Light-Cone Gauge Definition & Advantages

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Discussion Overview

The discussion focuses on the definition and advantages of the light-cone gauge, particularly in the context of string theory and quantum chromodynamics (QCD). Participants explore its implications and applications in theoretical physics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants seek a clear definition of light-cone gauge and its advantages.
  • One participant suggests that light-cone gauge is a "physical gauge" that includes only physical degrees of freedom, akin to quantizing QED with only transverse polarizations of photons.
  • Another participant emphasizes that while light-cone gauge is useful in string theory, it is also relevant in QCD, where it is defined as A^+=0.
  • Concerns are raised about the lack of manifest Lorentz invariance in the theory quantized in light-cone gauge, necessitating careful verification.
  • There is a suggestion that the discussion may be more relevant to QCD than string theory, indicating a potential divergence in focus among participants.

Areas of Agreement / Disagreement

Participants express differing views on the relevance of light-cone gauge to string theory versus QCD, indicating that multiple competing perspectives exist without a clear consensus.

Contextual Notes

Some limitations include the dependence on specific definitions of light-cone gauge and the varying contexts (string theory vs. QCD) in which it is applied. The discussion does not resolve the implications of these differences.

arroy_0205
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What is the definition of light-cone gauge? Is there any advantage for working in this gauge?
 
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arroy_0205 said:
What is the definition of light-cone gauge? Is there any advantage for working in this gauge?

Are you referring to string theory in particular (if so you might want to post in the Beyond The Standard Model subforum)? If yes, you should look at the book by Zwiebach where it is explained in details. Basically, it's the gauge where light-cone coordinates are used for the coordinates of string. The advantage in that gauge is that it's a "physical gauge" in the sense that only physical degrees of freedome are present from the very beginning. It's a bit like quantizing QED with only transverse polarizations of the photon present as the degrees of freedom. The disadvantage (like in QED) is that the theory quantized in that gauge is not manifestly Lorentz invariant and one has to check this carefully.
 
** the book by Zwiebach where it is explained in details

I can confirm that a detailed description of the light cone gauge is in Barton Zwiebach's book "A first course in string theory". It is part of general relativity and not part of an extension beyond the standard model.

It gets used in string theory.
 
I try to answer this question.

To my knowledge, string theory started from strong force theory, so I think it will be better
answer the question from QCD. Maybe this question is nothing to do with string theory.

In QCD, light-cone gauge is defined as A^+=0. It is reasonable as only one direction of the incident particle is comparable to light speed in high energy experiments. It is much clearer
from the Lorentz transformation matrix, the boost is only involved by one space axes and one time axes.


Any other explanations are welcome.
 

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