Electron-beam energy reconstruction for neutrino oscillation measurements (original) (raw)
Data availability
The raw data from this experiment are archived in the Jefferson Lab’s mass storage silo under the CLAS E2 run-period dataset. Access to these data can be facilitated by contacting either the corresponding authors or the Jefferson Lab computing centre at helpdesk@jlab.org.
Change history
25 November 2021
The linking to some of the Source Data files was originally incorrect and has now been amended.
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Acknowledgements
We acknowledge the efforts of the staff of the Accelerator and Physics Divisions at Jefferson Lab that made this experiment possible. We thank L. Pickering for useful discussions. The analysis presented here was carried out as part of the Jefferson Lab Hall B Data-Mining project supported by the US Department of Energy (DOE). The research was supported also by DOE, the US National Science Foundation, the Israel Science Foundation, the Chilean Comisión Nacional de Investigación Científica y Tecnológica, the French Centre national de la recherche scientifique and Commissariat à l'Energie Atomique et aux Energies Alternatives, the French–American Cultural Exchange, the Italian Istituto Nazionale di Fisica Nucleare, the National Research Foundation of Korea, and the UK Science and Technology Facilities Council. P. Coloma acknowledges support from project PROMETEO/2019/083. This project has been supported by the European Union Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement no. 674896 (Elusives, H2020-MSCA-ITN- 2015-674896). G.D.M. acknowledges support from the Spanish Ministerio de Economía y Competitividad and ERDF (European Regional Development Fund) under contract FIS2017-88410-P, by the University of Tokyo ICRRs Inter-University Research Program FY2020 & 2021, refs no. A07 and A06; by the Junta de Andalucia (grant no. FQM160); and by the European Union Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement no. 839481. This document was prepared by the e_4_ν Collaboration using the resources of the Fermi National Accelerator Laboratory (Fermilab), a US Department of Energy, Office of Science, HEP User Facility. Fermilab is managed by Fermi Research Alliance, LLC (FRA), acting under contract no. DE-AC02-07CH11359. Jefferson Science Associates operates the Thomas Jefferson National Accelerator Facility for the DOE, Office of Science, Office of Nuclear Physics under contract DE-AC05-06OR23177. The raw data from this experiment are archived in Jefferson Lab’s mass storage silo.
Author information
Author notes
- These authors contributed equally: M. Khachatryan and A. Papadopoulou
Authors and Affiliations
- Old Dominion University, Norfolk, VA, USA
M. Khachatryan, F. Hauenstein, L. B. Weinstein, M. J. Amaryan, D. Bulumulla, M. Hattawy, S. E. Kuhn, J. Poudel, Y. Prok & S. Stepanyan - Massachusetts Institute of Technology, Cambridge, MA, USA
A. Papadopoulou, A. Ashkenazi, F. Hauenstein, A. Nambrath, A. Hrnjic, O. Hen, A. Beck, R. Cruz-Torres, A. Denniston, I. Korover, S. May-Tal Beck, J. Pybus & E. P. Segarra - Tel Aviv University, Tel Aviv, Israel
E. Piasetzky, E. O. Cohen & M. Duer - Fermi National Accelerator Laboratory, Batavia, IL, USA
M. Betancourt - University of Pittsburgh, Pittsburgh, PA, USA
S. Dytman - Michigan State University, East Lansing, MI, USA
K. Mahn - Instituto de Física Corpuscular, Universidad de Valencia and CSIC, Valencia, Spain
P. Coloma - Universidad Autonoma de Madrid, Madrid, Spain
P. Coloma - Florida International University, Miami, Florida, USA
S. Adhikari, J. C. Carvajal, L. Guo, A. Khanal & B. Raue - The George Washington University, Washington, DC, USA
