Measurement of Coherent 
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 Production in Low Energy Neutrino-Carbon Scattering

Abe, K.; Andreopoulos, C.; Antonova, M.; Aoki, Shigeki; Ariga, A.; Assylbekov, S.; Autiero, D.; Ban, S.; Barbi, M.; Barker, G. J.; Barr, G.; Bartet-Friburg, P.; Batkiewicz, M.; Bay, F.; Berardi, V.; Berkman, S.; Bhadra, S.; Blondel, A.; Bolognesi, S.; Bordoni, S.; Boyd, S. B.; Brailsford, D.; Bravar, A.; Bronner, C.; Avanzini, M. Buizza; Calland, R. G.; Campbell, T.; Cao, S.; Rodríguez, J. Caravaca; Cartwright, S.; Castillo, R.; Catanesi, M. G.; Cervera, A.; Cherdack, D.; Chikuma, N.; Christodoulou, G.; Clifton, A.; Coleman, J. P.; Collazuol, G.; Coplowe, D.; Cremonesi, L.; Dąbrowska, A.; Rosa, G. De; Dealtry, T.; Denner, P. F.; Dennis, S. R.; Densham, C.; Dewhurst, D.; Lodovico, F. Di; Luise, S. Di; Dolan, S.; Drapier, O.; Duffy, K.; Dumarchez, J.; Dytman, S. A.; Dziewiecki, M.; Emery-Schrenk, S.; Ereditato, A.; Feusels, T.; Finch, A. J.; Fiorentini, G. A.; Friend, M.; Fujii, Y.; Fukuda, Daisuke; Fukuda, Y.; Furmanski, A. P.; Galymov, V.; Díaz, Antonio; Giffin, S.; Giganti, C.; Gizzarelli, F.; Gonin, M.; Grant, N.; Hadley, D. R.; Haegel, L.; Haigh, M. D.; Hamilton, P.; Hansen, D.; Harada, J.; Hara, T.; Hartz, M.; Hasegawa, T.; Hastings, N. C.; Hayashino, T.; Hayato, Y.; Helmer, R. L.; Hierholzer, M.; Hillairet, A.; Himmel, A.; Hiraki, T.; Hirota, S.; Hogan, M.; Holeczek, J.; Horikawa, S.; Hosomi, F.; Huang, K.; Ichikawa, A. K.; Ieki, K.; Ikeda, M.; Imber, J.; Insler, J.; Intonti, R. A.; Irvine, T. J.; Ishida, Toru; Ishii, T.; Iwai, E.; Iwamoto, K.; Izmaylov, A.; Jacob, Anu; Jamieson, B.; Jiang, M.; Johnson, S.; Jo, J. H.; Jönsson, P.; Jung, C. K.; Kabirnezhad, M.; Kaboth, A.; Kajita, T.; Kakuno, H.; Kameda, J.; Karlen, D.; Karpikov, I.; Katori, T.; Kearns, E.; Khabibullin, M.; Khotjantsev, A.; Kiełczewska, D.; Kikawa, T.; Kim, H.; Kim, J.; King, S.; Kisiel, J.; Knight, A.; Knox, A.; Kobayashi, T.; Koch, L.; Koga, T.; Konaka, A.; Kondo, K.; Kopylov, A.; Kormos, L. L.; Korzenev, A.; Koshio, Y.; Kropp, W. R.; Kudenko, Y.; Kurjata, R.; Kutter, T.; Łagoda, J.; Lamont, I.; Larkin, E.; Lasorak, P.; Laveder, M.; Lawe, M.; Lazos, M.; Lindner, T.; Liptak, Z.; Litchfield, R. P.; Li, X.; Longhin, A.; Lopez, J. P.; Ludovici, L.; Lu, X.