# D2-D8 system with massive strings and the Lifshitz spacetimes

@article{Singh2017D2D8SW, title={D2-D8 system with massive strings and the Lifshitz spacetimes}, author={Harvendra Singh}, journal={Journal of High Energy Physics}, year={2017}, volume={2017}, pages={1-18} }

A bstractThe Romans’ type IIA supergravity allows fundamental strings to have explicit mass term at the tree level. We show that there exists a (F1,D2,D8) brane configuration which gives rise to Lif4(2) × R1 × S5 vacua supported by the massive strings. The presence of D8-branes naturally excites massive fundamental strings. A compactification on circle relates these Lifshitz massive type-IIA background with the axion-flux Lif4(2) × S1 × S5 vacua in ordinary type-IIB theory. The massive T…

## 4 Citations

### RG flows and cascades of Lif4(2) × S1 × S5 vacua

- PhysicsJournal of High Energy Physics
- 2018

A bstractThe (F1,D2,D8) brane configuration produces Lif4(2) × S1 × S5 Lifshitz vacua supported by ‘massive’ B-field. We present exact deformations of this system under which new massless B-modes of…

### More on entanglement properties of $Lif_4^{(2)}\times {S}^1\times S^5$ spacetime with string excitations

- Physics
- 2022

The Lif (2)4 × S 1 × S 5 spacetime is an exact solution of F 1 − D 2 − D 8 conﬁguration in type IIA supergravity and can accommodate charged excitations of the fundamental string. By gauge/gravity…

### Entanglement entropy at higher orders for the states of a = 3 θ = 1 Lifshitz theory

- PhysicsNuclear Physics B
- 2019

### Holographic entanglement entropy for Lif4(2)×S1×S5 spacetime with string excitations

- Physics
- 2021

The $(F1,D2,D8)$ brane configuration with $Li{f}_{4}^{(2)}\ifmmode\times\else\texttimes\fi{}{S}^{1}\ifmmode\times\else\texttimes\fi{}{S}^{5}$ geometry is a known Lifshitz vacua supported by massive…

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