What Does Target Space Mean in Sigma-Models and String Theory?

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SUMMARY

The term "target space" is crucial in the context of sigma-models, particularly in string theory and other fields such as QCD and condensed matter physics. In string theory, target space refers to the abstract space represented by a collection of D scalar fields in two dimensions, which serve as coordinates. The worldvolume, or worldsheets in this case, is where these scalar fields function as embedding coordinates of the string. It is essential to differentiate between scalar fields in the worldvolume and their counterparts in target space, as well as to distinguish between worldvolume and target space spinors.

PREREQUISITES
  • Understanding of sigma-models in theoretical physics
  • Familiarity with string theory concepts
  • Knowledge of scalar fields and their roles in physics
  • Basic grasp of worldvolume and target space terminology
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  • Study the SUGRA textbook by Van Proeyen for detailed explanations of target space and sigma-models
  • Explore the applications of sigma-models in quantum chromodynamics (QCD)
  • Research the distinctions between worldvolume and target space spinors
  • Investigate the role of embedding coordinates in string theory
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The discussion is beneficial for theoretical physicists, particularly those specializing in string theory, quantum field theory, and anyone interested in the mathematical foundations of sigma-models.

Naake
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Hi,
in one (hep-th) paper I found the term "target space" and I can not find any reasonable explanation of this.
Do you know anyone this term?

Thanks,
Michal
 
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This term is often used in the context of sigma-models, which have a wide range of applications (QCD, string theory, condensed matter physics,...). I take as example string theory.

In ST you consider a collection of D scalar fields in two dimensions. The scalar fields can be seen as coordinates in some abstract space. This is the target space. The two-dimensional world the theory lives in is then called the worldvolume, or in this case worldsheet. The scalar fields are then functions from the worldvolume to the targetspace, and are the embedding coordinates of the string.

You then have to be careful; the scalar fields are "scalar" in the worldvolume. In the end, you identify the targetspace with spacetime (but this is not necessarily so for a general sigma model!), and the worldvolume with the area the string traverses in this targetspace/spacetime. The same goes for e.g. "spinors"; a worldvolume spinor should be distinguished from a targetspace spinor!

Similarly, the embedding coordinates of a point particle can be seen as a collection of D scalar fields living on a one-dimensional worldvolume called the worldline. The targetspace is again spacetime.

A textbook in which this is all explained is the SUGRA-textbook of Van Proeyen.
 

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