Quantum Electrodynamics of Strong Fields: With an Introduction into Modern Relativistic Quantum Mechanics
The fundamental goal of physics is an understanding of the forces of nature in their simplest and most general terms. Yet there is much more involved than just a basic set of equations which eventually has to be solved when applied to specific problems. We have learned in recent years that the structure of the ground state of field theories (with which we are generally concerned) plays an equally fundamental role as the equations of motion themselves. Heisenberg was probably the first to recognize that the ground state, the vacuum, could acquire certain properties (quantum numbers) when he devised a theory of ferromagnetism. Since then, many more such examples are known in solid state physics, e. g. supercon­ ductivity, superfluidity, in fact all problems concerned with phase transitions of many-body systems, which are often summarized under the name synergetics. Inspired by the experimental observation that also fundamental symmetries, such as parity or chiral symmetry, may be violated in nature, it has become wide­ ly accepted that the same field theory may be based on different vacua. Practical­ ly all these different field phases have the status of more or less hypothetical models, not (yet) directly accessible to experiments. There is one magnificent ex­ ception and this is the change of the ground state (vacuum) of the electron-posi­ tron field in superstrong electric fields.
"1111727060"
Quantum Electrodynamics of Strong Fields: With an Introduction into Modern Relativistic Quantum Mechanics
The fundamental goal of physics is an understanding of the forces of nature in their simplest and most general terms. Yet there is much more involved than just a basic set of equations which eventually has to be solved when applied to specific problems. We have learned in recent years that the structure of the ground state of field theories (with which we are generally concerned) plays an equally fundamental role as the equations of motion themselves. Heisenberg was probably the first to recognize that the ground state, the vacuum, could acquire certain properties (quantum numbers) when he devised a theory of ferromagnetism. Since then, many more such examples are known in solid state physics, e. g. supercon­ ductivity, superfluidity, in fact all problems concerned with phase transitions of many-body systems, which are often summarized under the name synergetics. Inspired by the experimental observation that also fundamental symmetries, such as parity or chiral symmetry, may be violated in nature, it has become wide­ ly accepted that the same field theory may be based on different vacua. Practical­ ly all these different field phases have the status of more or less hypothetical models, not (yet) directly accessible to experiments. There is one magnificent ex­ ception and this is the change of the ground state (vacuum) of the electron-posi­ tron field in superstrong electric fields.
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Quantum Electrodynamics of Strong Fields: With an Introduction into Modern Relativistic Quantum Mechanics

Quantum Electrodynamics of Strong Fields: With an Introduction into Modern Relativistic Quantum Mechanics

Quantum Electrodynamics of Strong Fields: With an Introduction into Modern Relativistic Quantum Mechanics

Quantum Electrodynamics of Strong Fields: With an Introduction into Modern Relativistic Quantum Mechanics

Paperback(Softcover reprint of the original 1st ed. 1985)

$169.99 
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Overview

The fundamental goal of physics is an understanding of the forces of nature in their simplest and most general terms. Yet there is much more involved than just a basic set of equations which eventually has to be solved when applied to specific problems. We have learned in recent years that the structure of the ground state of field theories (with which we are generally concerned) plays an equally fundamental role as the equations of motion themselves. Heisenberg was probably the first to recognize that the ground state, the vacuum, could acquire certain properties (quantum numbers) when he devised a theory of ferromagnetism. Since then, many more such examples are known in solid state physics, e. g. supercon­ ductivity, superfluidity, in fact all problems concerned with phase transitions of many-body systems, which are often summarized under the name synergetics. Inspired by the experimental observation that also fundamental symmetries, such as parity or chiral symmetry, may be violated in nature, it has become wide­ ly accepted that the same field theory may be based on different vacua. Practical­ ly all these different field phases have the status of more or less hypothetical models, not (yet) directly accessible to experiments. There is one magnificent ex­ ception and this is the change of the ground state (vacuum) of the electron-posi­ tron field in superstrong electric fields.

Product Details

ISBN-13: 9783642822742
Publisher: Springer Berlin Heidelberg
Publication date: 12/22/2011
Series: Theoretical and Mathematical Physics
Edition description: Softcover reprint of the original 1st ed. 1985
Pages: 596
Product dimensions: 6.69(w) x 9.61(h) x 0.05(d)

Table of Contents

1. Introduction.- 2. The Wave Equation for Spin-1/2 Particles.- 3. Dirac Particles in External Potentials.- 4. The Hole Theory.- 5. The Klein Paradox.- 6. Resonant States in Supercritical Fields.- 7. Quantum Electrodynamics of Weak Fields.- 8. The Classical Dirac Field Interacting with a Classical Electromagnetic Field — Formal Properties.- 9. Second Quantization of the Dirac Field and Definition of the Vacuum.- 10. Evolution of the Vacuum State in Supercritical Potentials.- 11. Superheavy Quasimolecules.- 12. The Dynamics of Heavy-Ion Collisions.- 13. Experimental Test of Supercritical Fields in Heavy-Ion Collisions.- 14. Vacuum Polarization.- 15. Vacuum Polarization: Arbitrarily Strong External Potentials.- 16. Many-Body Effects in QED of Strong Fields.- 17. Bosons Bound in Strong Potentials.- 18. Subcritical External Potentials.- 19. Overcritical Potential for Bose Fields.- 20. Strong Yang-Mills Fields.- 21. Strong Fields in General Relativity.- References.
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