Standard boost, particles with mass M > 0

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Discussion Overview

The discussion revolves around the calculation of the rotation W(Λ,p) in the context of quantum field theory (QFT) for particles with mass M > 0. Participants explore the choice of a standard boost L(p) that maps a four-momentum kμ to pμ, particularly focusing on the implications of the spatial components of kμ being zero.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that Weinberg considers particles with mass M > 0 and discusses the need for a specific standard boost L(p) to calculate W(Λ,p).
  • Another participant suggests that any Lorentz transformation mapping kμ to pμ can be chosen, but highlights that a standard choice is the rotation-free Lorentz boost defined by the velocity vector.
  • A third participant expresses appreciation for the clarity of a referenced manuscript and decides to read it in full.
  • Subsequent comments reflect on the quality of the English in the manuscript, with one participant humorously noting their enjoyment of reading it in German.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the necessity of a specific choice for L(p), as there are differing views on the flexibility of choosing Lorentz transformations.

Contextual Notes

The discussion includes references to specific components of Lorentz transformations and the implications of choosing different boosts, but does not resolve the underlying assumptions or the mathematical steps involved in the calculations.

Who May Find This Useful

Readers interested in quantum field theory, particularly those exploring the mathematical foundations of Lorentz transformations and boosts for massive particles.

kent davidge
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Weinberg considers (p.68 QFT Vol. 1) particles with mass M > 0. The Little Group is SO(3). He wants to calculate the rotation
W(Λ,p) ≡ L-1(Λp) Λ L(p). He says that for this we need to choose a standard boost L(p) which carries the four momentum from
kμ = (0,0,0,M) to pμ. He then shows the expressions for the components of L(p). What I don't understand is that because the spatial components of kμ all vanish, i.e. ki = 0, why does it matter to choose a specific set of expressions for (L(p))i j?
 
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You can choose any Lorentz transformation that maps ##k^{\mu}## into ##p^{\mu}##. The most convenient (standard) choice is to use the uniquely defined rotation free Lorentz boost, i.e., a boost with velocity ##\vec{p}/p^0=\vec{p}/\sqrt{M^2+\vec{p}^2}##.

For more details have a look at appendix B of my QFT manuscript:

https://th.physik.uni-frankfurt.de/~hees/publ/lect.pdf
 
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Likes   Reactions: kent davidge and dextercioby
Oh, your pdfs are incredible clear and helpful. I decided to read the whole manuscript instead of just appendix B.
 
Well, the English is a desaster. It was written when I just started to study QFT a long time ago...
 
vanhees71 said:
Well, the English is a desaster. It was written when I just started to study QFT a long time ago...
Never mind about that. I even enjoy reading your manuscripts in german :biggrin:
 

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