Using the parallelizing S 7 torsion as an ansatz we investigate wo solutions of gauged N = 8 supergravity with SO(7) invariance. Supersymmetry is uniformly broken. We calculate the masses for these.solutions which are both unstable. Certain apparent discrepancies with the results obtained by spontaneous compactification f d = 11 supergravity are discussed. We establish that the compactification the parallelized S7 has an SO(7) invariancc and clarify the issue of supersymmetry breaking. The lack of stability in d=4 indicates that this d = 11 solution is unstable. 1
The complete structure of N = 8 supergravity is presented with an optional local SO(8) invariance. T...
The complete structure of N = 8 supergravity is presented with an optional local SO(8) invariance. T...
We find a new SO(7) invariant solution of d = 11 supergravity by exploiting the relationship of this...
Using the parallelizing S7 torsion as an ansatz we investigate two solutions of gauged N=8 supergrav...
Using the parallelizing S7 torsion as an ansatz we investigate two solutions of gauged N=8 supergrav...
Using the parallelizing S7 torsion as an ansatz we investigate two solutions of gauged N=8 supergrav...
Gauged N = 8 supergravity emerges from spontaneous compactification of eleven-dimensional supergravi...
Gauged N = 8 supergravity emerges from spontaneous compactification of eleven-dimensional supergravi...
We investigate several aspects of the embedding of gauged N = 8 supergravity into d = 11 supergravit...
We investigate several aspects of the embedding of gauged N = 8 supergravity into d = 11 supergravit...
We find a new SO(7) invariant solution of d = 11 supergravity by exploiting the relationship of this...
We find a new SO(7) invariant solution of d = 11 supergravity by exploiting the relationship of this...
Gauged N = 8 supergravity emerges from spontaneous compactification of eleven-dimensional supergravi...
The complete structure of N = 8 supergravity is presented with an optional ocal SO(8) invariance. Th...
We investigate several aspects of the embedding of gauged N = 8 supergravity into d = 11 supergravit...
The complete structure of N = 8 supergravity is presented with an optional local SO(8) invariance. T...
The complete structure of N = 8 supergravity is presented with an optional local SO(8) invariance. T...
We find a new SO(7) invariant solution of d = 11 supergravity by exploiting the relationship of this...
Using the parallelizing S7 torsion as an ansatz we investigate two solutions of gauged N=8 supergrav...
Using the parallelizing S7 torsion as an ansatz we investigate two solutions of gauged N=8 supergrav...
Using the parallelizing S7 torsion as an ansatz we investigate two solutions of gauged N=8 supergrav...
Gauged N = 8 supergravity emerges from spontaneous compactification of eleven-dimensional supergravi...
Gauged N = 8 supergravity emerges from spontaneous compactification of eleven-dimensional supergravi...
We investigate several aspects of the embedding of gauged N = 8 supergravity into d = 11 supergravit...
We investigate several aspects of the embedding of gauged N = 8 supergravity into d = 11 supergravit...
We find a new SO(7) invariant solution of d = 11 supergravity by exploiting the relationship of this...
We find a new SO(7) invariant solution of d = 11 supergravity by exploiting the relationship of this...
Gauged N = 8 supergravity emerges from spontaneous compactification of eleven-dimensional supergravi...
The complete structure of N = 8 supergravity is presented with an optional ocal SO(8) invariance. Th...
We investigate several aspects of the embedding of gauged N = 8 supergravity into d = 11 supergravit...
The complete structure of N = 8 supergravity is presented with an optional local SO(8) invariance. T...
The complete structure of N = 8 supergravity is presented with an optional local SO(8) invariance. T...
We find a new SO(7) invariant solution of d = 11 supergravity by exploiting the relationship of this...