Tseytlin, “D-branes and dual gauge theories in type 0 strings,” Nucl.
AdS/CFT Correspondence and Type 0 String Theory
Martelli, “On the construction of gauge theories from non critical type 0 strings,” Adv.
AdS/CFT Correspondence and Type 0 String Theory
In both type IIA and IIB cases the NSNS sector includes a metric gµν, an antisymmetric two-form gauge potential Bµν, and a scalar (dilaton) ﬁeld φ.
Large N field theories from superstrings
The RR sector of type IIA theory contains a one-form and a three-form gauge potentials {Aµ, Aµν ρ}.
Large N field theories from superstrings
The central stabilizer therefore provides a new mechanism to produce non-abelian gauge symmetries in type II compactiﬁcations.
Conformal field theory, boundary conditions and applications to string theory
All the MAG-type gauges similar Creutz ratios.
A Generalized Maximal Abelian Gauge in SU(3) Lattice Gauge Theory
The second and fourth term are typically for the Feynman type gauge; they could be omitted, leading to the Landau type gauge.
G_2 invariant 7D Euclidean super Yang-Mills theory as a higher-dimensional analogue of the 3D super-BF theory
As the worldvolume fermions transform in a complex representation of the SO(2) normal bundle gauge group, this symmetry is also potentially anomalous for the type IIB D3 brane.
An index for the Dirac operator on D3 branes with background fluxes
The type of gauge (3.5) was introduced in [20, 18] where the structure of the Killing spinor of the supergravity background BPS conﬁguration was used for ﬁxing κ-symmetry.
An index for the Dirac operator on D3 branes with background fluxes
This is admissible for those compactiﬁed solutions of type IIB supergravity for which the pullback of the NS-NS form B2 on the D3–brane worldvolume is pure gauge, i.e. B2 = −dA|D3 .
An index for the Dirac operator on D3 branes with background fluxes
The same correction has been already found in [25, 26] by using a light-cone type gauge.
New Integrable System of 2dim Fermions from Strings on AdS_5 x S^5
Fermions are not involved in our gauge choice and, therefore, can be treated at the ﬁnal stage when all the bosonic type constraints have been already solved.
New Integrable System of 2dim Fermions from Strings on AdS_5 x S^5
According to the original Maldacena conjecture the chiral operators of the strongly coupled N = 4 SU (N ) gauge theory are in one-to-one correspondence with the modes of type IIB supergravity on AdS5 × S 5 .
On the pp-wave limit and the BMN structure of new Sasaki-Einstein spaces
There is another mass generation mechanism for nonabelian gauge ﬁelds for which the corresponding Lagrangian is constructed with the help of an antisymmetric g–valued (2, 0)-type tensor potential B coupled to the gauge ﬁeld A via the topological term tr (B ∧ F ).
An equivalence of two mass generation mechanisms for gauge fields
Actually one can construct other nonabelian gauge invariant actions which differ from (5) or (63) by terms quadratic in the (2.0)–type tensor ﬁeld.
An equivalence of two mass generation mechanisms for gauge fields
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