DeWitt | The Global Approach to Quantum Field Theory | Medienkombination | 978-0-19-851093-2 | www.sack.de

Medienkombination, Englisch, Format (B × H): 180 mm x 257 mm, Gewicht: 2744 g

DeWitt

The Global Approach to Quantum Field Theory


Erscheinungsjahr 2003
ISBN: 978-0-19-851093-2
Verlag: Oxford University Press

Medienkombination, Englisch, Format (B × H): 180 mm x 257 mm, Gewicht: 2744 g

ISBN: 978-0-19-851093-2
Verlag: Oxford University Press


The book shows how classical field theory, quantum mechanics, and quantum field theory are related. The
description is global from the outset. Quantization is explained using the Peierls bracket rather than the Poisson bracket. This allows one to deal immediately with observables, bypassing the canonical formalism of constrained Hamiltonian systems and bigger-than-physical Hilbert (or Fock) spaces. The Peierls bracket leads directly to the Schwinger variational principle and the Feynman functional integral, the latter of which is taken as defining the quantum theory.

Also included are the theory of tree amplitudes and conservation laws, which are presented classically and later extended to the quantum level. The quantum theory is developed from the many-worlds viewpoint, and ordinary path integrals and the topological issues to which they give rise are studied in some detail. The theory of mode functions and Bogoliubov coefficients for linear fields is fully developed, and then the quantum theory of nonlinear fields is confronted. The effective action, correlation functions and counter terms all make their appearance at this point, and the S-matrix is constructed via the introduction of asymptotic fields and the LSZ theorem. Gauge theories and ghosts are studied in great detail.

Many applications of the formalism are given: vacuum currents, anomalies, black holes, fourth-order systems, higher spin fields, the (lambda phi) to the fourth power model (and spontaneous symmetry breaking), quantum electrodynamics, the Yang-Mills field and its topology, the gravitational field, etc. Special chapters are devoted to
Euclideanization and renormalization, space and time inversion, and the closed-time-path or ``in-in'' formalism. Emphasis is given throughout to the role of the functional-integral measure in the theory. Six helpful appendices, ranging from superanalysis to analytic continuation in dimension, are included at the end.

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Weitere Infos & Material


- Classical Dynamical Theory

- 2: Dynamics and invariance transformations

- 3: Small disturbances and Green's functions

- 4: The Peierls bracket

- 5: Finite disturbances. Tree theorems. Asymptotic fields.

- 6: Conservation laws

- The Heuristic Road to Quantization. The Quantum Formalism and Its Interpretation

- 8: Quantum theory of measurement

- 9: Interpretation of the quantum formalism I

- 10: The Schwinger variational principle

- 11: The quantum mechanics of standard canonical systems

- 12: Interpretation of the quantum formalism II

- Evaluation and Approximation of Feynman Functional Integrals

- 14: Approximation and evaluation of the path integral

- 15: The nonrelativistic particle in a curved space

- 16: The heat kernel

- Linear Systems

- 18: Quantization of linear boson fields

- 19: Linear fermion fields. Stationary backgrounds.

- 20: Quantization of linear fermion fields

- 21: Linear fields in nonstationary backgrounds

- 22: Linear (or linearized) fields possessing invariant flows

- Nonlinear Fields

- 24: Gauge theories I. General formalism.

- 25: Gauge theories II. Background Field Methods. Scattering Theory.

- 26: Case-I gauge theory without ghosts. Description of cases II and III.

- Tools for Quantum Field Theory. Applications

- 28: Vacuum currents. Anomalies.

- 29: More vacuum phenomena

- 30: Black hole vacua. Hawking radiation.

- 31: The closed-time-path or 'in-in' formalism

- Special Topics

- 33: Canonical transformations. Space inversion and time reversal.

- 34: Quantum electrodynamics

- 35: The Yang-Mills and gravitational fields

- Simple Illustrative Examples

- X1: A simple Fermi system

- X2: A Fermi doublet

- X3: Fermi multiplet

- X4: The Fermi oscillator

- X5: The Bose oscillator

- X6: A fourth-order system

- X7: A model for ghosts

- X8: Free scalar field in flat spacetime

- X9: Massive vector field in four dimensional flat spacetime

- X10: Massive antisymmetric tensor field

- X11: Massive symmetric tensor field in flat spacetime

- X12: Massive spinor field in flat spacetime

- X13: Massive spin-3/2 field in flat spacetime

- X14: Elecromagnetic field in flat spacetime

- X15: Massless symmetric tensor field in flat spacetime

- X16: Massless spinor field in four dimensional flat spacetime

- X17: Massless spin-3/2 field in four dimensional flat spacetime

- X18: Renormalization group and spontaneous symmetry breaking in the (lambda phi) to the fourth power model

- X19: The relativistic particle in Minkowski spacetime

- X20: A simple soluble nonlinear model

- X21: Quantum mechanics on a circle

- X22: Quantum mechanics on a Klein bottle

- X23: Ghosts for ghosts

- X24: Massive antisymmetric tensor field

- A: Appendix A

- B: Appendix B

- C: Appendix C

- D: Appendix D

- E: Appendix E

- F: Appendix F


Prof. Bryce DeWitt
2411 Vista Lane
Austin, Texas 78703
dewitt@physics.utexas.edu
tel: 001-512-478-6037
fax: 001-512-471-0890

Birthplace: Dinuba, California, 8 January 1923



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