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Related papers: Comparing pion production models to MiniBooNE data

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Neutrino-induced pion and photon production from nucleons and nuclei are important for the interpretation of neutrino-oscillation experiments, and these processes are potential backgrounds in the MiniBooNE experiment [A. A. Aquilar-Arevalo…

Nuclear Theory · Physics 2010-11-30 Brian D. Serot , Xilin Zhang

The T2K Collaboration presents the first measurement of electron neutrino-induced charged-current pion production on carbon in a restricted kinematical phase space. This is performed using data from the 2.5$^{\deg}$ off-axis near detector,…

High Energy Physics - Experiment · Physics 2025-10-10 K. Abe , S. Abe , R. Akutsu , H. Alarakia-Charles , Y. I. Alj Hakim , S. Alonso Monsalve , L. Anthony , S. Aoki , K. A. Apte , T. Arai , T. Arihara , S. Arimoto , E. T. Atkin , N. Babu , V. Baranov , G. J. Barker , G. Barr , D. Barrow , P. Bates , L. Bathe-Peters , M. Batkiewicz-Kwasniak , N. Baudis , V. Berardi , L. Berns , S. Bhattacharjee , A. Blanchet , A. Blondel , P. M. M. Boistier , S. Bolognesi , S. Bordoni , S. B. Boyd , C. Bronner , A. Bubak , M. Buizza Avanzini , J. A. Caballero , F. Cadoux , N. F. Calabria , S. Cao , S. Cap , D. Carabadjac , S. L. Cartwright , M. P. Casado , M. G. Catanesi , J. Chakrani , A. Chalumeau , D. Cherdack , A. Chvirova , J. Coleman , G. Collazuol , F. Cormier , A. A. L. Craplet , A. Cudd , D. D'ago , C. Dalmazzone , T. Daret , P. Dasgupta , C. Davis , Yu. I. Davydov , P. de Perio , G. De Rosa , T. Dealtry , C. Densham , A. Dergacheva , R. Dharmapal Banerjee , F. Di Lodovico , G. Diaz Lopez , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , K. E. Duffy , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , J. Elias , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , L. Feng , D. Ferlewicz , A. J. Finch , M. D. Fitton , C. Forza , M. Friend , Y. Fujii , Y. Fukuda , Y. Furui , J. García-Marcos , A. C. Germer , L. Giannessi , C. Giganti , M. Girgus , V. Glagolev , M. Gonin , R. González Jiménez , J. González Rosa , E. A. G. Goodman , K. Gorshanov , P. Govindaraj , M. Grassi , M. Guigue , F. Y. Guo , D. R. Hadley , S. Han , D. A. Harris , R. J. Harris , T. Hasegawa , C. M. Hasnip , S. Hassani , N. C. Hastings , Y. Hayato , I. Heitkamp , D. Henaff , Y. Hino , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , M. C. F. Hooft , K. Hosokawa , J. Hu , A. K. Ichikawa , K. Ieki , M. Ikeda , T. Ishida , M. Ishitsuka , H. Ito , S. Ito , A. Izmaylov , N. Jachowicz , S. J. Jenkins , C. Jesús-Valls , M. Jia , J. J. Jiang , J. Y. Ji , T. P. Jones , P. Jonsson , S. Joshi , M. Kabirnezhad , A. C. Kaboth , H. Kakuno , J. Kameda , S. Karpova , V. S. Kasturi , Y. Kataoka , T. Katori , A. Kawabata , Y. Kawamura , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , S. King , V. Kiseeva , J. Kisiel , A. Klustová , L. Kneale , H. Kobayashi , L. Koch , S. Kodama , M. Kolupanova , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , Y. Kudenko , Y. Kudo , A. Kumar Jha , R. Kurjata , V. Kurochka , T. Kutter , L. Labarga , M. Lachat , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , A. Langella , D. H. Langridge , J. -F. Laporte , D. Last , N. Latham , M. Laveder , L. Lavitola , M. Lawe , D. Leon Silverio , S. Levorato , S. V. Lewis , B. Li , C. Lin , R. P. Litchfield , S. L. Liu , W. Li , A. Longhin , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , K. K. Mahtani , S. Manly , A. D. Marino , D. G. R. Martin , D. A. Martinez Caicedo , L. Martinez , M. Martini , T. Matsubara , R. Matsumoto , V. Matveev , C. Mauger , K. Mavrokoridis , N. McCauley , K. S. McFarland , C. McGrew , J. McKean , A. Mefodiev , G. D. Megias , L. Mellet , C. Metelko , M. Mezzetto , S. Miki , V. Mikola , E. W. Miller , A. Minamino , O. Mineev , S. Mine , J. Mirabito , M. Miura , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , A. Muñoz , L. Munteanu , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , K. D. Nakamura , A. Nakano , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , D. T. Nguyen , V. Q. Nguyen , K. Niewczas , S. Nishimori , Y. Nishimura , Y. Noguchi , T. Nosek , F. Nova , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , R. Okazaki , W. Okinaga , K. Okumura , T. Okusawa , N. Onda , N. Ospina , L. Osu , Y. Oyama , V. Paolone , J. Pasternak , D. Payne , M. Pfaff , L. Pickering , B. Popov , A. J. Portocarrero Yrey , M. Posiadala-Zezula , Y. S. Prabhu , H. Prasad , F. Pupilli , B. Quilain , P. T. Quyen , E. Radicioni , B. Radics , M. A. Ramirez , R. Ramsden , P. N. Ratoff , M. Reh , G. Reina , C. Riccio , D. W. Riley , E. Rondio , S. Roth , N. Roy , A. Rubbia , L. Russo , A. Rychter , W. Saenz , K. Sakashita , S. Samani , F. Sánchez , E. M. Sandford , Y. Sato , T. Schefke , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , T. Sekiya , D. Seppala , D. Sgalaberna , A. Shaikhiev , M. Shiozawa , Y. Shiraishi , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , A. J. Speers , R. Spina , A. Srivastava , P. Stowell , Y. Stroke , I. A. Suslov , A. Suzuki , S. Y. Suzuki , M. Tada , S. Tairafune , A. Takeda , Y. Takeuchi , K. Takeya , H. K. Tanaka , H. Tanigawa , V. V. Tereshchenko , N. Thamm , C. Touramanis , N. Tran , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , S. Valder , M. Varghese , I. Vasilyev , G. Vasseur , E. Villa , U. Virginet , T. Vladisavljevic , T. Wachala , D. Wakabayashi , H. T. Wallace , J. G. Walsh , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , K. Yamamoto , T. Yamamoto , C. Yanagisawa , Y. Yang , T. Yano , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , R. Zaki , A. Zalewska , J. Zalipska , G. Zarnecki , J. Zhang , X. Y. Zhao , H. Zheng , H. Zhong , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

