In this work, I study the deformation of the topological string by Ω¯, the complex conjugate of the Ω-deformation. Namely, I identify Ω¯ in terms of a physical state in the string spectrum and verify that the deformed Yang-Mills and ADHM actions are reproduced. This completes the study initiated in [1]where we show that Ω¯ decouples from the one-loop topological amplitudes in heterotic string theory. Simi-larly to the N=2*deformation, I show that the quadratic terms in the effective action play a crucial role in obtaining the correct realisation of the full Ω-deformation. Finally, I comment on the differences between the graviphoton and the Ω-deformation in general and discuss possible Ω¯ remnants at the boundary of the string moduli space
String theory on AdS3 with NS-NS fluxes admits a solvable irrelevant deformation which is close to t...
We investigate the “TT¯ ” deformations of two-dimensional supersymmetric quantum field theories. Mor...
It was recently shown that the $\mathcal{N}$ = 2 string topological amplitudes in the heterotic weak...
In this note, we study the deformation of the topological string by Ω¯. Namely, adopting the pertur...
In this note, we study the deformation of the topological string by Ω¯. Namely, adopting the perturb...
With the aim of providing a worldsheet description of the refined topological string, we continue th...
It is shown that the generating function of N = 2 topological strings, in the heterotic weak couplin...
30 pagesInternational audienceWith the aim of providing a worldsheet description of the refined topo...
With the aim of providing a worldsheet description of the refined topological string, we continue th...
AbstractWith the aim of providing a worldsheet description of the refined topological string, we con...
With the aim of providing a worldsheet description of the refined topological string, we continue th...
AbstractIn this paper, we explicitly construct string theory backgrounds that realise the so-called ...
The N = 2* supersymmetric gauge theory is a massive deformation of N = 4, in which the adjoint hyper...
The topological string captures certain superstring amplitudes which are also encoded in the underly...
In this work, we study a class of higher derivative couplings in the string effective action arising...
String theory on AdS3 with NS-NS fluxes admits a solvable irrelevant deformation which is close to t...
We investigate the “TT¯ ” deformations of two-dimensional supersymmetric quantum field theories. Mor...
It was recently shown that the $\mathcal{N}$ = 2 string topological amplitudes in the heterotic weak...
In this note, we study the deformation of the topological string by Ω¯. Namely, adopting the pertur...
In this note, we study the deformation of the topological string by Ω¯. Namely, adopting the perturb...
With the aim of providing a worldsheet description of the refined topological string, we continue th...
It is shown that the generating function of N = 2 topological strings, in the heterotic weak couplin...
30 pagesInternational audienceWith the aim of providing a worldsheet description of the refined topo...
With the aim of providing a worldsheet description of the refined topological string, we continue th...
AbstractWith the aim of providing a worldsheet description of the refined topological string, we con...
With the aim of providing a worldsheet description of the refined topological string, we continue th...
AbstractIn this paper, we explicitly construct string theory backgrounds that realise the so-called ...
The N = 2* supersymmetric gauge theory is a massive deformation of N = 4, in which the adjoint hyper...
The topological string captures certain superstring amplitudes which are also encoded in the underly...
In this work, we study a class of higher derivative couplings in the string effective action arising...
String theory on AdS3 with NS-NS fluxes admits a solvable irrelevant deformation which is close to t...
We investigate the “TT¯ ” deformations of two-dimensional supersymmetric quantum field theories. Mor...
It was recently shown that the $\mathcal{N}$ = 2 string topological amplitudes in the heterotic weak...