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Theory Of Scattering For Quasifree Particles, A

Om Theory Of Scattering For Quasifree Particles, A

In this book, the author presents the theory of quasifree quantum fields and argues that they could provide non-zero scattering for some particles. The free-field representation of the quantised transverse electromagnetic field is not closed in the weak*-topology. Its closure contains soliton-anti-soliton pairs as limits of two-photon states as time goes to infinity, and the overlap probability can be computed using Uhlmann's prescription. There are no free parameters: the probability is determined with no requirement to specify any coupling constant. All cases of the Shale transforms of the free field ¿ of the form ¿→¿+φ, where φ is not in the one-particle space, are treated in the book. There remain the cases of the Shale transforms of the form ¿ → T¿, where T is a symplectic map on the one-particle space, not near the identity.

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  • Språk:
  • Engelska
  • ISBN:
  • 9789814612067
  • Format:
  • Inbunden
  • Sidor:
  • 104
  • Utgiven:
  • 30. september 2014
  • Mått:
  • 231x157x12 mm.
  • Vikt:
  • 332 g.
  Fri leverans
Leveranstid: 2-4 veckor
Förväntad leverans: 19. december 2024
Förlängd ångerrätt till 31. januari 2025

Beskrivning av Theory Of Scattering For Quasifree Particles, A

In this book, the author presents the theory of quasifree quantum fields and argues that they could provide non-zero scattering for some particles. The free-field representation of the quantised transverse electromagnetic field is not closed in the weak*-topology. Its closure contains soliton-anti-soliton pairs as limits of two-photon states as time goes to infinity, and the overlap probability can be computed using Uhlmann's prescription. There are no free parameters: the probability is determined with no requirement to specify any coupling constant. All cases of the Shale transforms of the free field ¿ of the form ¿→¿+φ, where φ is not in the one-particle space, are treated in the book. There remain the cases of the Shale transforms of the form ¿ → T¿, where T is a symplectic map on the one-particle space, not near the identity.

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