nLab U-duality

Contents

Context

Duality in string theory

String theory

Group Theory

Contents

Idea

U-duality is a kind of duality in string theory.

The KK-compactifications of 11-dimensional supergravity to lower dimensional gauged supergravity theories have global/local gauge groups given by split real forms of the EE-series of the exceptional Lie groups.

Here the compact exceptional Lie groups form a series E8,E7, E6

E 8,E 7,E 6 E_8, E_7, E_6

which is usefully thought of to continue as

E 5Spin(10),E 4SU(5),E 3SU(3)×SU(2). E_5 \coloneqq Spin(10), E_4 \coloneqq SU(5), E_3 \coloneqq SU(3) \times SU(2) \,.

(Notice that E 4E_4, E 5E_5 and E 6E_6 are also the traditional choices for phenomenologically realistic grand unified theories, see there for more.)

The split real forms of this are traditionally written

E 8(8),E 7(7),E 6(6) E_{8(8)}, E_{7(7)}, E_{6(6)}

and one sets

E 5(5)Spin(5,5),E 4(4)SL(5,),E 3(3)SL(3,)×SL(2,). E_{5(5)} \coloneqq Spin(5,5), E_{4(4)} \coloneqq SL(5, \mathbb{R}), E_{3(3)} \coloneqq SL(3, \mathbb{R}) \times SL(2, \mathbb{R}) \,.

For instance the scalar fields in the field supermultiplet of 3d113 \leq d \leq 11-dimensional supergravity have moduli spaces parameterized by the homogeneous spaces

E n(n)/K n E_{n(n)}/ K_n

for

n=11d, n = 11 - d \,,

where K nK_n is the maximal compact subgroup of E n(n)E_{n(n)}:

K 8Spin(16),K 7SU(8),K 6Sp(4) K_8 \simeq Spin(16), K_7 \simeq SU(8), K_6 \simeq Sp(4)
K 5Spin(5)×Spin(5),K 4Spin(5),K 3SU(2)×SO(2). K_5 \simeq Spin(5) \times Spin(5), K_4 \simeq Spin(5), K_3 \simeq SU(2) \times SO(2) \,.

Therefore E n(n)E_{n(n)} acts as a global symmetry on the supergravity fields and more generally certain subgroups of it are “gauged” (have gauge fields) in gauged supergravity version.

So for instance maximal 3d supergravity has global (and in fact also local, see there) gauge group given by (the split real form of) E8.

This is no longer verbatim true for their UV-completion by the corresponding compactifications of string theory (e.g. type II string theory for type II supergravity, etc.). Instead, on these a discrete subgroup

E n(n)()E n(n) E_{n(n)}(\mathbb{Z}) \hookrightarrow E_{n(n)}

acts as global symmetry. This is called the U-duality group of the supergravity theory.

It has been argued that this pattern should continue in some way further to the remaining values 0d<30 \leq d \lt 3, with “Kac-Moody groupsE9, E10, E11 corresponding to the Kac-Moody algebras

𝔢 9,𝔢 10,𝔢 11. \mathfrak{e}_9, \mathfrak{e}_10, \mathfrak{e}_{11} \,.

Continuing in the other direction to d=10d = 10 (n=1n = 1) connects to the T-duality group O(d,d,)O(d,d,\mathbb{Z}) of type II string theory.

