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Related papers: Abelian M5-brane on $S^6_q$

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We study dimensional reduction of M5 branes on a circle bundle when the supersymmetry parameter is not constant along the circle. When the gauge group is Abelian and the fields appear quadratically in the Lagrangian, we can always obtain a…

High Energy Physics - Theory · Physics 2022-03-02 Andreas Gustavsson

The effect of a co--dimension--2 spherical monodromy defect on the free--field theory of a conformal scalar is investigated. The conformal anomaly is computed (in two ways) and thence the R\'enyi and entanglement entropies. The $C_T$…

High Energy Physics - Theory · Physics 2022-01-11 J. S. Dowker

We discuss several mechanisms to cancel the anomalies of a 5-brane embedded in M-theory. Two of them work, provided we impose suitable conditions either on the 11-dimensional manifold of M-theory or on the 4-form field strength of M-theory.

High Energy Physics - Theory · Physics 2010-02-04 L. Bonora , C. S. Chu , M. Rinaldi

We consider two supersymmetric M5 brane probe solutions in $\textrm{AdS}_7 \times S^4$ and one in $\textrm{AdS}_4 \times S^7$ that all have the $\textrm{AdS}_3 \times S^3$ world-volume geometry. The values of the classical action of the…

High Energy Physics - Theory · Physics 2025-01-09 Matteo Beccaria , Lorenzo Casarin , Arkady A. Tseytlin

Abelian gerbes and twisted bundles describe the topology of the NS-NS 3-form gauge field strength H. We review how they have been usefully applied to study and resolve global anomalies in open string theory. Abelian 2-gerbes and twisted…

High Energy Physics - Theory · Physics 2008-11-26 Paolo Aschieri , Branislav Jurco

Renyi entropy and central charge, $C_T$, are calculated for a coexact p--form on an even sphere with particular reference to the conformally invariant case. It is shown, for example, that the entanglement entropy is minus the standard…

High Energy Physics - Theory · Physics 2017-06-23 J. S. Dowker

We consider the non-abelian theory (http://arxiv.org/abs/arXiv:1203.4224) for an arbitrary number $N_5$ of five-branes and construct self-dual string solution with an arbitrary $N_2$ unit of self-dual charges. This generalizes the previous…

High Energy Physics - Theory · Physics 2015-06-15 Chong-Sun Chu , Pichet Vanichchapongjaroen

We derive the stability conditions for the M5-brane in topological M-theory using kappa-symmetry. The non-linearly self-dual 3-form on the world-volume is necessarily non-vanishing, as is the case also for the 2-form field strengths on…

High Energy Physics - Theory · Physics 2008-11-26 Ling Bao , Martin Cederwall , Bengt E. W. Nilsson

The effective four-dimensional supergravity of M-theory compactified on the orbifold S^1/Z_2 and a Calabi-Yau threefold includes in general moduli supermultiplets describing massless modes of five-branes. For each brane, one of these fields…

High Energy Physics - Theory · Physics 2010-12-03 Luca Carlevaro , Jean-Pierre Derendinger

The analysis of the worldvolume effective actions of the M-theory Kaluza-Klein monopole and 9-brane suggests that it should be possible to describe non-abelian configurations of M2-branes or M5-branes if the M2-branes are transverse to the…

High Energy Physics - Theory · Physics 2009-10-31 Yolanda Lozano

We construct an effective action describing an elementary M5-brane interacting with dynamical eleven-dimensional supergravity, which is free from gravitational anomalies. The current associated to the elementary brane is taken as a…

High Energy Physics - Theory · Physics 2009-11-07 K. Lechner , P. A. Marchetti , M. Tonin

We calculate the first supersymmetric and kappa-symmetric derivative deformation of the M5-brane worldvolume theory in a flat eleven-dimensional background. By applying cohomological techniques we obtain a deformation of the standard…

High Energy Physics - Theory · Physics 2009-11-10 J. M. Drummond , S. F. Kerstan

We derive an energy bound for a `baryonic' D5-brane probe in the $adS_5\times S^5$ background near the horizon of $N$ D3-branes. Configurations saturating the bound are shown to be 1/4 supersymmetric $S^5$-wrapped D5-branes, with a total…

High Energy Physics - Theory · Physics 2010-02-03 Joaquim Gomis , Alfonso Ramallo , Joan Simon , Paul Townsend

We perform a general reduction of an M5-brane on a spacetime that admits a null Killing vector, including couplings to background 4-form fluxes and possible twisting of the normal bundle. We give the non-abelian extension of this action and…

High Energy Physics - Theory · Physics 2020-12-30 Neil Lambert , Tristan Orchard

It was known that the U$(N)^4$ super Chern-Simons matrix model describing the worldvolume theory of D3-branes with two NS5-branes and two $(1,k)$5-branes in IIB brane configuration (dual to M2-branes after taking the T-duality and the…

High Energy Physics - Theory · Physics 2020-01-29 Naotaka Kubo , Sanefumi Moriyama

We obtain a Lagrangian for a lightlike dimensional reduction of the nonabelian M5 brane theory in six dimension. We assume that the six-manifold has at least one conformal Killing spinor and two commuting lightlike Killing vector fields,…

High Energy Physics - Theory · Physics 2023-05-31 Andreas Gustavsson

We present calculation of the anomaly cancellation in M-theory on orbifolds $S^1/Z_2$ and $T^5/Z_2$ in the upstairs approach. The main requirement that allows one to uniquely define solutions to the modified Bianchi identities in this case…

High Energy Physics - Theory · Physics 2009-10-31 Krzysztof A. Meissner , Marek Olechowski

The strong-field limit for the 2-form potential on an M5-brane yields a conformal chiral 2-form electrodynamics in six dimensions, with gauge-invariant self-interactions but no adjustable coupling constant; the stress tensor is that of a…

High Energy Physics - Theory · Physics 2021-03-17 Paul K. Townsend

We observe that there is a rigorous derivation of (abelian) anyonic quantum states, hence of "topological order", on the 1+2-dimensional fixed locus of M5-probes wrapped over a trivially Seifert-fibered 3-orbifold singularity. Similar…

High Energy Physics - Theory · Physics 2025-04-01 Hisham Sati , Urs Schreiber

We have found the solution to the back reaction of putting a stack of coincident D3 and D5 branes in $R^{3,1}\times M_6$, where $M_6$ is constructed from an infinite class of Sasaki-Einstein spaces, $L^{(p,q,r)}$. The non-zero fluxes…

High Energy Physics - Theory · Physics 2010-04-05 D. Gepner , Shesansu Pal