Giovanni Angelini, W. J. Briscoe, Y. Ilieva, C. W. Kim, A. Schmidt, I. I. Strakovsky & S. Strauch - Temple University, Philadelphia, PA, USA
H. Atac, M. Paolone & N. Sparveris - INFN, Ferrara, Italy
L. Barion, G. Ciullo, M. Contalbrigo, P. Lenisa, A. Movsisyan & L. L. Pappalardo - Thomas Jefferson National Accelerator Facility, Newport News, VA, USA
M. Battaglieri, S. Boiarinov, W. K. Brooks, V. D. Burkert, D. S. Carman, A. Deur, H. Egiyan, L. Elouadrhiri, G. Gavalian, F. X. Girod, L. Guo, D. Heddle, V. Kubarovsky, N. Markov, V. Mokeev, P. Nadel-Turonski, E. Pasyuk, P. Rossi, Y. G. Sharabian, S. Stepanyan, M. Ungaro & X. Wei - INFN, Genova, Italy
M. Battaglieri, A. Celentano, R. De Vita, L. Marsicano, M. Osipenko & M. Ripani - National Research Centre Kurchatov Institute - ITEP, Moscow, Russia
I. Bedlinskiy & O. Pogorelko - Duquesne University, Pittsburgh, PA, USA
F. Benmokhtar - Universita degli Studi di Brescia, Brescia, Italy
A. Bianconi, M. Leali, V. Mascagna & L. Venturelli - INFN, Pavia, Italy
A. Bianconi, M. Leali & L. Venturelli - Fairfield University, Fairfield, CT, USA
A. S. Biselli - Carnegie Mellon University, Pittsburgh, PA, USA
A. S. Biselli & R. A. Schumacher - University of Paris-Saclay, Gif-sur-Yvette, France
F. Bossu, M. Defurne & F. Sabati - Universidad Tecnica Federico Santa Maria, Valpara, Chile
W. K. Brooks, A. El Alaoui, H. Hakobyan & T. Mineeva - University Paris-Saclay, Orsay, France
P. Chatagnon, R. Dupre, M. Guidal, A. Hobart, D. Marchand, C. Munoz Camacho, S. Niccolai & E. Voutier - Lomonosov Moscow State University, Moscow, Russia
V. Chesnokov, E. Golovatch, B. S. Ishkhanov, E. L. Isupov, V. Mokeev & Iu. Skorodumina - Mississippi State University, Mississippi State, MS, USA
T. Chetry & L. El Fassi - University di Ferrara, Ferrara, Italy
G. Ciullo, P. Lenisa & L. L. Pappalardo - University of Glasgow, Glasgow, United Kingdom
L. Clark, D. I. Glazier, D. G. Ireland, K. Livingston, I. J. D. MacGregor, B. McKinnon, D. Protopopescu, G. Rosner, D. Sokhan & R. Tyson - University of Connecticut, Storrs, CT, USA
B. A. Clary, S. Diehl & K. Joo - Lamar University, Beaumont, TX, USA
P. L. Cole - Idaho State University, Pocatello, ID, USA
P. L. Cole, T. A. Forest & M. Holtrop - Florida State University, Tallahassee, FL, USA
V. Crede, P. Eugenio & A. I. Ostrovidov - INFN, Rome, Italy
A. D’Angelo, L. Lanza & A. Rizzo - Universita di Roma Tor Vergata, Rome, Italy
A. D’Angelo & A. Rizzo - Yerevan Physics Institute, Yerevan, Armenia
N. Dashyan, H. Hakobyan & H. Voskanyan - Ohio University, Athens, OH, USA
C. Djalali, K. Hicks & U. Shrestha - University of South Carolina, Columbia, SC, USA
C. Djalali, R. W. Gothe, Y. Ilieva, K. Neupane, Iu. Skorodumina, S. Strauch, N. Tyler & M. H. Wood - Argonne National Laboratory, Argonne, IL, USA
M. Ehrhart - Christopher Newport University, Newport News, VA, USA
R. Fersch & D. Heddle - INFN, Sezione di Torino, Torino, Italy
A. Filippi - University of New Hampshire, Durham, NH, USA
G. Gavalian & R. Paremuzyan - University of Richmond, Richmond, VA, USA
G. P. Gilfoyle - James Madison University, Harrisonburg, VA, USA
K. L. Giovanetti & G. Niculescu - College of William and Mary, Williamsburg, VA, USA
K. A. Griffioen & T. B. Hayward - Kyungpook National University, Daegu, Republic of Korea
H. S. Jo, W. Kim & K. Park - University of Virginia, Charlottesville, VA, USA
D. Keller, Y. Prok & J. Zhang - Norfolk State University, Norfolk, VA, USA
M. Khandaker & C. Salgado - Rensselaer Polytechnic Institute, Troy, NY, USA
V. Kubarovsky & M. Ungaro - INFN, Laboratori Nazionali di Frascati, Frascati, Italy
M. Mirazita, P. Rossi & O. Soto - Institute fur Kernphysik (Juelich), Juelich, Germany
J. Ritman - University of York, York, UK
D. Watts & N. Zachariou - Canisius College, Buffalo, NY, USA