supergravity gauge group (split real form)T-duality group (via toroidal KK-compactification)U-dualitymaximal gauged supergravity
SL(2,)SL(2,\mathbb{R})1 SL ( 2 , ) SL(2,\mathbb{Z}) S-dualityD=10 type IIB supergravity
SL(2,)×(2,\mathbb{R}) \times O(1,1) 2\mathbb{Z}_2 SL ( 2 , ) SL(2,\mathbb{Z}) × 2\times \mathbb{Z}_2D=9 supergravity
SU(3)×\times SU(2)SL(3,)×SL(2,)(3,\mathbb{R}) \times SL(2,\mathbb{R})O(2,2;)O(2,2;\mathbb{Z})SL(3,)×SL(2,)SL(3,\mathbb{Z})\times SL(2,\mathbb{Z})D=8 supergravity
SU(5)SL(5,)SL(5,\mathbb{R})O(3,3;)O(3,3;\mathbb{Z})SL(5,)SL(5,\mathbb{Z})D=7 supergravity
Spin(10)Spin(5,5)Spin(5,5)O(4,4;)O(4,4;\mathbb{Z})O(5,5,)O(5,5,\mathbb{Z})D=6 supergravity
E₆E 6(6)E_{6(6)}O(5,5;)O(5,5;\mathbb{Z})E 6(6)()E_{6(6)}(\mathbb{Z})D=5 supergravity
E₇E 7(7)E_{7(7)}O(6,6;)O(6,6;\mathbb{Z})E 7(7)()E_{7(7)}(\mathbb{Z})D=4 supergravity
E₈E 8(8)E_{8(8)}O(7,7;)O(7,7;\mathbb{Z})E 8(8)()E_{8(8)}(\mathbb{Z})D=3 supergravity
E₉E 9(9)E_{9(9)}O(8,8;)O(8,8;\mathbb{Z})E 9(9)()E_{9(9)}(\mathbb{Z})D=2 supergravityE₈-equivariant elliptic cohomology
E₁₀E 10(10)E_{10(10)}O(9,9;)O(9,9;\mathbb{Z})E 10(10)()E_{10(10)}(\mathbb{Z})
E₁₁E 11(11)E_{11(11)}O(10,10;)O(10,10;\mathbb{Z})E 11(11)()E_{11(11)}(\mathbb{Z})

(Hull-Townsend 94, table 1, table 2)

More generally, there is a “magic pyramid” of super-Einstein-Yang-Mills theories and their U-duality groups.

Properties

Relation to T-duality and S-duality

U-duality may be understood as being the combination of T-duality for the compactification torus and S-duality of type IIB superstring theory. see (West 12, section 17.5.4).

References

General

The hidden global E7-symmetry (and local K(E 7)SU(8)K(E_7) \simeq SU(8)-symmetry) of the KK-compactification of 11-dimensional supergravity on a 7-dimensional torus to D=4 N=8 supergravity was first realized

and the hidden global E8-symmetry (and local K(𝔢 8)𝔰𝔬 16K(\mathfrak{e}_8) \simeq \mathfrak{so}_{16}-symmetry) in

See also:

The concept and terminology of U-duality in string theory/M-theory originates with:

Discussion via the BFSS matrix model:

Early review:

Monographs:

Systematization of U-duality via the relation between supersymmetry and division algebras and the Freudenthal magic square is due to

Quick surveys include

Reviews focusing on gauged supergravity and the non-discrete duality groups include

with slides in

Further discussion with an eye towards M-theory:

Discussion in line with the F-theory perspective on the SL(2,)SL(2,\mathbb{Z})-S-duality – namely “F'-theory” – is in

Discussion of 11-dimensional supergravity in a form that exhibits the higher U-duality groups already before KK-compactification, via a kind of exceptional generalized geometry,is in

Review of U-duality and exceptional generalized geometry in KK-compactification of D=11 supergravity:

On U-duality (and possibly mysterious duality) via Hypothesis H as automorphisms of iterated (rational) cyclic loop spaces of the (rational) 4-sphere:

review in:

n=3n=3

The case of SL(3,)×SL(2,)SL(3,\mathbb{Z}) \times SL(2,\mathbb{Z}) in 8d supergravity is discussed in

n=4n=4

The case of SL(5,)SL(5,\mathbb{Z}) in 7d supergravity from M-theory is discussed in

n=7n=7

The E 7(7)E_{7(7)}-symmetry was first discussed in

n=8n=8

The case of E 8(8)E_{8(8)} is discussed in

n=9n=9

The case of E9 is discussed in

n=10n=10

The case of E10 is discussed for bosonic degrees of freedom in

and for fermionic degrees of freedom

and for supersymmetric quantum cosmology in

Review includes

Discussion of phenomenology:

n=11n=11

The case of of E11 is discussed in

Further details

A careful discussion of the topology of the Kac-Moody U-duality groups is in

A discussion in the context of generalized complex geometry / exceptional generalized complex geometry is in

  • Paulo Pires Pacheco, Daniel Waldram, M-theory, exceptional generalised geometry and superpotentials (arXiv:0804.1362)

  • Nicholas Houston, Supergravity and Generalized Geometry Thesis (2010) (pdf)

General discussion of the Kac-Moody groups arising in this context is for instance in

Relation to automorphic forms

String theory partition functions as automorphic forms for U-duality groups are discussed in

  • Michael Green, Jorge G. Russo, Pierre Vanhove, Automorphic properties of low energy string amplitudes in various dimensions (arXiv:1001.2535)

Last revised on November 5, 2024 at 15:36:17. See the history of this page for a list of all contributions to it.