Version 10, the stable version aug 2003 - nov 2004
CHAOS: CLASSICAL AND QUANTUM
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Contents | |||
Index | |||
Chapter 1 |
Overture
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Nov 20 2002
90% finished |
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Appendix A: | you might also want to read about the history of the subject. | ||
Exercises | Jan 30 2002 | ||
Jun 10 2003 | |||
Chapter 2 |
Flows
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Jun 18 2003
70% finished |
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Exercises | Jan 30 2002 | ||
Aug 21 2002 | |||
Chapter 3 |
Maps
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Jun 18 2003
70% finished |
Exercises | Jan 30 2002 |
Aug 21 2002 | |||
Chapter 4 |
Local stability
|
Nov 20 2002
60% finished |
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Exercises | Jan 30 2002 | ||
Jan 30 2002 | |||
Chapter 5 |
Newtonian dynamics
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Jun 18 2003
60% finished |
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Appendix C: | Stability of Hamiltonian flows: more details, especially for the helium. | ||
Exercises | Jan 30 2002 | ||
Jan 30 2002 | |||
Chapter 6 |
Get straight
|
Jun 18 2003
60% finished |
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Exercises | Aug 30 2003 | ||
Chapter 7 |
Transporting densities
|
Nov 20 2002
60% finished |
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Exercises | Jan 30 2002 | ||
10 Feb 2000 | |||
Chapter 8 |
Averaging
On the necessity of studying the averages of observables in chaotic dynamics. Formulas for averages are cast in a multiplicative form that motivates the introduction of evolution operators. |
Nov 20 2002
90% finished |
|
Exercises | Jan 30 2002 | ||
Aug 10 2002 | |||
Chapter 9 |
Qualitative dynamics, for pedestrians
|
Nov 20 2002
60% finished |
Appendix E: | deals with further, more advanced symbolic dynamics techniques. |
8 aug 99
80% finished |
Exercises | Jan 30 2002 | ||
10 Feb 2000 | |||
Chapter 10 |
Counting, for pedestrians
|
Aug 30 2003
60% finished |
|
Exercises | 22 aug 98 | ||
10 Feb 2000 | |||
Chapter 11 |
Trace formulas
|
Nov 20 2002
85% finished |
|
Exercises | Jan 30 2002 | ||
Aug 10 2002 | |||
Chapter 12 |
Spectral determinants
|
Nov 20 2002
85% finished |
|
Exercises | Jan 30 2002 | ||
Aug 10 2002 | |||
Chapter 13 |
Why does it work?
This chapter faces the singular kernels, the infinite dimensional vector spaces and all those other subtleties that are needed to put the spectral determinants on more solid mathematical footing, to the extent this can be achieved without proving theorems. |
Nov 20 2002
76% finished | |
Exercises | 12 aug 2000 | ||
16 May 2001 | |||
Chapter 14 |
Fixed points, and how to get them
|
4 Oct 98
70% finished |
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Exercises | 16 mar 98 | ||
12 aug 2000 | |||
Chapter 15 |
Cycle expansions
|
30 Aug 98
90% finished |
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Exercises | Jan 30 2002 | ||
10 Feb 2000 | |||
Chapter 16 |
Why cycle?
In the preceeding chapters we have moved at rather brisk pace and derived a gaggle of formulas. Here we slow down in order to develop some fingertip feeling for the objects derived so far. Just to make sure that the key message - the ``trace formulas'' and their ilk - have sunk in, we rederive them in a rather different, more intuitive way, and extol their virtues. This part is bedtime reading. A few special determinants are worked out by hand. |
Nov 20 2002
50% finished | |
Exercises | Jan 30 2002 | ||
Aug 10 2002 | |||
Chapter 17 |
Thermodynamic formalism
Generalized dimensions, entropies and such. |
25 aug 2000
50% finished | |
Exercises | 25 aug 2000 | ||
Chapter 18 |
Intermittency
What to do about sticky, marginally stable trajectories? Power-law rather than exponential decorrelations? |
Nov 20 2002
75% finished | |
Exercises | 7 jun 2000 | ||
7 jun 2000 | |||
Chapter 19 |
Discrete symmetries
Dynamics often comes equipped with discrete symmetries, such as the reflection and the rotation symmetries. Symmetries simplify and improve the cycle expansions in a rather beautiful way. This chapter explains how symmetries factorize the cycle expansions. | Nov 20 2002 | |
Appendix I: | deals with further examples of discrete symmetry (rectangles and squares). |
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|
Exercises | 10 jan 99 | ||
Chapter 20 |
Deterministic diffusion
We look at transport coefficients and derive exact formulas for diffusion constants when diffusion is normal, and the anomalous diffusion exponents when it is not. All done from first principles without ever invoking any probabilistic notions. |
Nov 20 2002
85% finished | |
Exercises | 16 mar 98 | ||
10 feb 2000 | |||
Chapter 21 |
Irrationally winding
Circle maps and their thermodynamics analyzed in detail. |
Dec 96
85% finished | |
Exercises |
Part II: Quantum chaos
Chapter 22 |
Prologue
|
Jun 15 2003
70% finished |
|
Chapter 23 |
Quantum mechanics, briefly
We first recapitulate basic notions of quantum mechanics and define the main quantum objects of interest, the quantum propagator and the Green's function. |
Jan 30 2002
85% finished | |
Chapter 24 |
WKB quantization
A review of the Wentzel-Kramers-Brillouin quantization of 1-dimensional systems. |
Jan 30 2002
85% finished | |
Exercises | Jun 15 2003 | ||
