Abstract:In this paper we construct a version of the standard model gauge sector on noncommutative space-time which is one-loop renormalizable to first order in the expansion in the noncommutativity parameter θ. The one-loop renormalizability is obtained by the Seiberg-Witten redefinition of the noncommutative gauge potential for the model containing the usual six representations of matter fields of the first generation.
“…In this work we consider the standard-model (SM) forbidden Z → γγ decay originating from the renormalizable gauge sector of the noncommutative standard model (NCSM) given in [1], which could be probed in highenergy collider experiments.…”
mentioning
confidence: 99%
“…Even more, its noncommutative part is finite or free of divergences, so the noncommutativity parameter θ need not be renormalized. A detailed description of the renormalization procedure, including the results for the bare fields and couplings, is given in [1]. Finally, from the action (6) we extract the triplegauge boson terms which are not present in the commutative SM Lagrangian.…”
In this work we propose the Z → γγ decay as a process strictly forbidden in the standard model, suitable for the search of noncommutativity of coordinates at very short distances. We computed the Z → γγ partial width in the framework of the recently proposed one-loop renormalizable gauge sector of the noncommutative standard model. New experimental possibilities at LHC are analyzed and a firm bound to the scale of noncommutativity parameter is set around 1 TeV.
“…In this work we consider the standard-model (SM) forbidden Z → γγ decay originating from the renormalizable gauge sector of the noncommutative standard model (NCSM) given in [1], which could be probed in highenergy collider experiments.…”
mentioning
confidence: 99%
“…Even more, its noncommutative part is finite or free of divergences, so the noncommutativity parameter θ need not be renormalized. A detailed description of the renormalization procedure, including the results for the bare fields and couplings, is given in [1]. Finally, from the action (6) we extract the triplegauge boson terms which are not present in the commutative SM Lagrangian.…”
In this work we propose the Z → γγ decay as a process strictly forbidden in the standard model, suitable for the search of noncommutativity of coordinates at very short distances. We computed the Z → γγ partial width in the framework of the recently proposed one-loop renormalizable gauge sector of the noncommutative standard model. New experimental possibilities at LHC are analyzed and a firm bound to the scale of noncommutativity parameter is set around 1 TeV.
“…Now taking into account the results of the θ 1 models [44,45], where in the NC SU(N) model [45] was explicitly shown that θ 1 parameter runs while having a negative β function, we conjecture that β functions associated with the parameters κ, η 1 , and (2η 4 − η 5 ) could be negative too. The (η 2 − η 3 ) difference should have a zero β function.…”
A novel nonlocal four-photon interaction on the deformed spacetime is derived and studied in the three selected models (I, II, III). The first two models (I, II) are obtained via two distinct second-order θ-exact Seiberg-Witten maps of the noncommutative U(1) gauge field strength on Moyal space. The third one (III), inspired by the manifestly gauge invariant structures emerging in the first two, due to the model generality has been constructed with a different set of freedom parameters. The physical relevancy of all models is analyzed by evaluating the four-photon-tadpole diagram, which, when combined with the bubble graph, enables us to fully consider all contributions to the one-loop photon polarization tensor. For an arbitrary noncommutative matrix θ µν , the full quadratic IR divergence cancellation in the one-loop photon two-point function is obtained with particular combinations of Seiberg-Witten map/gauge-symmetry freedom parameters in models I and II. Finally, our model III enables complete elimination of all pathological terms in the photon polarization tensor at one-loop order if a special value for the θ matrix is chosen.
“…A very incomplete list of articles addressing problems in this research area includes refs. [78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99].…”
Numerical simulation is an important non-perturbative tool to study quantum field theories defined in non-commutative spaces. In this contribution, a selection of results from Monte Carlo calculations for non-commutative models is presented, and their implications are reviewed. In addition, we also discuss how related numerical techniques have been recently applied in computer simulations of dimensionally reduced supersymmetric theories.
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