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Energy-momentum-tensor in quantumelectrodynamics

Thesis/Dissertation:

Abstract

This work deals with the operator properties of the energy-momentum-tensor (ET) in the framework of quantum electrodynamics. The principles of construction of the ET are discussed for quantized fields in the Schwinger variation principle. Dealing with the conserved quantities for quantized fields operator problems are coming up in the Coulomb gauge because Dirac- and Maxwellfield do not commute completely. Further on contemporary commutators of the ET components are investigated mutually. Finally non-canonical methods are developed.
Authors:
Publication Date:
Jan 01, 1974
Product Type:
Thesis/Dissertation
Reference Number:
AIX-07-258177; EDB-77-033750
Resource Relation:
Other Information: Thesis (Ph. D.). 85 refs.; with apps. Available from ZAED
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; ENERGY-MOMENTUM TENSOR; QUANTUM ELECTRODYNAMICS; ENERGY; LINEAR MOMENTUM; POINCARE GROUPS; QUANTUM OPERATORS; ELECTRODYNAMICS; FIELD THEORIES; LIE GROUPS; MATHEMATICAL OPERATORS; QUANTUM FIELD THEORY; SYMMETRY GROUPS; TENSORS; 645400* - High Energy Physics- Field Theory
OSTI ID:
7337934
Country of Origin:
Germany
Language:
German
Availability:
INIS
Submitting Site:
INIS
Size:
Pages: 104
Announcement Date:
May 13, 2001

Thesis/Dissertation:

Citation Formats

Schott, T. Energy-momentum-tensor in quantumelectrodynamics. Germany: N. p., 1974. Web.
Schott, T. Energy-momentum-tensor in quantumelectrodynamics. Germany.
Schott, T. 1974. "Energy-momentum-tensor in quantumelectrodynamics." Germany.
@misc{etde_7337934,
title = {Energy-momentum-tensor in quantumelectrodynamics}
author = {Schott, T}
abstractNote = {This work deals with the operator properties of the energy-momentum-tensor (ET) in the framework of quantum electrodynamics. The principles of construction of the ET are discussed for quantized fields in the Schwinger variation principle. Dealing with the conserved quantities for quantized fields operator problems are coming up in the Coulomb gauge because Dirac- and Maxwellfield do not commute completely. Further on contemporary commutators of the ET components are investigated mutually. Finally non-canonical methods are developed.}
place = {Germany}
year = {1974}
month = {Jan}
}