We constructed a new Monte Carlo generator of events for neutrino CC single pion production on free nucleon targets. The code uses dynamical models of the DIS with the PDFs modified according to the recent JLab data and of the Delta…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jan T. Sobczyk , Jaroslaw A. Nowak , Krzysztof M. Graczyk

Coherent pion production in low energy neutrino reactions is discussed in the framework of the partially conserved axial vector current theory (PCAC). The role of lepton mass effects in suppressing production of positively charged pions is…

High Energy Physics - Phenomenology · Physics 2009-12-07 Christoph Berger

Neutrino-induced productions (neutrinoproduction) of photons and pions from nucleons and nuclei are important for the interpretation of neutrino-oscillation experiments, as they are potential backgrounds in the MiniBooNE experiment [A. A.…

Nuclear Theory · Physics 2012-09-28 Brian D. Serot , Xilin Zhang

Some of the recent progress in the physics of pion production induced by neutrinos on nucleons and nuclei is reviewed from a theoretical perspective. The importance of Watson's theorem to reconcile ANL and BNL data with the off-diagonal…

High Energy Physics - Phenomenology · Physics 2016-12-21 L. Alvarez-Ruso , E. Hernandez , J. Nieves , M. J. Vicente Vacas

We analyse neutrino-induced reactions in the small $Q^2$ region and for energies covering the production and decay of the delta resonance. One of our results is the agreement with the MiniBooNE data for $1\pi^+$ and $1\pi^0$ final states.…

High Energy Physics - Phenomenology · Physics 2013-03-05 E. A. Paschos , Dario Schalla

The precise knowledge of the single pion production cross-section of neutrino around the ~1 GeV energy region is an essential ingredient in the interpretation of neutrino oscillation experiments. The unique opportunities and prospects of…

High Energy Physics - Experiment · Physics 2008-11-26 SciBooNE Collaboration , Yasuhiro Nakajima

The MiniBooNE experiment has collected what is currently the world's largest sample of neutrino muon charged current single charged pion interactions, roughly 46,000 events. The purity of the CC1pi+ sample is 87% making this the purest…

High Energy Physics - Phenomenology · Physics 2009-12-07 Jaroslaw A. Nowak

We report the result from a search for charged-current coherent pion production induced by muon neutrinos with a mean energy of 1.3 GeV. The data are collected with a fully active scintillator detector in the K2K long-baseline neutrino…

High Energy Physics - Experiment · Physics 2009-09-09 K2K collaboration , M. Hasegawa

We present a high-statistics measurement of muon antineutrino-induced charged-current neutral pion production on a hydrocarbon target using the NOvA Near Detector. The differential cross sections as functions of the momenta and angles of…

High Energy Physics - Experiment · Physics 2026-05-12 The NOvA Collaboration

Pion production is a major source of systematic uncertainty in neutrino oscillation measurements. We report a systematic investigation of neutrino-induced pion production using MINERvA and MicroBooNE data within the GiBUU theoretical…

