Variation of the auxiliary worldsheet metric

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    Metric Variation
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Discussion Overview

The discussion revolves around the variation of the auxiliary worldsheet metric in the context of string theory, specifically how it is affected by reparametrization of the worldsheet. Participants seek clarification on the derivation of a specific formula related to this topic.

Discussion Character

  • Technical explanation, Conceptual clarification

Main Points Raised

  • One participant requests clarification on the derivation of the formula for the variation of the auxiliary worldsheet metric due to reparametrization.
  • Another participant expresses uncertainty about which formula is being referenced and asks for it to be provided or for a reference to be given.
  • A specific reference is provided by a participant, citing Clifford J. Johnson's work on D-branes, indicating that the relevant formula can be found on page 30, Equation 2.26.
  • A further participant explains the notation used in the reference, detailing the worldsheet coordinates and the embedding functions, and suggests that the infinitesimal variations of these expressions should be examined when changing coordinates.

Areas of Agreement / Disagreement

Participants have not reached a consensus on the specific formula in question, and there is ongoing clarification and exploration of the topic.

Contextual Notes

The discussion includes references to specific equations and notation, which may depend on the definitions used in the context of string theory. There are unresolved aspects regarding the derivation of the formula and the implications of the coordinate changes.

Jack2013
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Can somebody clarify how the formula for variation of the auxilliary worldsheet metric is obtained due to reparametrization of the worldsheet in string theory??
 
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I could probably explain if I knew which formula you are talking about. Could you type it out, or maybe give a reference to one of the string theory books?
 
In D-branes Clifford J. Johnson page 30 Equation 2.26
 
OK, Clifford is using [itex]\zeta^1, \zeta^2[/itex] to refer to the worldsheet coordinates [itex]\sigma, \tau[/itex]. So the embedding functions are

[tex]X^\mu(\zeta^1, \zeta^2)[/tex]
and the worldsheet metric with "up" indices is

[tex]\gamma^{ab}(\zeta^1, \zeta^2) \frac{\partial}{\partial \zeta^a} \otimes \frac{\partial}{\partial \zeta^b}[/tex]
So, all you need to do is look at the infinitesimal variations of these expressions when you change coordinates

[tex]\zeta^a = \zeta^a(\xi^1, \xi^2)[/tex]
 

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