Types of quantum field thories
abstract duality: opposite category,
The term S-duality can mean two different things:
In the original and restricted sense, S-duality refers to the conjectured Montonen-Olive duality auto-equivalence of (super) Yang-Mills theory in 4 dimensions under which the coupling constant is inverted, and more generally under which the combined coupling constant and theta angle tranform under an action of the modular group. At least for super Yang-Mills theory this conjecture can be argued for in detail.
There is also a duality in string theory called S-duality. Specifically in type IIB superstring theory/F-theory this is given by an action of the modular group on the axio-dilaton, hence is, via the proportionality of the dilatorn to the string coupling constant, again a weak-strong coupling duality.
Indeed, at least for super Yang-Mills theory Montonen-Olive S-duality may be understood as a special case of the string duality (Witten 95a, Witten 95b): one may understand N=2 D=4 super Yang-Mills theory as the KK-compactification of the M5-brane 6d (2,0)-superconformal QFT on the F-theory torus (Johnson 97) to get the D3-brane worldvolume theory, and the remnant modular group action on the compactified torus is supposed to be the 4d Montonen-Olive S-duality (Witten 07).
In its original form, S-duality refers to Montonen-Olive duality , which is about the following phenomenon:
each pairing the curvature 2-form with itself in an invariant polynomial, but the first involving the Hodge star operator dual, and the second not. One can combine the coefficients and into a single complex number
Montonen-Olive duality asserts that the quantum field theories induced from one such parameter value and another one obtained from it by an action of on the upper half plane are equivalent.
This is actually not quite true for ordinary Yang-Mills theory, but seems to be true for N=2 D=4 super Yang-Mills theory.
In (Witten 95a, Witten 95b, Witten 07) it was suggested that the above S-duality of N=2 D=4 super Yang-Mills theory may be understood geometrically by regarding the super Yang-Mills theory as the Kaluza-Klein compactification of the 6d (2,0)-superconformal QFT – that instead of a gauge field given by a principal bundle with connection involves a principal 2-bundle with 2-connection – on a complex torus. The -invariance of the resulting 4-dimensional theory is then the modular group remnant of the conformal invariance of the 6-dimensional theory under conformal transformations of that torus.
Moreover, Witten has suggested that this S-duality secretly drives a host of other subtle phenomena, notably that the geometric Langlands duality (see there for more) is just an aspect of a special case of this.
The AGT correspondence refines this further and regards the 6d (2,0)-superconformal QFT as something like a “2d SCFT with values in 4d super-Yang-Mills theories”. This way the whole mapping class group of general 2d Riemann surfaces acts as a generalized S-duality on 4d super-Yang-Mills theory
Type IIB string theory is obtained by KK-compactification of M-theory on a torus bundle followed by T-dualizing one of the torus cycles. This perspective – referred to as F-theory – exhibits the axio-dilaton of type IIB string theory as the fiber of an elliptic fibration (essentially the torus bundle that M-theory was compactified on (Johnson 97)).
The type IIB F1-string and the D1-brane appear this way by double dimensional reduction from the M2-brane wrapping (either) one of the two cycles of the compactifying torus. S-duality mixes these strings by the evident modular group action on the labels of the (p,q)-strings. Here at least part of the S-duality action on -strings may be seen as a system of autoequivalences of the super L-infinity algebras which defines the extended super spacetime constituted by the type II superstring (Bandos 00, FSS 13, section 4.3).
Similarly the D5-brane and the NS5-brane are the double dimensional reduction of the M5-brane wrapping one of the two cycles of the compactifying torus, and hence the S-duality modular group also acts on -5-branes, exchanging them.
Finally, the D3-brane is instead the double dimensional reduction of the M5-brane, wrapping both compactifying dimensions. Accordingly the worldvolume theory of the D3, which is super Yang-Mills theory in has an S-self-duality. That is supposed to be the Montonen-Olive duality discussed above, which is thereby unified with type IIB S-duality.
While F-theory does capture much of this non-perturbative S-duality, there currently remains a puzzle as to the correct differential cohomology nature of all the fields under S-duality: by the above S-duality mixes the Kalb-Ramond field with the degree-3 component of the RR-field. But the best available description of the fine-structure of these fields is (see also at orientifold) that is a cocycle in (twisted) ordinary differential cohomology while is (only) one component of a cocycle in (twisted) KU (or really: KR-theory).
