2001
DOI: 10.1088/1126-6708/2001/06/023
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Non-abelian brane intersections

Abstract: We study new solutions of the low-energy equations of motion for the non-abelian D-string. We find a "fuzzy funnel" solution consisting of a noncommutative four-sphere geometry which expands along the length of the D-string. We show that this funnel solution has an interpretation as D-strings ending on a set of orthogonal D5-branes. Although not supersymmetric, the system appears to be stable within this framework. We also give a dual description of this configuration as a bion spike in the non-abelian world v… Show more

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Cited by 114 publications
(284 citation statements)
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References 43 publications
(186 reference statements)
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“…For a detailed description of these constructions we refer the interested reader to [31,32,11] and the references therein In terms of the physical radius we find a similar relationship to the case of the SU(2) algebra, where we write 3) note that in this instance R must be positive definite and the Casimir is given by products of the G i , as usual, where we have…”
Section: Higher (Even) Dimensional Fuzzy Spheresmentioning
confidence: 64%
“…For a detailed description of these constructions we refer the interested reader to [31,32,11] and the references therein In terms of the physical radius we find a similar relationship to the case of the SU(2) algebra, where we write 3) note that in this instance R must be positive definite and the Casimir is given by products of the G i , as usual, where we have…”
Section: Higher (Even) Dimensional Fuzzy Spheresmentioning
confidence: 64%
“…Indeed, given that this solution is static, one can immediately derive its energy from the full non-Abelian DBI action of a stack of N D6-branes extended along σ. Remarkably, this energy density can be expressed as the square root of a sum of perfect squares [20]: 6) where STr denotes the symmetrized trace [14,21,22]. Thus any solution of (3.3)-(3.4) sets the first square to zero and, as one expects for supersymmetric solutions, also satisfies the full non-Abelian equations of motion [15].…”
Section: Jhep11(2016)179mentioning
confidence: 97%
“…In these cases the large-N limit often has some sort of abelian geometrical description. For the leading large-N in these cases the ordering of Matrices does not matter and, at the level of classical equations of motion, the system can be compared with an abelian dual [10,11]. Here we have extended the comparison to fluctuations and found agreement.…”
Section: Discussion and Outlookmentioning
confidence: 58%
“…Related systems involve D1⊥D3 brane intersections [7,8,9]. Equivalence at the level of classical solutions exists in a large class of examples [5,10,11] including higher dimensional fuzzy spheres [12,13,14,15,16]. It is natural to explore whether the equivalence at the level of classical solutions extends to an equivalence at the level of quadratic fluctuations.…”
Section: Introductionmentioning
confidence: 99%