-G.; Magaletti, L.; Mahn, Kendall; Malek, M.; Manly, S.; Marino, A. D.; Marteau, J.; Martin, J. F.; Martins, P.; Martynenko, S.; Maruyama, T.; Matveev, V.; Mavrokoridis, K.; Y., W.; Mazzucato, E.; McCarthy, M.; McCauley, N.; McFarland, K. S.; McGrew, C.; Mefodiev, A.; Metelko, C.; Mezzetto, M.; Mijakowski, P.; Minamino, A.; Mineev, O.; Mine, S.; Missert, A.; Miura, Makoto; Moriyama, S.; Mueller, Th A.; Murphy, S.; Myslik, J.; Nakadaira, T.; Nakahata, M.; Nakamura, K.; Nakamura, K.; Nakamura, K.; Nakayama, S.; Nakaya, T.; Nakayoshi, K.; Nantais, C.; Nielsen, C.; Nirkko, M.; Nishikawa, K.; Nishimura, Y.; Novella, P.; Nowak, J.; O’Keeffe, H. M.; Ohta, R.; Okumura, K.; Okusawa, T.; Oryszczak, W.; Oser, S. M.; Ovsyannikova, T.; Owen, R. A.; Oyama, Y.; Palladino, V.; Palomino, J. L.; Paolone, V.; Patel, N. D.; Pavin, M.; Payne, D. J.; Perkin, J. D.; Petrov, Y.; Pickard, L.; Pickering, L.; Guerra, E. S. Pinzon; Pistillo, C.; Popov, Б.; Posiadała-Zezula, M.; Poutissou, J. M.; Poutissou, R.; Przewłocki, P.; Quilain, B.; Radermacher, T.; Radicioni, E.; Ratoff, P. N.; Ravonel, M.; Rayner, M.; Redij, A.; Reinherz‐Aronis, E.; Riccio, C.; Rojas, Pablo Fierro; Rondio, E.; Roth, Stefan; Rubbia, A.; Rychter, A.; Sacco, R.; Sakashita, K.; Sánchez, F.; Sato, F.; Scantamburlo, E.; Scholberg, K.; Schoppmann, S.; Schwehr, J.; Scott, M.; Seiya, Y.; Sekiguchi, T.; Sekiya, H.; Sgalaberna, D.; Shah, R.; Shaikhiev, A.; Shaker, F.; Shaw, D.; Shiozawa, M.; Shirahige, T.; Short, S.; Smy, M.; Sobczyk, J. T.; Sobel, H. W.; Sorel, M.; Southwell, L.; Stamoulis, P.; Steinmann, J.; Stewart, T.; Stowell, P.; Suda, Y.; Suvorov, S.; Suzuki, A.; Suzuki, K.; Suzuki, S.; Suzuki, Y.; Tacik, R.; Tada, M.; Takahashi, Sentaro; Takeda, Atsushi; Takeuchi, Y.; Tanaka, Hiroyuki; Tanaka, H. A.; Terhorst, D.; Terri, R.; Thakore, T.; Thompson, L. F.; Tobayama, S.; Toki, W. H.; Tomura, T.; Touramanis, C.; Tsukamoto, T.; Tzanov, M.; Uchida, Y.; Vacheret, A.; Vagins, M. R.; Vallari, Z.; Vasseur, G.; Wąchała, T.; Wakamatsu, K.; Walter, C. W.; Wark, D.; Warzycha, W.; Wascko, M. O.; Weber, A.; Wendell, R.; Wilkes, R. J.; Wilking, M. J.; Wilkinson, C.; Wilson, J. R.; Wilson, R. J.; Yamada, Y.; Yamamoto, K.; Yamamoto, M.; Yanagisawa, C.; Yano, T.; Yen, S.; Yershov, N.; Yokoyama, M.; Yoo, J.; Yoshida, Kyohei; Yuan, Tianlu; Yu, M.; Zalewska, A.; Zalipska, J.; Zambelli, L.; Заремба, К.; Ziembicki, M.; Zimmerman, E. D.; Zito, M.; Żmuda, J.