This issue was first highlighted in (DMW 00, section 11). In (DFM 03, section 9) it was observed that taking into account the cubical structure in M-theory on the 11-dimensional Chern-Simons term of the supergravity C-field the conceptual mismatch is alleviated, but not quite resolved. See also (BEJVS 05)
On the other hand, as discussed at cubical structure in M-theory, this structure plausibly relates to a generalized cohomology theory beyond ordinary cohomology and beyond K-theory, namely to elliptic cohomology/tmf. Hints like this led in (KrizSati 05) to the conjecture that the right cohomology theory to capture the S-duality of type IIB/F-theory is modular equivariant elliptic cohomology.
Something substantial should go here, for the moment the following is copied from a discussion forum comment by some Olof here:
For the Het/I relation, the first observation is that the massless spectra of the two models agree. Moreover, if we make the identification
the low energy effective supergravity actions of the two models match. Since the string coupling constants and are given as the expectation values of the exponentials of the dilatons and , respectively, the above equations relates the type-I theory at strong coupling to the heterotic theory at weak coupling:
From the relative scaling of the metric in (1) we also see that the string length in the two theories are related by
As a non-perturbative check we can consider the tension of the type-I D1 brane. The brane is a BPS object, so for all values of the coupling the tension is given by the same formula
where I’ve used relations (2) and (3). But this is equal to the tension of the fundamental heterotic string
This indicates that it is sensible to identify the strong coupling limit of the type-I D1 brane with the heterotic string.
A priori type IIA superstring theory does not have S-duality, but by compactifying M-theory on a torus one can sort of read off what the non-perturbative additions to type IIA should be that make it have S-duality after all, see
|reduction from 11d||electric σ-model||weak/strong coupling duality||magnetic σ-model|
|M2-brane in 11d sugra EFT||electric-magnetic duality||M5-brane in 11d sugra EFT|
|on orientifold K3||on orientifold K3|
|F1-brane in heterotic supergravity||S-duality||black string in heterotic sugra|
|on orientifold T4||on orientifold T4|
|F1-brane in heterotic supergravity||S-duality||black string in type IIA sugra|
|on K3||on K3|
|F1-brane in IIA sugra||S-duality||black string in heterotic sugra|
|F1-brane in IIA sugra||S-duality||black string in type IIA sugra|
|F1-brane in IIB sugra||S-duality||D1-brane in 10d IIB sugra|
|D3-brane in IIB sugra||S-duality||D3-brane in IIB sugra|
|M-theory perspective via AdS7-CFT6||F-theory perspective|
|Kaluza-Klein compactification on||compactificationon elliptic fibration followed by T-duality|
|7-dimensional Chern-Simons theory|
|AdS7-CFT6 holographic duality|
|6d (2,0)-superconformal QFT on the M5-brane with conformal invariance||M5-brane worldvolume theory|
|KK-compactification on Riemann surface||double dimensional reduction on M-theory/F-theory elliptic fibration|
|N=2 D=4 super Yang-Mills theory with Montonen-Olive S-duality invariance; AGT correspondence||D3-brane worldvolume theory with type IIB S-duality|
|topologically twisted N=2 D=4 super Yang-Mills theory|
|KK-compactification on Riemann surface|
|A-model on , Donaldson theory|
|gauge theory induced via AdS5-CFT4|
|type II string theory|
|Kaluza-Klein compactification on|
|5-dimensional Chern-Simons theory|
|AdS5-CFT4 holographic duality|
|N=4 D=4 super Yang-Mills theory|
|topologically twisted N=4 D=4 super Yang-Mills theory|
|KK-compactification on Riemann surface|
|A-model on and B-model on , geometric Langlands correspondence|
It was originally noticed in
This led to the electric/magnetic duality conjecture formulation in
See also the references at electro-magnetic duality.
The insight that the Montonen-Olive duality works more naturally in super Yang-Mills theory is due to
and that it works particularly for N=4 D=4 super Yang-Mills theory is due to
The observation that the electric/magnetic duality extends to an -action in this case is due to
John Cardy, E. Rabinovici, Phase Structure Of Zp Models In The Presence Of A Theta Parameter, Nucl. Phys. B205 (1982) 1-16;
John Cardy, Duality And The Theta Parameter In Abelian Lattice Models, Nucl. Phys. B205 (1982) 17-26.
A. Shapere and Frank Wilczek, Selfdual Models With Theta Terms, Nucl. Phys. B320 (1989) 669-695.
The suggestion of an -duality action in type II superstring theory goes back to
Duality Symmetric Actions, Nucl. Phys. B411 (1994) 35-63 (arXiv:hep-th/9304154)
A textbook account is in
A 2-loop test is in
The cohomological problem of the type II S-duality action on the 3-form flux was originally highlighted in
The conjecture that with combined targetspace/worldsheet modular transformations the type IIB S-duality is reflected in modular equivariant elliptic cohomology is due to
The relation of S-duality to geometric Langlands duality was understood in
Exposition of this is in