M. H. Wood - Duke University, Durham, NC, USA
Z. W. Zhao - CERN, European Organization for Nuclear Research, Geneva, Switzerland
S. Dolan - Research Center for Cosmic Neutrinos, Institute for Cosmic Ray Research, University of Tokyo, Kashiwa, Chiba, Japan
G. D. Megias - Fermi National Accelerator Laboratory, Batavia, IL, USA
S. Gardiner
Authors
- M. Khachatryan
- A. Papadopoulou
- A. Ashkenazi
- F. Hauenstein
- A. Nambrath
- A. Hrnjic
- L. B. Weinstein
- O. Hen
- E. Piasetzky
- M. Betancourt
- S. Dytman
- K. Mahn
- P. Coloma
Consortia
the CLAS Collaboration
- M. Khachatryan
- , A. Papadopoulou
- , A. Ashkenazi
- , F. Hauenstein
- , L. B. Weinstein
- , O. Hen
- , E. Piasetzky
- , A. Nambrath
- , A. Hrnjic
- , M. Betancourt
- , S. Dytman
- , K. Mahn
- , P. Coloma
- , S. Adhikari
- , M. J. Amaryan
- , Giovanni Angelini
- , H. Atac
- , L. Barion
- , M. Battaglieri
- , I. Bedlinskiy
- , A. Beck
- , F. Benmokhtar
- , A. Bianconi
- , A. S. Biselli
- , F. Bossu
- , S. Boiarinov
- , W. J. Briscoe
- , W. K. Brooks
- , D. Bulumulla
- , V. D. Burkert
- , D. S. Carman
- , J. C. Carvajal
- , A. Celentano
- , P. Chatagnon
- , V. Chesnokov
- , T. Chetry
- , G. Ciullo
- , L. Clark
- , B. A. Clary
- , E. O. Cohen
- , P. L. Cole
- , M. Contalbrigo
- , V. Crede
- , R. Cruz-Torres
- , A. D’Angelo
- , N. Dashyan
- , R. De Vita
- , M. Defurne
- , A. Denniston
- , A. Deur
- , S. Diehl
- , C. Djalali
- , M. Duer
- , R. Dupre
- , H. Egiyan
- , M. Ehrhart
- , A. El Alaoui
- , L. El Fassi
- , L. Elouadrhiri
- , P. Eugenio
- , R. Fersch
- , A. Filippi
- , T. A. Forest
- , G. Gavalian
- , G. P. Gilfoyle
- , K. L. Giovanetti
- , F. X. Girod
- , D. I. Glazier
- , E. Golovatch
- , R. W. Gothe
- , K. A. Griffioen
- , M. Guidal
- , L. Guo
- , H. Hakobyan
- , M. Hattawy
- , T. B. Hayward
- , D. Heddle
- , K. Hicks
- , A. Hobart
- , M. Holtrop
- , Y. Ilieva
- , D. G. Ireland
- , B. S. Ishkhanov
- , E. L. Isupov
- , H. S. Jo
- , K. Joo
- , D. Keller
- , A. Khanal
- , M. Khandaker
- , C. W. Kim
- , W. Kim
- , I. Korover
- , V. Kubarovsky
- , S. E. Kuhn
- , L. Lanza
- , M. Leali
- , P. Lenisa
- , K. Livingston
- , I. J. D. MacGregor
- , D. Marchand
- , N. Markov
- , L. Marsicano
- , V. Mascagna
- , B. McKinnon
- , S. May-Tal Beck
- , T. Mineeva
- , M. Mirazita
- , V. Mokeev
- , A. Movsisyan
- , C. Munoz Camacho
- , P. Nadel-Turonski
- , K. Neupane
- , S. Niccolai
- , G. Niculescu
- , M. Osipenko
- , A. I. Ostrovidov
- , M. Paolone
- , L. L. Pappalardo
- , R. Paremuzyan
- , K. Park
- , E. Pasyuk
- , O. Pogorelko
- , J. Poudel
- , Y. Prok
- , D. Protopopescu
- , J. Pybus
- , M. Ripani
- , B. Raue
- , J. Ritman
- , A. Rizzo
- , G. Rosner
- , P. Rossi
- , F. Sabati
- , C. Salgado
- , A. Schmidt
- , R. A. Schumacher
- , E. P. Segarra
- , Y. G. Sharabian
- , U. Shrestha
- , Iu. Skorodumina
- , D. Sokhan
- , O. Soto
- , N. Sparveris
- , S. Stepanyan
- , I. I. Strakovsky
- , S. Strauch
- , N. Tyler
- , R. Tyson
- , M. Ungaro
- , L. Venturelli
- , H. Voskanyan
- , E. Voutier
- , D. Watts
- , X. Wei
- , M. H. Wood
- , N. Zachariou
- , J. Zhang
- & Z. W. Zhao
e4ν Collaboration*
- M. Khachatryan
- , A. Papadopoulou
- , A. Ashkenazi
- , F. Hauenstein
- , L. B. Weinstein
- , O. Hen
- , E. Piasetzky
- , A. Nambrath
- , A. Hrnjic
- , M. Betancourt
- , S. Dytman
- , K. Mahn
- , P. Coloma
- , S. Dolan
- , G. D. Megias
- , M. Khachatryan
- , A. Papadopoulou
- , A. Ashkenazi
- , F. Hauenstein
- , L. B. Weinstein
- , O. Hen
- , E. Piasetzky
- , A. Nambrath
- , A. Hrnjic
- , M. Betancourt
- , S. Dytman
- , K. Mahn
- , P. Coloma
- , S. Dolan
- , G. D. Megias
- & S. Gardiner
Contributions
