Noncommutative Tachyon Kinks as D$(p-1)$-branes from Unstable D$p$-brane

Details Noncommutative Tachyon Kinks as D$(p-1)$-branes from Unstable D$p$-brane Noncommutative Tachyon Kinks as D$(p-1)$-branes from Unstable D$p$-brane

2004-07-27

arxiv.org/abs/hep-th/0407229v2

JHEP 0501:023,2005

Physics

High Energy Physics

High Energy Physics - Theory

29 pages, references added

Scientific paper

10.1088/1126-6708/2005/01/023

We study noncommutative (NC) field theory of a real NC tachyon and NC U(1) gauge field, describing the dynamics of an unstable D$p$-brane. For every given set of diagonal component of open string metric $G_{0}$, NC parameter $\theta_{0}$, and interpolating electric field ${\hat E}$, we find all possible static NC kinks as exact solutions, in spite of complicated NC terms, which are classified by an array of NC kink-antikink and topological NC kinks. By computing their tensions and charges, those configurations are identified as an array of D0${\bar {\rm D}}$0 and single stable D0 from the unstable D1, respectively. When the interpolating electric field has critical value as $G_{0}^{2}={\hat E}^{2}$, the obtained topological kink becomes a BPS object with nonzero thickness and is identified as BPS D0 in the fluid of fundamental strings. Particularly in the scaling limit of infinite $\theta_{0}$ and vanishing $G_{0}$ and ${\hat E}$, while keeping $G_{0}\theta_{0}={\hat E}\theta_{0}=1$, finiteness of the tension of NC kink corresponds to tensionless kink in ordinary effective field theory. An extension to stable D$(p-1)$ from unstable D$p$ is straightforward for pure electric cases with parallel NC parameter and interpolating two-form field.

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