous. 1/2. 5/8. Poincare- Birkhoff fixed point theorem Homoclinic tangle: generic chaos Tori which survives the onset of chaos - PowerPoint PPT Presentation
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Semi-classics for non-integrable systems
Lecture 8 of “Introduction to Quantum Chaos”
Kicked oscillator: a model of Hamiltonian chaos
5/8
1/2
Poincare-Birkhoff fixed point theoremHomoclinic tangle: generic chaosTori which survives the onset of chaosin phase space the longest has actiongiven by the “golden mean”.
Cantorous
Homoclinic tangle
Localization and resonance in quantum chaotic systems
Previous lecture: A system that is classically diffusive can be dynamically localized in the analogous quantum case, e.g., kicked rotator,
but also can show quantum resonances (Lecture 4)
Quantum
QuantumClassical
Universal and non-universal features of quantum chaotic systems
Universal features of eigenvaluespacing.
Quantum scaring ofthe wavefunction.
Classical phase space of non-integrable system is not motion ond-dimensional torus – whorls and tendrils of topologically mixing phase space.
Usual semi-classical approach (as we will see) relies on motion on a torus.
Semi-classics of quantum chaotic systems
WKB approximation
neglect in semi-classical limit
Can now integrate to find S and A.
Stationary phase approximation
Semi-classics for integrable systems
Position space
Momentum space
Fourier transform to obtain wavefunction in momentum spaceand then use stationary phase approximation.
Semi-classics for integrable systems
Solution valid at classical turningpoint
But breaks down here!
Hence, switch back to position space
Semi-classics for integrable systems
Phase has been accumulatedfrom the turning point!
Again, use stationary phase approximation
Maslov index
Bohr-Sommerfeld quantisation conditionwith Maslov index
• Feynmann path integral result for the propagator• Useful (classical) relations• Semiclassical propagator• Semiclassical Green’s function• Monodromy matrix• Gutzwiller trace formula
Semi-classics where the corresponding classical system is not integrable
Road map for semi-classics for non-integrable systems:
Feynmann path integral result for the propagator
Feynmann path integral result for the propagator
Feynmann path integral result for the propagator
Feynmann path integral result for the propagator
Feynman path integral; integral overall possible paths (not only classicallyallowed ones).
Useful (classical) relations
Useful (classical) relations
The semiclassical propagator
Only classical trajectoriesallowed!
The semiclassical propagator
The semiclassical propagator
Caustic
Focus
Zero’s of D correspond to caustics or focus points.
The semiclassical propagator
Example: propagation of Gaussian wave packet
Maslov index:equal to number ofzero’s of inverse D
The semiclassical propagator
The semiclassical Green’s function
The semiclassical Green’s function
Require in terms of action and notHamilton’s principle function
Evaluating the integral with stationary phase approximation leads to
The semiclassical Green’s function
The semiclassical Green’s function
The semiclassical Green’s function
The semiclassical Green’s function
Finally find
Monodromy matrix
Monodromy matrix
For periodic system monodromy matrix coordinate independent
Gutzwiller trace formula
Gutzwiller trace formula
Only periodic orbits contribute to semi-classicalspectrum!
Gutzwiller trace formula
Gutzwiller trace formula
Gutzwiller trace formula
Semiclassical quantum spectrum given by sum of periodicorbit contributions