The CEBAF Large Acceptance Spectrometer was designed and constructed by the CLAS Collaboration and Jefferson Lab. Data acquisition, processing and calibration, Monte Carlo simulations of the detector and data analyses were performed by a large number of CLAS Collaboration members, who also discussed and approved the scientific results. The analysis presented here was performed by M. Khachatryan, A.P., A.A., A. Hrnjic and A.N. with guidance from A.A., F.H., O.H., E. Piasetzky and L.B.W., and was reviewed by the CLAS Collaboration. S. Dytman., M. Betancourt and K.M. provided expertise on neutrino scattering. S. Dytman, G.M., S. Dolan and S.G. helped develop _e_-GENIE. P. Coloma performed a simulation of the DUNE sensitivity to the oscillation parameters, and determined the impact of our results on the fit.
Corresponding author
Correspondence toA. Ashkenazi.
Ethics declarations
Competing interests
The authors declare no competing interests.
Additional information
Peer review information Nature thanks Tingjun Yang and the other, anonymous, reviewer(s) for their contribution to the peer review of this work. Peer reviewer reports are available.
Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Extended data figures and tables
Extended Data Fig. 1 Energy distributions of different ν μ beams.
Left, Before oscillation at the near detector; and right, after oscillation at the far detector61,62. The vertical lines show the three electron beam energies of this measurement. The NO_ν_A far-detector beam flux is calculated using the near-detector flux and the neutrino oscillation parameters from the Particle Data Group. arb., arbitrary units.
Extended Data Fig. 2 Peak energy reconstruction fraction and width.
Left, The ratio of _e_-GENIE to data for the fraction of the weighted cross-section that reconstructs to the correct incident energy, plotted versus incident energy; and right, the e_-GENIE–data weighted cross-section ratio for events that reconstruct to the correct incident energy, plotted versus incident energy. The triangles and dashed lines indicate the G2018/data ratios and the squares and solid lines indicate the SuSAv2/data ratios. SuSAv2 is not intended to model nuclei lighter than 12C. Yellow shows the carbon, blue shows helium and green shows iron. Error bars show the 68% (1_σ) confidence limits for the statistical and point-to-point systematic uncertainties added in quadrature. Error bars are not shown when they are smaller than the size of the data point. Normalization uncertainties of 3% not shown.
Extended Data Fig. 3 Particle multiplicities and include cross-section extraction.
Left, The proton (black) and charged pion (blue) multiplicities for data (points), SuSAv2 (solid histogram) and G2018 (dashed histogram) for 2.257-GeV carbon. Right, Comparison between the inclusive C(e, e_′) cross-sections measured at 37.5° for data (points) and SuSAv2 (lines) for the 0.961- and 1.299-GeV SLAC data42 and our 1.159-GeV CLAS data. Error bars show the 68% (1_σ) confidence limits for the statistical and point-to-point systematic uncertainties added in quadrature. Error bars are not shown when they are smaller than the size of the data point. Normalization uncertainties of 3% not shown.
Extended Data Fig. 4 Energy feed-down cross-sections.
a–d, (_E_rec – _E_true)/_E_true for data (points) and SuSAv2 (lines) for 1.159 GeV (red triangles and dotted lines), 2.257 GeV (green squares and solid lines) and 4.453 GeV (blue dots and solid lines) for C _E_cal (a), C _E_QE (b), Fe _E_cal (c), and Fe E_QE (d). The plots are area-normalized and each bin has been scaled by the bin width. Error bars show the 68% (1_σ) confidence limits for the statistical and point-to-point systematic uncertainties added in quadrature. Error bars are not shown when they are smaller than the size of the data point. Normalization uncertainties of 3% not shown.
