Heterotic strings (another question for experts)

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Discussion Overview

The discussion revolves around the properties of heterotic strings, particularly focusing on the presence of tachyons in bosonic strings and their implications in heterotic string theory. Participants explore the relationship between supersymmetry and the existence of tachyons, as well as the structure of heterotic strings in different dimensional contexts.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that the presence of a tachyon in bosonic strings is problematic, questioning why this issue does not extend to the bosonic part of heterotic strings.
  • Another participant explains that the "standard" heterotic string is a "correlated" product of a left-moving bosonic string and a right-moving superstring, which prevents the tachyon from appearing if the theory includes space-time supersymmetry.
  • It is mentioned that heterotic strings can also be constructed without supersymmetry, in which case tachyons typically do appear.
  • A later reply clarifies that the tachyon is the unique ground state of the string, leading to the conclusion that there is only one tachyon state that affects both sectors of the heterotic theory, and the GSO projection removes it from both the right and left sectors.

Areas of Agreement / Disagreement

Participants express differing views on the implications of tachyons in heterotic strings, particularly regarding the role of supersymmetry and the structure of the string theory. The discussion remains unresolved on certain aspects, particularly concerning the construction of heterotic strings without supersymmetry.

Contextual Notes

Some limitations include the dependence on definitions of tachyons and supersymmetry, as well as the specific conditions under which the GSO projection operates. The discussion does not resolve the broader implications of these factors within the context of heterotic string theory.

Demystifier
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The problem with bosonic strings is the fact that they contain a tachyon.
Why that is not a problem for the bosonic part of heterotic strings?
 
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The "standard" heterotic string is not a direct product of a (left-moving) bosonic string with a (right-moving) superstring, but it is a "correlated" product. That's why the bosonic string tachyon does not need to appear, and in fact it cannot appear if the theory has space-time supersymmetry (as applies for the standard SUSY 10d heterotic string).

But one can also construct heterotic strings without supersymmetry, either in ten or in less than ten dimensions. In these cases tachyons typically do appear.
 
Now I am able to answer my question by myself.
The point is that the tachyon is the GROUND STATE of the string, which is a unique state. Thus, there is not a right-moving tachyon and a left-moving tachyon, but only one tachyon.
In the heterotic theory we have supersymmetry only in the right sector, so we can apply the GSO projection only in that sector, but the tachyon is a common state of BOTH sectors. Therefore, the GSO projection that removes tachyon from the right sector removes it also from the left sector as well.

Now it seems simple, but it took time until I realized that simple point. :)
 

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