Emergence of L7-branes and fuzzy S in compactification scenarios of M(atrix) theory
نویسنده
چکیده
The M(atrix) theory contains membranes and longitudinal 5-branes (L5-branes) as extended objects. The transverse components of these brane solutions can be described by fuzzy CP (k = 1, 2), where k = 1 corresponds to spherical membranes and k = 2 to L5-branes of CP×S1 world-volume geometry. In addition to these, we show the existence of L7-branes of CP×S1 geometry, introducing extra potentials to the M(atrix) theory Lagrangian. As in the cases of k = 1, 2, these L7-branes (corresponding to k = 3) also break the supersymmetries of M(atrix) theory. The extra potentials are introduced such that the energy of a static L7-brane solution becomes finite in the large N limit. As a consequence, fluctuations from the static L7-branes are suppressed, which effectively describes compactification of M(atrix) theory down to 7 dimensions. We show that one of the extra potentials can be considered as a matrix-valued 7-form. The presence of the 7-form in turn supports a possibility of Freund-Rubin type compactification in M(atrix) theory. Compactification down to fuzzy S is also discussed and a realistic matrix model of M-theory in four dimensions is obtained. Current address: Cereja Technology Co., Ltd. 3-1 Tsutaya-Bldg. 5F, Shimomiyabi-cho Shinjuku-ku, Tokyo, 162-0822, Japan ([email protected])
منابع مشابه
Mixed Branes and M(atrix) Theory on Noncommutative Torus
We derive the noncommutative torus compactification of M(atrix) theory directly from the string theory by imposing mixed boundary conditions on the membranes. The relation of various dualities in string theory and M(atrix) theory compactification on the noncommutative torus are studied.
متن کاملEnhanced Gauge Symmetry in M(atrix) Theory
We discuss the origin of enhanced gauge symmetry in ALE (and K3) compactification of M theory, either defined as the strong coupling limit of the type IIa superstring, or as defined by Banks et al. In the D-brane formalism, wrapped membranes are D0 branes with twisted string boundary conditions, and appear on the same footing with the Kaluza-Klein excitations of the gauge bosons. In M(atrix) th...
متن کاملM ( atrix ) Theory on T 5 / Z 2 Orbifold and Five - Branes 1
We show that compactification of the M(atrix) theory on orbifold T5/Z2 is described by N = 8 supersymmetric quantum mechanics with USp(2N) gauge group and Spin(5)⊗Spin(4) R-symmetry. Using zero-brane and two-brane as probes, we find that each of the thirtytwo orbifold fixed points carry G-flux ∮ [G/2π] = −1/2. This anomalous G-flux is cancelled supersymmetrically by turning on sixteen longitudi...
متن کاملOrbifold and Five-branes
We study M(atrix) theory description of M theory compactified on T5/Z2 orbifold. In the large volume limit we show that M theory dynamics is described by N = 8 supersymmetric USp(2N) M(atrix) quantum mechanics. Via zero-brane parton scattering, we show that each orbifold fixed point carries anomalous G-flux ∮ [G/2π] = −1/2. To cancel the anomalous Gflux , we introduce twisted sector consisting ...
متن کاملInteractions of Eight-branes in String Theory and M(atrix) Theory
We consider eight-brane configurations in M(atrix) theory and compute their interaction potentials with gravitons, membranes, and four-branes. We compare these results with the interactions of D8-branes with D0-branes, D2-branes, and D4-branes in IIA string theory.
متن کامل