doi:10.1103/physrevlett.117.192501

Cited by 33 publications

(29 citation statements)

References 46 publications

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“…[25]. Production of pions in coherent inelastic scattering is described by a tuned model of Rein-Sehgal [26], which agrees with recent measurements [27,28]. As in Ref.…”

supporting

confidence: 88%

Search for CP Violation in Neutrino and Antineutrino Oscillations by the T2K Experiment with 2.2×1021 Protons on Target

Abe¹,

Akutsu²,

Ali³

et al. 2018

Phys. Rev. Lett.

Self Cite

221

227

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“…[25]. Production of pions in coherent inelastic scattering is described by a tuned model of Rein-Sehgal [26], which agrees with recent measurements [27,28]. As in Ref.…”

supporting

confidence: 88%

Search for CP Violation in Neutrino and Antineutrino Oscillations by the T2K Experiment with 2.2×1021 Protons on Target

Abe¹,

Akutsu²,

Ali³

et al. 2018

Phys. Rev. Lett.

Self Cite

221

227

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“…49. This includes recent measurements from ArgoNEUT [33] and T2K [71] which are significantly less precise than the MINERvA measurements and do not report differential cross sections. The T2K measurement, however, plays a special role here in that it shows consistency of the cross section at lower energies than accessible by MINERvA with the dσ=dE π at low pion energies below the prediction of the GENIE Rein-Sehgal model.…”

Section: Discussionmentioning

confidence: 99%

Measurement of total and differential cross sections of neutrino and antineutrino coherent π± production on carbon

Mislivec¹,

Higuera²,

Aliaga³

et al. 2018

Phys. Rev. D

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Neutrino induced coherent charged pion production on nuclei,ν μ A → μ AE π ∓ A, is a rare inelastic interaction in which the four-momentum squared transferred to the nucleus is nearly zero, leaving it intact. We identify such events in the scintillator of MINERvA by reconstructing jtj from the final state pion and muon momenta and by removing events with evidence of energetic nuclear recoil or production of other final state particles. We measure the total neutrino and antineutrino cross sections as a function of neutrino energy between 2 and 20 GeV and measure flux integrated differential cross sections as a function of Q 2 , * Deceased.

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“…The charged current version serves mainly as a background to µ + µ − tridents, but can also appear as a background for e ± µ ∓ tridents for incoming electron neutrinos or antineutrinos. It has been studied before at MiniBooNE [60], MINERνA [61,62], T2K [28,63], and for the first time in LAr at ArgoNeuT [64]. This process has a very distict low 4-momentum transfer to the nucleus |t| [61], but a much flatter distribution in invariant mass if compared to trident.…”

Section: C1 Pion Productionmentioning

confidence: 99%

Neutrino trident scattering at near detectors

Ballett

Hostert

Pascoli

et al. 2019

J. High Energ. Phys.

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Neutrino trident scattering is a rare Standard Model process where a chargedlepton pair is produced in neutrino-nucleus scattering. To date, only the dimuon final-state has been observed, with around 100 total events, while the other channels are as yet unexplored. In this work, we compute the trident production cross section by performing a complete four-body phase space calculation for different hadronic targets. This provides a correct estimate both of the coherent and the diffractive contributions to these cross sections, but also allows us to address certain inconsistencies in the literature related to the use of the Equivalent Photon Approximation in this context. We show that this approximation can give a reasonable estimate only for the production of dimuon final-states in coherent scattering, being inadmissible for all other cases considered. We provide estimates of the number and distribution of trident events at several current and future near detector facilities subjected to intense neutrino beams from accelerators: five liquid-argon detectors (SBND, µBooNE, ICARUS, DUNE and νSTORM), the iron detector of T2K (INGRID) and three detectors made of composite material (MINOS, NOνA and MINERνA). We find that for many experiments, trident measurements are an attainable goal and a valuable addition to their near detector physics programme.

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Measurement of Coherent π+ Production in Low Energy Neutrino-Carbon Scattering

Cited by 33 publications

References 46 publications

Search for CP Violation in Neutrino and Antineutrino Oscillations by the T2K Experiment with 2.2×1021 Protons on Target

Search for CP Violation in Neutrino and Antineutrino Oscillations by the T2K Experiment with 2.2×1021 Protons on Target

Measurement of total and differential cross sections of neutrino and antineutrino coherent π± production on carbon

Neutrino trident scattering at near detectors

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