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Theory Of Scattering For Quasifree Particles, A
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Theory Of Scattering For Quasifree Particles, A

Book Details

Format Hardback or Cased Book
ISBN-10 9814612065
ISBN-13 9789814612067
Publisher World Scientific Publishing Co Pte Ltd
Imprint World Scientific Publishing Co Pte Ltd
Country of Manufacture GB
Country of Publication GB
Publication Date Sep 30th, 2014
Print length 104 Pages
Weight 332 grams
Dimensions 15.70 x 23.10 x 1.20 cms
Product Classification: Particle & high-energy physics
Ksh 10,100.00
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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 ???+f, where f 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.

 

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 ϕ of the form ϕ→ϕ+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 ϕ → Tϕ, where T is a symplectic map on the one-particle space, not near the identity.


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