The presence of a constant background antisymmetric tensor for open strings or D-branes forces the space-time coordinates to be noncommutative. This effect is equivalent to replacing ordinary products in the effective theory by the deformed star product. An immediate consequence of this is that all fields get complexified. The only possible noncommutative Yang-Mills theory is the one with U(N) gauge symmetry. By applying this idea to gravity one discovers that the metric becomes complex. We show in this article that this procedure is completely consistent and one can obtain complexified gravity by gauging the symmetry $U(1,D-1)$ instead of the usual $SO(1,D-1)$. The final theory depends on a Hermitian tensor containing both the symmetric me...
We illustrate the various ways in which the algebraic framework of noncommutative geometry naturally...
Noncommutative gravity in three dimensions with vanishing cosmological constant is examined. We find...
We do not know the symmetries underlying string theory. Furthermore, there must exist an inherently ...
The presence of a constant background antisymmetric tensor for open strings or D-branes forces the s...
The possible role of gravity in a noncommutative geometry is investigated. Due to the Moyal *-produc...
We review some aspects of the implementation of spacetime symmetries in noncommutative field theorie...
Two main problems face the construction of noncommutative actions for gravity with star products: th...
We apply noncommutative geometry to a system of N parallel D-branes, which is interpreted as a quant...
The extension of the noncommutative u*(N) Lie algebra to noncommutative orthogonal and symplectic Li...
Noncommutative gravity in three dimensions with no cosmological constant is reviewed. We find a solu...
We consider open strings ending on D-branes in the presence of constant metric, G, antisymmetric ten...
In this paper we consider the quantization of open strings ending on D-branes with a background B fi...
Noncommutative gauge theories can be constructed from ordinary U(∞) gauge theories in lower dimensio...
In this paper the noncommutative gravity is treated as a gauge theory ofthe noncommutative SO(2; 3)*...
In this work, we calculate the leading order corrections to general relativity formulated on a canon...
We illustrate the various ways in which the algebraic framework of noncommutative geometry naturally...
Noncommutative gravity in three dimensions with vanishing cosmological constant is examined. We find...
We do not know the symmetries underlying string theory. Furthermore, there must exist an inherently ...
The presence of a constant background antisymmetric tensor for open strings or D-branes forces the s...
The possible role of gravity in a noncommutative geometry is investigated. Due to the Moyal *-produc...
We review some aspects of the implementation of spacetime symmetries in noncommutative field theorie...
Two main problems face the construction of noncommutative actions for gravity with star products: th...
We apply noncommutative geometry to a system of N parallel D-branes, which is interpreted as a quant...
The extension of the noncommutative u*(N) Lie algebra to noncommutative orthogonal and symplectic Li...
Noncommutative gravity in three dimensions with no cosmological constant is reviewed. We find a solu...
We consider open strings ending on D-branes in the presence of constant metric, G, antisymmetric ten...
In this paper we consider the quantization of open strings ending on D-branes with a background B fi...
Noncommutative gauge theories can be constructed from ordinary U(∞) gauge theories in lower dimensio...
In this paper the noncommutative gravity is treated as a gauge theory ofthe noncommutative SO(2; 3)*...
In this work, we calculate the leading order corrections to general relativity formulated on a canon...
We illustrate the various ways in which the algebraic framework of noncommutative geometry naturally...
Noncommutative gravity in three dimensions with vanishing cosmological constant is examined. We find...
We do not know the symmetries underlying string theory. Furthermore, there must exist an inherently ...