High Energy Physics - Experiment · Physics 2025-11-17 Qiyu Yan , Kaile Wen , Kai Gallmeister , Xianguo Lu , Ulrich Mosel , Yangheng Zheng

Understanding electron neutrino interactions is crucial for measurements of neutrino oscillations and searches for new physics in neutrino experiments. We present the first measurement of the flux-averaged $\nu_e$ + $\bar{\nu}_e$ charged…

High Energy Physics - Experiment · Physics 2025-08-06 MicroBooNE collaboration , P. Abratenko , D. Andrade Aldana , L. Arellano , J. Asaadi , A. Ashkenazi , S. Balasubramanian , B. Baller , A. Barnard , G. Barr , D. Barrow , J. Barrow , V. Basque , J. Bateman , O. Benevides Rodrigues , S. Berkman , A. Bhat , M. Bhattacharya , M. Bishai , A. Blake , B. Bogart , T. Bolton , M. B. Brunetti , L. Camilleri , D. Caratelli , F. Cavanna , G. Cerati , A. Chappell , Y. Chen , J. M. Conrad , M. Convery , L. Cooper-Troendle , J. I. Crespo-Anadon , R. Cross , M. Del Tutto , S. R. Dennis , P. Detje , R. Diurba , Z. Djurcic , K. Duffy , S. Dytman , B. Eberly , P. Englezos , A. Ereditato , J. J. Evans , C. Fang , B. T. Fleming , W. Foreman , D. Franco , A. P. Furmanski , F. Gao , D. Garcia-Gamez , S. Gardiner , G. Ge , S. Gollapinni , E. Gramellini , P. Green , H. Greenlee , L. Gu , W. Gu , R. Guenette , P. Guzowski , L. Hagaman , M. D. Handley , O. Hen , C. Hilgenberg , G. A. Horton-Smith , A. Hussain , B. Irwin , M. S. Ismail , C. James , X. Ji , J. H. Jo , R. A. Johnson , D. Kalra , G. Karagiorgi , W. Ketchum , M. Kirby , T. Kobilarcik , N. Lane , J. -Y. Li , Y. Li , K. Lin , B. R. Littlejohn , L. Liu , W. C. Louis , X. Luo , T. Mahmud , C. Mariani , J. Marshall , N. Martinez , D. A. Martinez Caicedo , S. Martynenko , A. Mastbaum , I. Mawby , N. McConkey , L. Mellet , J. Mendez , J. Micallef , T. Mohayai , A. Mogan , M. Mooney , A. F. Moor , C. D. Moore , L. Mora Lepin , M. M. Moudgalya , S. Mulleria Babu , D. Naples , A. Navrer-Agasson , N. Nayak , M. Nebot-Guinot , C. Nguyen , J. Nowak , N. Oza , O. Palamara , N. Pallat , V. Paolone , A. Papadopoulou , V. Papavassiliou , H. Parkinson , S. F. Pate , N. Patel , Z. Pavlovic , E. Piasetzky , K. Pletcher , I. Pophale , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , M. Reggiani-Guzzo , J. Rodriguez Rondon , M. Rosenberg , M. Ross-Lonergan , I. Safa , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , R. Sharankova , J. Shi , E. L. Snider , S. Soldner-Rembold , J. Spitz , M. Stancari , J. St. John , T. Strauss , A. M. Szelc , N. Taniuchi , K. Terao , C. Thorpe , D. Torbunov , D. Totani , M. Toups , A. Trettin , Y. -T. Tsai , J. Tyler , M. A. Uchida , T. Usher , B. Viren , J. Wang , M. Weber , H. Wei , A. J. White , S. Wolbers , T. Wongjirad , K. Wresilo , W. Wu , E. Yandel , T. Yang , L. E. Yates , H. W. Yu , G. P. Zeller , J. Zennamo , C. Zhang

Neutrino-induced pion production on nuclear targets is the major inelastic channel in all present-day neutrino-oscillation experiments. It has to be understood quantitatively in order to be able to reconstruct the neutrino-energy at…

Nuclear Theory · Physics 2010-05-07 T. Leitner , O. Lalakulich , O. Buss , U. Mosel , L. Alvarez-Ruso

Charged pion production via charged current $\nu_{\mu}$ interactions on plastic (CH) is studied using the MINERvA detector exposed to the NuMI wideband neutrino beam at Fermilab. Events with hadronic invariant mass W $<$ 1.4 GeV are…

With the neutrino experiments advancing toward high-precision measurements and greater emphasis on reducing systematic uncertainties, improving the single-pion production models, a major component of the hadronic activity observed in the…

High Energy Physics - Phenomenology · Physics 2025-05-08 R K Pradhan , R Lalnuntluanga , A Giri

As a result of a new improved fit to old bubble chamber data of the dominant axial C_5^A nucleon-to-Delta form factor, and due to the relevance of this form factor for neutrino induced coherent pion production, we re-evaluate our model…

High Energy Physics - Phenomenology · Physics 2010-10-27 E. Hernández , J. Nieves , M. Valverde