Dualisation of the D = 9 matter coupled supergravity

@article{Yilmaz2005DualisationOT,
  title={Dualisation of the D = 9 matter coupled supergravity},
  author={Nejat Tevfik Yilmaz},
  journal={Journal of High Energy Physics},
  year={2005},
  volume={2005},
  pages={031-031}
}
  • N. T. Yilmaz
  • Published 15 June 2005
  • Physics
  • Journal of High Energy Physics
We perform the bosonic dualisation of the matter coupled = 1, D = 9 supergravity. We derive the Lie superalgebra which parameterizes the coset map whose Cartan form realizes the second-order bosonic field equations. Following the non-linear coset construction we present the first-order formulation of the bosonic field equations as a twisted self-duality condition. 
Nonlinear Realization of the {N}=2, D = 6 Supergravity
We have applied the method of dualisation to construct the coset realisation of the bosonic sector of the N=2, D=6 supergravity which is coupled to a tensor multiplet. The bosonic field equations areExpand
Nonlinear realization of pure N=4,D=5 supergravity
We perform the nonlinear realization or the coset formulation of the pure N=4, D=5 supergravity. We derive the Lie superalgebra which parameterizes a coset map whose induced Cartan-Maurer formExpand
Heterotic string dynamics in the solvable Lie algebra gauge
Abstract A revision of the toroidal Kaluza–Klein compactification of the massless sector of the E 8 × E 8 heterotic string is given. Under the solvable Lie algebra gauge the dynamics of the O ( p , qExpand
ON THE SYMMETRIC SPACE σ-MODEL KINEMATICS
The solvable Lie algebra parametrization of the symmetric spaces is discussed. Based on the solvable Lie algebra gauge two equivalent formulations of the symmetric space sigma model are studied.Expand

References

SHOWING 1-10 OF 23 REFERENCES
Dualisation of the D=7 Heterotic String
The dualisation and the first-order formulation of the D=7 abelian Yang-Mills supergravity which is the low energy effective limit of the D=7 fully Higssed heterotic string is discussed. TheExpand
Dualisation of the Salam-Sezgin D=8 Supergravity
The first-order formulation of the Salam–Sezgin D=8 supergravity coupled to N vector multiplets is discussed. The non-linear realization of the bosonic sector of the D=8 matter coupled Salam–SezginExpand
Hidden superconformal symmetry in M-theory
The bosonic sectors of the eleven-dimensional and IIA supergravity theories are derived as non-linear realisations. The underlying group includes the conformal group, the general linear group and asExpand
Dualisation of the symmetric space sigma model with couplings
Abstract The first-order formulation of the G / K symmetric space sigma model of the scalar cosets of the supergravity theories is discussed when there is coupling of ( m − 1 )-form matter fields.Expand
Dualisation of the General Scalar Coset in Supergravity Theories
The dualised formulation of the symmetric space sigma model is peformed for a general scalar coset G/K where G is a maximally non-compact group and K is it's maximal compact subgroup.By using theExpand
Supergravity in d=9 and its coupling to the non-compact σmodel
N=1 supergravity in d=9 coupled to n vector multiplets, each containing a real scalar, is constructed by the Noether method. It is shown that the scalars parametrise the coset space Hn=SO(n,1)/SO(n).
Kac-Moody symmetries of IIB supergravity
Abstract We formulate the bosonic sector of IIB supergravity as a non-linear realisation. We show that this non-linear realisation contains the Borel subalgebras of SL (11) and E 7 and argue that itExpand
The Complete N=2, D=10 Supergravity
The alternative N = 2, d = 10 supergravity, which is not derivable by dimensional reduction from the N = 1, d = 11 theory, is constructed at the full non-linear level. The transformation laws of theExpand
Covariant field equations of chiral N = 2 D = 10 supergravity
Even though chiral N = 2 D = 10 supergravity does not have a manifestly Lorentz-invariant action principle, it does have covariant field equations. The latter are obtained by first deriving the localExpand
Symmetries and Transformations of Chiral N=2 D=10 Supergravity
An SU(1,1) symmetry is identified in chiral N = 2, D = 10 supergravity. Complete supersymmetry transformation formulas are obtained for each of the fields in the theory in a covariant formalism withExpand
...
1
2
3
...