open/closed string duality



Duality in string theory

String theory



In string theory a given worldsheet with boundaries (Riemann surface with punctures) may typically be read in at least two different ways as describing either a closed string or an open string scattering-process.

graphics grabbed from Schomerus 07, Figure 4

But since the corresponding string scattering amplitude is the same no matter which perspective is taken, this exhibits an equivalence (“duality”) between these open- and closed string amplitudes.

For example, a cylinder worldsheet stretching between two D-brane worldvolumes manifestly represents equivalently the following two rather different-seeming string scattering-processes:

  1. a closed string emitted from one of the branes and absorbed by the other;

  2. an open string with ends on both branes going around a 1-loop vacuum diagram.

graphics grabbed from Schomerus 07, Figure 4, see also e.g. Peschanskia 09, Figure 1


  1. closed string excitations include gravitons inducing gravity

    (in the above example: the gravitational attraction between the two branes)

  2. open string excitations include gluons inducing the force described by Yang-Mills gauge fields –e.g. the strong nuclear force in quantum chromodynamics

    (in the above example: the worldvolume gauge field on coincident branes)

open/closed string duality implies gauge/gravity duality between these different effective field theories. This is exhibited by phenomena such as


In large NN limit and holography

Open/closed string duality plays a subtle role when interpreting the 't Hooft double line notation of gauge theory Feynman diagrams in the large N limit alternatively as open string or as closed string worldsheets (Gopakumar-Vafa 98, Gaiotto-Rastelli 03, Gopakumar 04).



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Last revised on May 19, 2020 at 15:36:28. See the history of this page for a list of all contributions to it.