We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensions, and derive the SL(2, R) x O(6, 6 + n) transformations which leave the equations of motion invariant. For n = 0 SL(2, R) is also a symmetry of the action, but for n > 0 only those SL(2, R) transformations which act linearly on all fields leave the action invariant. The resulting four-dimensional theory is related to the bosonic part of the usual formulation of N = 4 supergravity coupled to matter by a duality transformation.</p
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We construct supersymmetric R+R4-actions in ten dimensions. Two invariants, of which the bosonic par...
We construct supersymmetric R+R4-actions in ten dimensions. Two invariants, of which the bosonic par...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
The symmetries of the tree level string effective action are discussed. An appropriate effective act...
The symmetries of the tree level string effective action are discussed. An appropriate effective act...
We show that the duality transformation relating the two versions of d=10, N=1 supergravity can be e...
Actions containing R2 terms in d = 4, N = 1 supergravity are constructed in the on-shell and the new...
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We construct supersymmetric R+R4-actions in ten dimensions. Two invariants, of which the bosonic par...
We construct supersymmetric R+R4-actions in ten dimensions. Two invariants, of which the bosonic par...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
We reduce the dual version of D = 10, N = 1 supergravity coupled to n vector fields to four dimensio...
The symmetries of the tree level string effective action are discussed. An appropriate effective act...
The symmetries of the tree level string effective action are discussed. An appropriate effective act...
We show that the duality transformation relating the two versions of d=10, N=1 supergravity can be e...
Actions containing R2 terms in d = 4, N = 1 supergravity are constructed in the on-shell and the new...
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimens...
We construct supersymmetric R+R4-actions in ten dimensions. Two invariants, of which the bosonic par...
We construct supersymmetric R+R4-actions in ten dimensions. Two invariants, of which the bosonic par...