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Related papers: Anomaly and Nonplanar Diagrams in Noncommutative G…

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We discuss both the UV and IR origin of the one-loop triangle gauge anomalies for noncommutative nonabelian chiral gauge theories with fundamental, adjoint and bi-fundamental fermions for U(N) groups. We find that gauge anomalies only come…

High Energy Physics - Theory · Physics 2008-11-26 C. P. Martin

As pointed out, chiral non-commutative theories exist, and examples can be constructed via string theory. Gauge anomalies require the matter content of individual gauge group factors, including U(1) factors, to be non-chiral. All ``bad''…

High Energy Physics - Theory · Physics 2009-11-07 Ken Intriligator , Jason Kumar

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

The Konishi anomalies for noncommutative N=1 supersymmetric U(1) gauge theory arising from planar and nonplanar diagrams are calculated. Whereas planar Konishi anomaly is the expected \star-deformation of the commutative anomaly, nonplanar…

High Energy Physics - Theory · Physics 2009-11-10 Farhad Ardalan , Neda Sadooghi

We discuss nonplanar anomalies in noncommutative gauge theories. In particular we show that a nonplanar anomaly exists when the external noncommutative momentum is zero and that it leads to a non-conservation of the associated axial charge.…

High Energy Physics - Theory · Physics 2011-07-19 Adi Armoni , Esperanza Lopez , Stefan Theisen

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

Although axial QED suffers from a gauge anomaly, gauge invariance may be maintained by the addition of a nonlocal counterterm. Such nonlocal conterterms, however, are expected to ruin unitarity of the theory. We explicitly investigate some…

High Energy Physics - Theory · Physics 2009-10-30 C. Adam

We derive maps relating currents and their divergences in non-abelian U(N) noncommutative gauge theory with the corresponding expressions in the ordinary (commutative) description. For the U(1) theory, in the slowly-varying-field…

High Energy Physics - Theory · Physics 2007-05-23 Rabin Banerjee , Kuldeep Kumar

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

The covariant form of the non-Abelian gauge anomaly on noncommutative R2n is computed for U(N) groups. Its origin and properties are analyzed. Its connection with the consistent form of the gauge anomaly is established. We show along the…

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

Invariant (nonplanar) anomaly of noncommutative QED is reexamined. It is found that just as in ordinary gauge theory UV regularization is needed to discover anomalies, in noncommutative case, in addition, an IR regularization is also…

High Energy Physics - Theory · Physics 2009-11-11 F. Ardalan , H. Arfaei , N. Sadooghi

Generalized Konishi anomaly relations in the chiral ring of N=1 supersymmetric gauge theories with unitary gauge group and chiral matter field in two-index tensor representations are derived. Contrary to previous investigations of related…

High Energy Physics - Theory · Physics 2009-11-10 Karl Landsteiner

The structure of the moduli space of N=1 supersymmetric gauge theories is analyzed from an algebraic geometric viewpoint. The connection between the fundamental fields of the ultraviolet theory, and the gauge invariant composite fields of…

High Energy Physics - Theory · Physics 2009-10-30 Gustavo Dotti , Aneesh Manohar

Abelian quiver gauge theories provide nonsupersymmetric candidates for the conformality approach to physics beyond the standard model. Written as ${\cal N}=0$, $U(N)^n$ gauge theories, however, they have mixed $U(1)_p U(1)_q^2$ and $U(1)_p…

High Energy Physics - Theory · Physics 2008-11-26 Edoardo Di Napoli , Paul H. Frampton

It is argued on general ground and demonstrated in the particular example of the Chiral Schwinger Model that there is nothing wrong with apparently anomalous chiral gauge theory. If quantised correctly, there should be no gauge anomaly and…

High Energy Physics - Theory · Physics 2011-04-15 Tien D Kieu

Here we examine the noncommutative counterpart of QED, which is called as noncommutative QED. The theory is obtained by examining the consistent minimal coupling to noncommutative U(1) gauge field. The *-product admits the coupling of the…

High Energy Physics - Theory · Physics 2009-10-31 M. Hayakawa

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 study duality in $\mathcal{N}=1$ supersymmetric QCD in the non-Abelian Coulomb phase, order-by-order in scheme-independent series expansions. Using exact results, we show how the dimensions of various fundamental and composite chiral…

High Energy Physics - Theory · Physics 2018-04-04 Thomas A. Ryttov , Robert Shrock

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
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