Path Integrals In Quantum Mechanics, Statistics, Polymer Physics, And Financial Markets (5th Edition) - Tapa blanda

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Hagen Kleinert is professor of physics at the Freie Universitat Berlin, Germany. As a visiting scientist, he has spent extended periods of time at CERN, the European Organization for Nuclear Research in Geneva; at Caltech in Pasadena; at the Universities of California in Berkeley, Santa Barbara, and San Diego; at the Los Alamos National Laboratory in New Mexico; and at Princeton University, New Jersey. He has made numerous contributions to the understanding of particle physics, mathematical physics, condensed matter physics, chemical physics, and nuclear physics. His two-volume book Gauge Fields in Condensed Matter (World Scientific, 1989), develops a new quantum field theory of phase transitions on the basis of disorder fields. Such fields have meanwhile become a powerful tool to investigate the statistical properties of fluctuating line-like excitations in various many-body systems, such as superfluids, superconductors, and crystals. Another book on Path Integrals was published by World Scientific in 1990 (5th edition, 2009). It is by far the most comprehensive text on this subject. He also published with World Scientific in 2001, in collaboration with V Schulte-Frohlinde, a thorough review book on the field-theoretic renormalization group approach to critical phenomena. The title is Critical Properties of Ø4-Theories. There a short-cut approach is developed on the basis of a field theoretic version of variational perturbation theory (VPT). Another book of his is entitled Multivalued Fields in Condensed Matter, Electromagnetism, and Gravitation (World Scientific, 2008). It shows that many phenomena in physics, in particular all those commonly explained by gauge theories, can be understood as consequences of a Riemann-sheet nature of fields.

De la contraportada

This is the fifth, expanded edition of the comprehensive textbook published in 1990 on the theory and applications of path integrals. It is the first book to explicitly solve path integrals of a wide variety of nontrivial quantum-mechanical systems, in particular the hydrogen atom. The solutions have been made possible by two major advances. The first is a new euclidean path integral formula which increases the restricted range of applicability of Feynman's time-sliced formula to include singular attractive 1/r- and 1/r2-potentials. The second is a new nonholonomic mapping principle carrying physical laws in flat spacetime to spacetimes with curvature and torsion, which leads to time-sliced path integrals that are manifestly invariant under coordinate transformations.

In addition to the time-sliced definition, the author gives a perturbative, coordinate-independent definition of path integrals, which makes them invariant under coordinate transformations. A consistent implementation of this property leads to an extension of the theory of generalized functions by defining uniquely products of distributions.

The powerful FeynmanKleinert variational approach is explained and developed systematically into a variational perturbation theory which, in contrast to ordinary perturbation theory, produces convergent results. The convergence is uniform from weak to strong couplings, opening a way to precise evaluations of analytically unsolvable path integrals in the strong-coupling regime where they describe critical phenomena.

Tunneling processes are treated in detail, with applications to the lifetimes of supercurrents, the stability of metastable thermodynamic phases, and thelarge-order behavior of perturbation expansions. A variational treatment extends the range of validity to small barriers. A corresponding extension of the large-order perturbation theory now also applies to small orders.

Special attention is devoted to path integrals with topological restrictions needed to understand the statistical properties of elementary particles and the entanglement phenomena in polymer physics and biophysics. The ChernSimons theory of particles with fractional statistics (anyons) is introduced and applied to explain the fractional quantum Hall effect.

The relevance of path integrals to financial markets is discussed, and improvements of the famous BlackScholes formula for option prices are developed which account for the fact, recently experienced in the world markets, that large fluctuations occur much more frequently than in Gaussian distributions.