Chapter 25 |
Relaxation for cyclists
In Chapter 14 we offered an introductory, hands-on guide to extraction of periodic orbits by means of the Newton-Raphson method. Here we take a very different tack, drawing inspiration from variational principles of classical mechanics, and path integrals of quantum mechanics. |
Aug 30 2003
85% finished | |
Exercises | Aug 30 2003 | ||
10 Feb 2000 | |||
Chapter 26 |
Semiclassical evolution
We relate the quantum propagator to the classical flow of the underlying dynamical system; the semiclassical propagator and Green's function. |
Jan 30 2002
85% finished | |
Exercises | Jan 30 2002 | ||
10 Feb 2000 | |||
Chapter 27 |
Semiclassical quantization
This is what could have been done with the old quantum mechanics if physicists of 1910's were as familiar with chaos as you by now are. The Gutzwiller trace formula together with the corresponding spectral determinant, the central results of the semiclassical periodic orbit theory, are derived. |
Jan 30 2002
80% finished | |
Exercises | Jan 30 2002 | ||
Aug 10 2002 | |||
Chapter 28 |
Chaotic scattering
Scattering off N disks, exact and semiclassical. |
12 aug 2000
80% finished | |
Appendix K: | What is the meaning of traces and determinants for infinite-dimensional operators? |
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Exercises | 12 aug 2000 | ||
10 Feb 2000 | |||
Chapter 29 |
Helium atom
The helium atom spectrum computed via semiclassical spectral determinants. |
17 june 2000
96% finished | |
Appendix C: | Stability of Hamiltonian flows: more details, especially for the helium. | ||
Exercises | 12 aug 2000 | ||
Aug 10 2002 | |||
Chapter 30 |
Diffraction distraction
Diffraction effects of scattering off wedges, eavesdropping around corners incorporated into periodic orbit theory. |
Jan 30 2002
95% finished | |
Exercises | Jan 30 2002 | ||
Epilogue
Take-home problem set for the third millenium. |
6 Sept 96
10% finished |
Part www: Material which will be kept on the web
Appendix A |
Brief history of chaos
Classical mechanics has not stood still since Newton. The formalism that we use today was developed by Euler and Lagrange. By the end of the 1800's the three problems that would lead to the notion of chaotic dynamics were already known: the three-body problem, the ergodic hypothesis, and nonlinear oscillators. |
22 Jul 97
66% finished | |
Appendix B |
Infinite-dimensional flows
Flows described by partial differential equations are infinite dimensional because if one writes them down as a set of ordinary differential equations (ODEs) then one needs an infinity of the ordinary kind to represent the dynamics of one equation of the partial kind (PDE). |
20 nov 2002
30% finished | |
Appendix C |
Stability of Hamiltonian flows
Symplectic invariance, classical collinear helium stability worked out in detail. |
12 aug 2000
80% finished | |
Appendix D |
Implementing evolution
To sharpen our intuition, we outline the fluid dynamical vision, have a bout of Koopmania, and show that short-times step definition of the Koopman operator is a prescription for finite time step integration of the equations of motion. |
15 nov 2002
50% finished | |
Exercises | |||
Appendix E |
Symbolic dynamics techniques
Further, more advanced symbolic dynamics techniques. |
9 March 98
60% finished | |
Appendix F |
Counting itineraries
Further, more advanced cycle counting techniques. |
30 nov 2001
60% finished | |
Exercises | |||
Appendix G |
Finding cycles
More on Newton-Raphson method. |
9 March 98
60% finished | |
Appendix H |
Applications
To compute an average using cycle expansions one has to find the right eigenvalue and maybe a few of its derivatives. Here we explore how to do that for all sorts of averages, some more physical than others. |
Jan 30 2002
60% finished | |
Exercises | Jan 30 2002 | ||
10 Feb 2000 | |||
Appendix I |
Discrete symmetries
Dynamical zeta functions for systems with symmetries of squares or rectangles worked out in detail. |
10 Jan 99
80% finished | |
Appendix J |
Convergence of spectral determinants
A heuristic estimate of the n-th cummulant. |
12 aug 2000
30% finished | |
Appendix K |
Infinite dimensional operators
What is the meaning of traces and determinants for infinite-dimensional operators? |
9 Feb 96
95% finished | |
Appendix L |
Statistical mechanics recycled
The Ising-like spin systems recycled. The Feigenbaum scaling function and the Fisher droplet model. |
14 Nov 96
33% finished | |
Exercises | 9 sep 98 | ||
10 Feb 2000 | |||
Appendix M |
Noise/quantum trace formulas
The quantum/noise perturbative corrections formulas derived as Bohr and Sommerfeld would have derived them were they cogniscenti of chaos, with some Vattayismo rumminations along the way. |
5 Jun 1995
50% finished | |
Appendix N |
What reviewers say
Bohr, Feynman and so on turning in their graves. Ignore this. |
12 aug 2000
1% finished | |
Appendix O |
Solutions
Solutions to selected problems - often more instructive than the text itself. Recommended. |
Jan 30 2002
55% finished | |
Appendix P |
Projects
The essence of this subject is incommunicable in print; the only way to developed intuition about chaotic dynamics is by computing, and you are urged to try to work through the essential steps in a project that combines the techniques learned in the course with some application of interest to you.
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12 aug 2000
55% finished |