nLab non-critical string

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Context

String theory

Physics

physics, mathematical physics, philosophy of physics

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theory (physics), model (physics)

experiment, measurement, computable physics

Gravity

Quantum field theory

Higher spin geometry

Elliptic cohomology

Contents

Idea

For both the bosonic string and the superstring, the corresponding Polyakov action has a gauge anomaly for the conformal symmetry, depending on the dimension DD of target spacetime, and on the strength of the dilaton background field. For vanishing dilaton field this anomaly vanishes exactly for D=26D = 26 for the bosonic model, and in D=10D = 10 for the superstring. String theories at these dimensions are known as critical string theories. By contrast, string theories in dimensions different from these are known as non-critical string theories.

Often, the term “non-critical” string is used to refer to a string theory formulated on dimensions less than the critical dimensions. However, it is also possible to consider theories in dimensions greater than the critical dimensions, provided an appropriate dilaton profile is used. In this way, one may more precisely speak of subcritical and supercritical strings.

Subcritical strings

(some motivation, e.g. an alternative to compactifications)

Supercritical strings

Hellerman 04 motivates looking at supercritical heterotic strings by conjecturing an S-duality between these and type I string theory with additional D9 brane-antibrane pairs.

References

General non-critical strings

Subcritical strings

Supercritical strings

Last revised on March 25, 2025 at 19:46:10. See the history of this page for a list of all contributions to it.