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The quantum kicked rotator. First approach to “Quantum Chaos”: take a system that is classically chaotic and quantize it. Classical kicked rotator. One parameter map; can incorporate all others into choice of units. Diffusion in the kicked rotator. K = 5.0; strongly chaotic regime. - PowerPoint PPT Presentation
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The quantum kicked rotator
First approach to “Quantum Chaos”: take a system that is classically chaoticand quantize it.
Diffusion in the kicked rotator
• K = 5.0; strongly chaotic regime.•Take ensemble of 100,000 initial points with zero angularmomentum, and pseudo-randomly distributed angles.•Iterate map and take ensemble average at each time step
Diffusion in the kicked rotator
•System can get “trapped” for very long times in regions of cantori. Theseare the fractal remnants of invarient tori.•K = 1.0; i.e. last torus has been destroyed (K=0.97..).
Central limit theorem
Characteristic function of a joint probabilitydistribution is the product of individual distributions(if uncorrelated)
And Fourier transform back givesa Gaussian distribution – independent of thenature of the X random variable!
Quantum kicked rotator
•How do the physical properties of the system change when we quantize?•Two parameters in this Schrodinger equation; Planck’s constant is the additionalparameter.
The Floquet map
F is clearly unitary, as it must be, withthe Floquet phases as the diagonalelements.
Irrational a: transient diffusion
•Only for short time scales can diffusive behavior be seen•Spectrum of Floquet operator is now discrete.
Quantum chaos in ultra-cold atoms
All this can be seen in experiment; interaction of ultra-cold atoms (micro Kelvin)with light field; dynamical localization of atoms is seen for certain field modulations.
Irrational a: transient diffusion
System does not “feel” discrete nature of spectrum
Rapidly oscillating phasecancels out, only zero phaseterm survives
Since F is a banded matrix then the U’s will also all be banded, and hencefor l, k, k’ larger than some value there is no contribution to sum.
Disorder in the on-site potentials
•One dimensional lattice of 300 sites;•Ordered system: zero on-site potential.•Disordered system: pseudo-random on-sitepotentials in range [-0.5,0.5] with t=1.•Peaks in the spectrum of the orderedsystem are van Hove singularities; peaks in the spectrum of the disorderedsystem are very different in origin
Localisation of electrons by disorder
On-site order On-site disorder
Probability of finding system at a given site (y-axis) plotted versus energy index (x-axis); magnitude of probability indicated by size of dots.
TB Hamiltonian from a quantum map
If b is irrational then x distributed uniformly on [0,1]
Thus the analogy between Anderson localization in condensed matter and theangular momentum (or energy) localization is quantum chaotic systems is established.
Next weeks lecture
Proof that on-site disorder leads to localisationHusimi functions and (p,q) phase space
Examples of quantum chaos:•Quantum chaos in interaction of ultra-cold atoms with light field.•Square lattice in a magnetic field.
Some of these topics..
Resources used
“Quantum chaos: an introduction”, Hans-Jurgen Stockman, Cambridge University Press, 1999. (many typos!)
“The transition to chaos”: L. E. Reichl, Springer-Verlag (in library)
On-line: A good scholarpedia article about the quantum kicked oscillator; http://www.scholarpedia.org/article/Chirikov_standard_map
Other links which look nice (Google will bring up many more).
http://george.ph.utexas.edu/~dsteck/lass/notes.pdfhttp://lesniewski.us/papers/papers_2/QuantumMaps.pdfhttp://steck.us/dissertation/das_diss_04_ch4.pdf