Abstract
Abstract
The (F1,D2,D8) brane configuration produces Lif
4
(2)
× S
1 × S
5 Lifshitz vacua supported by ‘massive’ B-field. We present exact deformations of this system under which new massless B-modes of strings also get excited. Due to these massless modes the deformed solutions flow to conformally Lif
4
(3)
× S
1 × S
5 vacua in the IR. The latter types are supersymmetric solutions of ordinary type IIA theory. The massive and massless B
μν
modes segregate out in the IR. We confirm that the massive B mode and cosmological constant indeed decouple from the theory rendering the IR field dynamics controlled by massless fields only. A similar effect is observed on the UV side of the flow where a relativistic regime reappears. We also present ‘cascading’ Lifshitz vacua in which dynamical exponent has integral jumps along the flow; Lif
4
(3)
→ Lif
4
(2)
→ Lif
4
(1)
. The critical Lif
4
(2)
theory separates ‘deconfining’ Lif
4
(3)
IR theory from the confining Yang-Mills phase in UV.
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
Cited by
2 articles.
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