T-duality
Builds on String theoryCirclePolyakov action
Definition
Consider closed bosonic string theory, with Regge slope , on the spacetime , where is a circle of radius . A closed string state has a momentum number , with momentum along the circle, a winding number , and oscillator levels . Its mass in the non-compact dimensions satisfies T-duality is the equivalence of the theory at radius with the theory at radius . It maps states by exchanging and and keeping and . On the worldsheet fields it acts by and on the left- and right-moving parts of the circle coordinate.
Remarks
Check on the spectrum: the mass formula and the condition are unchanged by together with . The duality also holds for interactions. Example: at the self-dual radius the map sends the theory to itself, and extra massless states appear, giving an enhanced gauge symmetry. Non-example: on a non-compact direction there are no winding states, and there is no T-duality in that direction. For open strings, T-duality exchanges Neumann and Dirichlet boundary conditions, and so relates D-branes of different dimensions. For type II superstrings, T-duality on one circle maps type IIA on radius to type IIB on radius . The Polyakov action gives the worldsheet theory on which the duality acts.
Reading path
To understand this page from the ground up, read these 4 pages in order. The foundations come first.
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- no evidence level
- Circle concept
- Polyakov action concept
- String theory concept
- T-duality definition
Further reading
About this page
| Tag | TJXVBG1TQJ |
|---|---|
| URI | m2://TJXVBG1TQJ |
| Kind | definition |
| Writing | W0 stub |
| MSC | 81T30, 83E30 |
| Defines | T-duality |
| Uses | String theory, Circle, Polyakov action |
| Changed | 3 November 2026 |
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