Extended Data Fig. 5 Transverse missing-momentum-dependent differential cross-section.
The cross-section plotted versus transverse missing momentum P_T for data (black points), SuSAv2 (black solid curve) and G2018 (black dotted curve). Different panels show results for different beam energy and target nucleus combinations: a–c, Carbon target at 1.159 GeV (a), 2.257 GeV (b) and 4.453 GeV (c). d, e, Iron target at 2.257 GeV (d) and 4.453 GeV (e). The 4.453-GeV yields have been scaled by four to have the same vertical scale. Coloured lines show the contributions of different processes to the SuSAv2 GENIE simulation: QE (blue), MEC (red), RES (green) and DIS (orange). Error bars show the 68% (1_σ) confidence limits for the statistical and point-to-point systematic uncertainties added in quadrature. Error bars are not shown when they are smaller than the size of the data point. Normalization uncertainties of 3% not shown.
Extended Data Fig. 6 δ_α_T-dependent differential cross-section.
a–j, The cross-section plotted versus δ_α_T (a–e) and versus δ_ϕ_T (f–j) for data (black points), SuSAv2 (black solid curve) and G2018 (black dotted curve). Different panels show results for different beam energy and target nucleus combinations: a–c, Carbon target at 1.159 GeV (a), 2.257 GeV (b) and 4.453 GeV (c). d, e, Iron target at 2.257 GeV (d) and 4.453 GeV (e). The 4.453-GeV yields have been scaled by two to have the same vertical scale. Coloured lines show the contributions of different processes to the SuSAv2 GENIE simulation: QE (blue), MEC (red), RES (green) and DIS (orange). Error bars show the 68% (1_σ_) confidence limits for the statistical and point-to-point systematic uncertainties added in quadrature. Error bars are not shown when they are smaller than the size of the data point. Normalization uncertainties of 3% not shown.
Extended Data Fig. 7 The effect of undetected pion subtraction.
The number of weighted events as a function of reconstructed energy _E_QE for 4.453-GeV Fe(e, _e_′) events for: left, events with a detected _π_± or photon (blue), events with one (red) or two (light brown) undetected _π_± or photons; and right, all (e, e_′_X) events with detected or undetected _π_± or photon (blue), (e, _e_′) events with no detected _π_± or photon (red), and (e, _e_′) events after subtraction for undetected π_± or photon (light brown). The uncertainties are statistical only and are shown at the 1_σ or 68% confidence level. Error bars are not shown when they are smaller than the size of the data point.
Extended Data Fig. 8 Acceptance and radiation corrections.
a–c, Acceptance correction factors; d–f, acceptance correction factor uncertainties; and g–i, electron radiation correction factors plotted versus _E_cal for the three incident beam energies. Results for carbon are shown in black, helium in green and iron in magenta. The left column (a, d, g) shows the 1.159-GeV results, the middle column (b, e, h) shows the 2.257-GeV results and the right column (c, f, i) shows the 4.453-GeV results.
Extended Data Fig. 9 CLAS detector and its calibration performance.
a, Cutaway drawing of CLAS showing the sector structure and the different detectors. Yellow, toroidal magnet; blue, drift chambers; magenta, Cherenkov counter; red, scintillation counters (time of flight); green, electromagnetic calorimeter. The beam enters from the upper left and the target is in the center of CLAS. CLAS detector image reproduced with permission of the CLAS Collaboration. b, The 2.257-GeV 3He(e, e_′_pp)X missing mass for data (solid histogram) and simulation (dashed histogram). c, The H(e, e_′_π +)X missing mass for data (black) and fit to data (red).
Extended Data Table 1 (e, e_′_p)1_p_0_π_ events reconstructed to the correct beam energy
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Khachatryan, M., Papadopoulou, A., Ashkenazi, A. et al. Electron-beam energy reconstruction for neutrino oscillation measurements.Nature 599, 565–570 (2021). https://doi.org/10.1038/s41586-021-04046-5
- Received: 29 June 2020
- Accepted: 22 September 2021
- Published: 24 November 2021
- Version of record: 24 November 2021
- Issue date: 25 November 2021
- DOI: https://doi.org/10.1038/s41586-021-04046-5