Asymptotic completeness, global existence and the infrared problem for the Maxwell-Dirac equations

著者

書誌事項

Asymptotic completeness, global existence and the infrared problem for the Maxwell-Dirac equations

Moshé Flato, Jacques C.H. Simon, Erik Taflin

(Memoirs of the American Mathematical Society, no. 606)

American Mathematical Society, 1997

大学図書館所蔵 件 / 17

この図書・雑誌をさがす

注記

"May 1997, volume 127, number 606 (second of 4 numbers)"

Includes bibliographical references (p. 309-311)

内容説明・目次

内容説明

The purpose of this work is to present and give full proofs of new original research results concerning integration of and scattering for the classical Maxwell-Dirac equations. These equations govern first quantized electrodynamics and are the starting point for a rigorous formulation of quantum electrodynamics. The presentation is given within the formalism of nonlinear group and Lie algebra representations, i.e. the powerful new approach to nonlinear evolution equations covariant under a group action.The authors prove that the nonlinear Lie algebra representation given by the manifestly covariant Maxwell-Dirac equations is integrable to a global nonlinear representation of the Poincare group on a differentiable manifold of small initial conditions. This solves, in particular, the small-data Cauchy problem for the Maxwell-Dirac equations globally in time. The existence of modified wave operators and asymptotic completeness is proved. The asymptotic representations (at infinite time) turn out to be nonlinear. A cohomological interpretation of the results in the spirit of nonlinear representation theory and its connection to the infrared tail of the electron are developed.

目次

Introduction The nonlinear representation $T$ and spaces of differentiable vectors The asymptotic nonlinear representation Construction of the approximate solution Energy estimates and $L^2-L^\infty$ estimates for the Dirac field Construction of the modified wave operator and its inverse Appendix.

「Nielsen BookData」 より

関連文献: 1件中  1-1を表示

詳細情報

ページトップへ