Measurement of differential cross sections for muon-neutrino electron scattering

Vilain, P.; Wilquet, G.; Beyer, R.; Flegel, W.; Grote, H.; Mouthuy, T.; Øverås, H.; Panman, J.; Rozanov, Alexandre; Winter, K.; Zacek, G.; Zacek, V.; Büsser, F.W.; Foos, C.; Gerland, L.; Layda, T.; Niebergall, F.; Rädel, G.; Stähelin, P.; Voß, T.; Favart, D.; Grégoire, G.; Knoops, E. B. F. G.; Lemaı̂tre, V.; Gorbunov, P.; Grigoriev, E.; Khovansky, V.; Maslennikov, A. L.; Lippich, W.; Nathaniel, A.; Staude, A.; Vogt, J.; Cocco, A. G.; Ereditato, A.; Fiorillo, G.; Marchetti-Stasi, F.; Palladino, V.; Strolin, P.; Capone, A.; Pedis, D. De; Capua, E. Di; Dore, U.; Frenkel-Rambaldi, A.; Loverre, P.; Macina, D.; Piredda, G.; Santacesaria, R.

doi:10.1016/0370-2693(93)90408-a

Cited by 67 publications

(91 citation statements)

References 11 publications

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“…However, from the experimental publications, the exact neutrino fluxes seem to be unknown and the SM prediction of the differential cross section given in [70] seems to be determined by a shape fit. Therefore, we are in doubt whether a rigorous calculation of the neutrino rate R at CHARM-II is possible and whether the χ 2 -fit used for limit determination in [8] is applicable.…”

Section: Charm-iimentioning

confidence: 99%

“…The CHARM-II collaboration has published both the measured total number of scattering events [69] as well as the differential cross section [70].…”

Section: Charm-iimentioning

confidence: 99%

“…In addition we consider the experimental measurements of solar neutrinos with Borexino [17,67,68], laboratory neutrino experiments such as, e.g. CHARM-II [69,70], COHER-ENT [71,72] and TEXONO [73] as well as tests of neutrino trident production [12,[74][75][76]. Furthermore, we include new astrophysical limits from the energy loss of white dwarfs [77].…”

Section: Jhep07(2018)094mentioning

confidence: 99%

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Hunting all the hidden photons

Bauer¹,

Foldenauer²,

Jaeckel³

2018

J. High Energ. Phys.

373

450

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We explore constraints on gauge bosons of a weakly coupled U(1) B−L , U(1) Lµ−Le , U(1) Le−Lτ and U(1) Lµ−Lτ . To do so we apply the full constraining power of experimental bounds derived for a hidden photon of a secluded U(1) X and translate them to the considered gauge groups. In contrast to the secluded hidden photon that acquires universal couplings to charged Standard Model particles through kinetic mixing with the photon, for these gauge groups the couplings to the different Standard Model particles can vary widely. We take finite, computable loop-induced kinetic mixing effects into account, which provide additional sensitivity in a range of experiments. In addition, we collect and extend limits from neutrino experiments as well as astrophysical and cosmological observations and include new constraints from white dwarf cooling. We discuss the reach of future experiments in searching for these gauge bosons.

show abstract

Section: Charm-iimentioning

confidence: 99%

“…The CHARM-II collaboration has published both the measured total number of scattering events [69] as well as the differential cross section [70].…”

Section: Charm-iimentioning

confidence: 99%

Section: Jhep07(2018)094mentioning

confidence: 99%

See 1 more Smart Citation

Hunting all the hidden photons

Bauer¹,

Foldenauer²,

Jaeckel³

2018

J. High Energ. Phys.

373

450

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show abstract

“…There are various neutrino-electron scattering experiments which are mainly TEXONO [13][14][15], BOREXINO [16], GEMMA [17] as well as LSND [18] and CHARM II [19]. A light dark photon could be searched using these data.…”

Section: Introductionmentioning

confidence: 99%

Constraints on dark photon from neutrino-electron scattering experiments

et al. 2015

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“…While the B − L breaking scale χ = m Z /(2g B−L ) is constrained to be larger than 3.45 TeV from LEP-II [3][4][5][6], these limits are not applicable when m Z becomes too small. Neutrino scattering experiments set an effective limit on χ 1 TeV [7][8][9][10][11]. The wider m Z − g B−L parameter space can for example be explored using the Constraints On New Theories Using Rivet (CONTUR) method for m Z 1 GeV incorporating ATLAS and CMS results [12,13].…”

Section: Introductionmentioning

confidence: 99%

Searching for a light Z′ through Higgs production at the LHC

2019

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We investigate the potential of LHC resonance searches in leptonic final states to probe the Z in the minimal U (1) B−L model. Considering the current constraints on the Z in terms of its mass m Z and the associated gauge coupling g B−L as well as constraints in the Higgs sector, we analyse the potential of dilepton and four lepton final states for Z production. This includes Drell-Yan production, Higgs mediated decays and final state radiation processes concentrating only on the ATLAS and CMS detectors at the LHC. We show that the four-lepton final state is sensitive to m Z as low as 0.25 GeV. Furthermore, setting the Higgs mixing to sin α = 0.3, this final state has a strong sensitivity and it probes regions of parameter space where the Z is long-lived. We demonstrate the sensitivity at the High Luminosity LHC and comment on the potential of probing displaced vertices due to long-lived Z . Finally, we also comment on the strength of Z and Higgs mediated heavy neutrino processes by taking into account the constraints derived.

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Measurement of differential cross sections for muon-neutrino electron scattering

Cited by 67 publications

References 11 publications

Hunting all the hidden photons

Hunting all the hidden photons

Constraints on dark photon from neutrino-electron scattering experiments

Searching for a light Z′ through Higgs production at the LHC

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