Results 51 to 60 of about 5,628 (239)
Abstract The b ghost, or b operator, used for fixing Siegel gauge in the pure spinor superfield formalism, is a composite operator of negative ghost number, satisfying {q,b}=□$\lbrace q,b\rbrace =\square$, where q is the pure spinor differential (BRST operator). It is traditionally constructed using non‐minimal variables.
Martin Cederwall
wiley +1 more source
On the BPS Sector in AdS3/CFT2 Holography
Abstract The BPS sector in AdS3/CFT2$AdS_3/CFT_2$ duality has been fertile ground for the exploration of gauge/gravity duality, from the match between black hole entropy and the CFT elliptic genus to the construction of large families of geometrical microstates and the identification of the corresponding states in the CFT.
Emil J. Martinec+2 more
wiley +1 more source
Towards generalized mirror symmetry for twisted connected sum G 2 manifolds
We revisit our construction of mirror symmetries for compactifications of Type II superstrings on twisted connected sum G 2 manifolds. For a given G 2 manifold, we discuss evidence for the existence of mirror symmetries of two kinds: one is an ...
Andreas P. Braun, Michele Del Zotto
doaj +1 more source
Duality without supersymmetry [PDF]
I show that physical quantities in several two-dimensional condensed-matter models are related to the Seiberg-Witten calculation of exact quantities in supersymmetric gauge theory. In particular, the magnetization in the Kondo problem and the current in the boundary sine-Gordon model can each be expressed in the form $\int dx/y$, where for example in ...
openaire +3 more sources
Conformal Interactions Between Matter and Higher‐Spin (Super)Fields
Abstract In even spacetime dimensions, the interacting bosonic conformal higher‐spin (CHS) theory can be realised as an induced action. The main ingredient in this definition is the model S[φ,h]$\mathcal {S}[\varphi ,h]$ describing a complex scalar field φ coupled to an infinite set of background CHS fields h, with S[φ,h]$\mathcal {S}[\varphi ,h ...
Sergei M. Kuzenko+2 more
wiley +1 more source
A new duality between N $$ \mathcal{N} $$ = 8 superconformal field theories in three dimensions
We propose a new duality between two 3d N $$ \mathcal{N} $$ = 8 superconformal Chern-Simons-matter theories: the U(3)1 × U(3)−1 ABJM theory and a theory consisting of the product between the (SU(2)3 × SU(2)− 3)/ℤ2 BLG theory and a free N $$ \mathcal{N} $$
Nathan B. Agmon+2 more
doaj +1 more source
T-duality and world-sheet supersymmetry [PDF]
15 pages ...
Bakas, I, Sfetsos, K
openaire +5 more sources
Dualities of adjoint SQCD and supersymmetry enhancement
Abstract We propose a new dual description of four-dimensional $$ \mathcal{N} $$ N = 1 SU(N) gauge theory with one adjoint (X) and Nf fundamental matters with a superpotential W = TrXp+1. The dual theory consists of the $$ \mathcal{D} $$ D p[SU(N)] Argyres-Douglas
Kazunobu Maruyoshi+2 more
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Instantons on Young diagrams with matters
We present the unrefined instanton partition functions of various 5d gauge theories with matter beyond the fundamental representation as sums over Young diagrams.
Yanyan Chen+3 more
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The action with manifest E7 type symmetry
We generalize Cremmer-Julia 1st order action of N = 8 $$ \mathcal{N}=8 $$ supergravity with manifest E 7(7) symmetry to cases of N = 6 $$ \mathcal{N}=6 $$ with manifest SO∗(12) and N = 5 $$ \mathcal{N}=5 $$ with manifest SU(1, 5) duality symmetries ...
Renata Kallosh
doaj +1 more source