E 10 and SO ( 9 , 9 ) invariant supergravity
نویسنده
چکیده
We show that (massive) D = 10 type IIA supergravity possesses a hidden rigid D 9 ≡ SO(9, 9) symmetry and a hidden local SO(9) × SO(9) symmetry upon dimensional reduction to one (time-like) dimension. We explicitly construct the associated locally supersymmetric Lagrangian in one dimension, and show that its bosonic sector, including the mass term, can be equivalently described by a truncation of an E 10 /K(E 10) non-linear σ-model to the level ℓ ≤ 2 sector in a decomposition of E 10 under its D 9 subalgebra. This decomposition is presented up to level ℓ = 10, and the even and odd level sectors are identified tentatively with the Neveu–Schwarz and Ramond sectors, respectively. Further truncation to the level ℓ = 0 sector yields a model related to the reduction of D = 10 type I supergravity. The hyperbolic Kac–Moody algebra DE 10 , associated to the latter, is shown to be a proper subalgebra of E 10 , in accord with the embedding of type I into type IIA supergravity. The corresponding decomposition of DE 10 under D 9 is presented up to level ℓ = 5.
منابع مشابه
Super D-branes
We present a manifestly Lorentz invariant, spacetime supersymmetric, and 'κ-invariant' worldvolume action for all type II Dirichlet p-branes, p ≤ 9, in a general type II supergravity background, including massive backgrounds in the IIA case. The p = 0, 2 cases are rederived from D=11. The p = 9 case provides a supersymmetrization of the D=10 Born-Infeld action.
متن کاملIia and Iib Spinors from K(e 10 )
We analyze the decomposition of recently constructed unfaithful spinor representations of K(E10) under its SO(9)×SO(9), and SO(9)×SO(2) subgroups, respectively, where K(E10) is the ‘maximal compact’ subgroup of the hyperbolic Kac–Moody group E10. We show that under these decompositions, respectively, one and the same K(E10) spinor gives rise to both the fermionic fields of IIA supergravity, and...
متن کاملar X iv : h ep - t h / 99 02 06 3 v 1 9 F eb 1 99 9 SU ( 2 ) Charges as Angular - momentum in N = 1 Self - dual Supergravity ∗
The N = 1 self-dual supergravity has SL(2,C) symmetry . This symmetry results in SU(2) charges as the angular-momentum. As in the nonsupersymmetric self-dual gravity, the currents are also of their potentials and are therefore identically conserved. The charges are generally invariant and gauge covariant under local SU(2) transforms approaching to be rigid at spatial infinity. The Poisson brack...
متن کاملar X iv : h ep - t h / 05 06 26 5 v 2 1 9 Ju l 2 00 5 UW / PT 05 - 15 hep - th / 0506265 Super Janus
We propose and study a supersymmetric version of the Janus domain wall solution of type IIB supergravity. Janus is dual to N = 4 super Yang Mills theory with a coupling constant that jumps across an interface. While the interface in the Janus field theory completely breaks all supersymmetries, it was found earlier that some supersymmetry can be restored in the field theory at the cost of breaki...
متن کاملar X iv : h ep - t h / 98 08 19 0 v 1 3 1 A ug 1 99 8 UFIFT - HEP - 98 - 22 M ( ysterious ) Patterns in SO ( 9 )
The light-cone little group, SO(9), classifies the massless degrees of freedom of eleven-dimensional supergravity, with a triplet of representations. We observe that this triplet generalizes to four-fold infinite families with the quantum numbers of massless higher spin states. Their mathematical structure stems from the three equivalent ways of embedding SO(9) into the exceptional group F4. To...
متن کامل