Light-Cone Gauge Definition & Advantages

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SUMMARY

The light-cone gauge is a specific framework used primarily in string theory, defined by the use of light-cone coordinates. This gauge offers the advantage of incorporating only physical degrees of freedom from the outset, akin to quantizing quantum electrodynamics (QED) with only transverse polarizations of photons. However, it lacks manifest Lorentz invariance, necessitating careful verification of this property. Key references include Barton Zwiebach's book "A First Course in String Theory," which provides a comprehensive explanation of the light-cone gauge.

PREREQUISITES
  • Understanding of light-cone coordinates in string theory
  • Familiarity with quantum electrodynamics (QED)
  • Basic knowledge of Lorentz invariance
  • Awareness of quantum chromodynamics (QCD)
NEXT STEPS
  • Read Barton Zwiebach's "A First Course in String Theory" for an in-depth understanding of light-cone gauge
  • Explore the implications of Lorentz invariance in quantum field theories
  • Investigate the role of light-cone gauge in quantum chromodynamics (QCD)
  • Study the differences between physical and unphysical gauges in theoretical physics
USEFUL FOR

This discussion is beneficial for theoretical physicists, string theorists, and students of quantum field theory seeking to deepen their understanding of gauge choices and their implications in high-energy physics.

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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