2009
DOI: 10.1103/physrevd.79.013007
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Large gauge invariant nonstandard neutrino interactions

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Cited by 137 publications
(179 citation statements)
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“…Model dependent [21,[54][55][56][57][58][59][60][61][62][63][64][65][66] and independent [53,67,68] bounds are obtained for these matter NSI parameters and are shown in the following table. In obtaining model dependent bounds on matter NSI the experiments with neutrinos and charged leptons -LSND, CHARM, CHARM-II, NuTeV and also LEP-II have been considered.…”
Section: Nsi and Its Effect On Neutrino Oscillation Probabilitiesmentioning
confidence: 99%
“…Model dependent [21,[54][55][56][57][58][59][60][61][62][63][64][65][66] and independent [53,67,68] bounds are obtained for these matter NSI parameters and are shown in the following table. In obtaining model dependent bounds on matter NSI the experiments with neutrinos and charged leptons -LSND, CHARM, CHARM-II, NuTeV and also LEP-II have been considered.…”
Section: Nsi and Its Effect On Neutrino Oscillation Probabilitiesmentioning
confidence: 99%
“…When H acquires a non-zero vacuum expectation value v, this operator leads to SU (2)-violating four-fermion contact interactions, so that NSI in the neutrino sector can be generated without inducing phenomenologically-problematic four-charged-lepton couplings or other harmful effects. On the other hand, this procedure leads to an additional suppression of order v2/M 2 and requires some cancellation conditions at tree level [164]. Larger non-standard effects could be generated in theories involving light mediators (≪ M W ) with very small couplings.…”
Section: Effective Theory Of New Physics In the Neutrino Sectormentioning
confidence: 99%
“…Model-independent experimental constraints on the ε s,d,m αβ range from 10 −4 to O(1) [16,[159][160][161][162], while model-dependent limits are often much tighter [163,164] since, in concrete models, NSI in the neutrino sector are usually accompanied by non-standard effects in the charged-lepton sector that are constrained, for example, by rare decay searches or measurements of the weak mixing angle.…”
Section: Effective Theory Of New Physics In the Neutrino Sectormentioning
confidence: 99%
“…However, it has been shown [17,18,26,27] that for the NU and 4L operators, it is possible to cancel all contributions to processes with four charged fermions while lepton flavour violation is still present in the neutrino sector. For the 2L2Q operators, it is trivial to expand the operators in components and see that this cancellation is not possible for the four-chargedfermion (4CF) operators with quarks, since both up and down quarks carry electromagnetic charge and both contributions would need to cancel simultaneously.…”
Section: New Physics At Near Detectorsmentioning
confidence: 99%
“…III along with the weaker model-independent ones. The operator can in principle also be realized by a combination of the other types of mediator fields, e.g., Z ′ (1 v 0 ) and W ′ (3 v 0 ), in which the couplings between leptons and the mediation fields must follow a specific relation to cancel 4CF [27]. …”
Section: New Physics With Leptons: 4l Operators a Bounds On 4lmentioning
confidence: 99%