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Related papers: Noncommutative Supersymmetric Gauge Anomaly

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We use the method of Banerjee, Banerjee and Mitra and minimal homotopy paths to compute the consistent gauge anomaly for several superspace models of SSYM coupled to matter. We review the derivation of the anomaly for N=1 in four dimensions…

High Energy Physics - Theory · Physics 2012-08-27 S. J. Gates, , M. T. Grisaru , M. E. Knutt , S. Penati , H. Suzuki

Using cohomological methods we discuss several issues related to chiral anomalies in noncommutative U(N) YM theories in any even dimension. We show that for each dimension there is only one solution of the WZ consistency condition and that…

High Energy Physics - Theory · Physics 2009-11-07 L. Bonora , A. Sorin

We discuss the noncommutative counterparts of chiral gauge theories and compute the associated anomalies.

High Energy Physics - Theory · Physics 2008-11-26 J. M. Gracia-Bondia , C. P. Martin

We show that the recently constructed higher-derivative 6D SYM theory involves an internal chiral anomaly breaking gauge invariance. The anomaly is cancelled when adding to the theory an adjoint matter hypermultiplet.

High Energy Physics - Theory · Physics 2008-11-26 A. V. Smilga

The explicit form of non-Abelian noncommutative supersymmetric (SUSY) chiral anomaly is calculated, the Wess-Zumino consistency condition is verified and the correspondence of the Yang-Mills sector to the previously obtained results is…

High Energy Physics - Theory · Physics 2007-05-23 L. O. Chekhov , A. K. Khizhnyakov

Using path integral method (Fujikawa's method) we calculate anomalies in noncommutative gauge theories with fermions in the bi-fundamental and adjoint representations. We find that axial and chiral gauge anomalies coming from non-planar…

High Energy Physics - Theory · Physics 2013-05-29 Tadahito Nakajima

Chiral gauge anomalies on noncommutative Minkowski Space-time are computed and have their origin elucidated. The consistent form and the covariant form of the anomaly are obtained. Both Fujikawa's method and Feynman diagram techniques are…

High Energy Physics - Theory · Physics 2009-11-07 C. P. Martin

An intriguing feature of the Standard Model is that the representations of the unbroken gauge symmetries are vector-like whereas those of the spontaneously broken gauge symmetries are chiral. Here we provide a toy model which shows that a…

High Energy Physics - Theory · Physics 2009-04-30 A. Salvio , M. Shaposhnikov

We study two well-known $SU(N)$ chiral gauge theories with fermions in the symmetric, anti-symmetric and fundamental representations. We give a detailed description of the global symmetry, including various discrete quotients. Recent work…

High Energy Physics - Theory · Physics 2022-01-11 Philip Boyle Smith , Avner Karasik , Nakarin Lohitsiri , David Tong

The axial anomaly of the noncommutative U(1) gauge theory is calculated by a number of methods and compared with the commutative one. It is found to be given by the corresponding Chern class.

High Energy Physics - Theory · Physics 2009-10-31 Farhad Ardalan , Neda Sadooghi

We analyze the theory and phenomenology of anomalous global chiral symmetries in the presence of an extra dimension. We propose a simple extension of the Standard Model in 5D whose signatures closely resemble those of supersymmetry with…

High Energy Physics - Phenomenology · Physics 2009-08-10 Csaba Csaki , Johannes Heinonen , Jay Hubisz , Yuri Shirman

Anomalies arising from nonplanar triangle diagrams of noncommutative gauge theory are studied. Local chiral gauge anomalies for both noncommutative U(1) and U(N) gauge theories with adjoint matter fields are shown to vanish. For…

High Energy Physics - Theory · Physics 2009-10-31 Farhad Ardalan , Neda Sadooghi

We calculate conformal anomalies in noncommutative gauge theories by using the path integral method (Fujikawa's method). Along with the axial anomalies and chiral gauge anomalies, conformal anomalies take the form of the straightforward…

High Energy Physics - Theory · Physics 2009-11-07 Tadahito Nakajima

We define $\mathcal N=2$ supersymmetric and gauge-invariant path integral measure in $D=4$, $\mathcal N=2$ SQCD in terms of $\mathcal N=1$ superfields. As a further consequence, we derive the $\mathcal N=2$ version of the chiral anomaly in…

High Energy Physics - Theory · Physics 2026-05-14 Akihisa D. -E. Tateishi

An elementary derivation of the chiral gauge anomaly in all even dimensions is given in terms of noncommutative traces of pseudo-differential operators.

High Energy Physics - Theory · Physics 2009-10-28 Edwin Langmann , Jouko Mickelsson

A search for supersymmetry anomalies requires an examination of the BRS cohomology of supersymmetric Yang-Mills coupled to chiral matter, and the physically interesting (on-shell) anomalies are those which cannot be eliminated using the…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. A. Dixon

The \gamma-trace anomaly of supersymmetry current in a supersymmetric gauge theory shares a superconformal anomaly multiplet with the chiral R-symmetry anomaly and the Weyl anomaly, and its holographic reproduction is a valuable test to the…

High Energy Physics - Theory · Physics 2015-06-26 M. Chaichian , W. F. Chen

We study 't Hooft anomalies of global symmetries in 1+1d lattice Hamiltonian systems. We consider anomalies in internal and lattice translation symmetries. We derive a microscopic formula for the "anomaly cocycle" using topological defects…

Strongly Correlated Electrons · Physics 2024-04-10 Sahand Seifnashri

A calculation of the chiral anomaly on a finite lattice without fermion doubling is presented . The lattice gauge field is defined in the spirit of noncommutative geometry. Standard formulas for the continuum anomaly are obtained as a…

High Energy Physics - Lattice · Physics 2007-05-23 Jouko Mickelsson

We present a direct field theoretical calculation of the consistent gauge anomaly in the superfield formalism, on the basis of a definition of the effective action through the covariant gauge current. The scheme is conceptually and…

High Energy Physics - Theory · Physics 2009-10-31 Yoshihisa Ohshima , Kiyoshi Okuyama , Hiroshi Suzuki , Hirofumi Yasuta
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