# Measurements of $$\pi ^\pm$$π± differential yields from the surface of the T2K replica target for incoming 31 GeV/c protons with the NA61/SHINE spectrometer at the CERN SPS

@article{Abgrall2016MeasurementsO,
title={Measurements of \$\$\pi ^\pm \$\$$\pi± differential yields from the surface of the T2K replica target for incoming 31 GeV/c protons with the NA61/SHINE spectrometer at the CERN SPS}, author={Nicolas Abgrall and Antoni Aduszkiewicz and M. Ajaz and Yasir Ali and Evgeny V. Andronov and Tome Anti{\vc}i{\'c} and Nikolaos G. Antoniou and Bayasgalan Baatar and F. Bay and Alain Blondel and Johannes Bl{\"u}mer and M. Bogomilov and A. V. Brandin and Alessandro Bravar and J. Brzychczyk and S. A. Bunyatov and O. V. Busygina and Panagiotis Christakoglou and Milan M. Cirkovic and Tobiasz Czopowicz and Nikolaos Davis and S. Debieux and Hans Peter Dembinski and Michael Deveaux and Fotis K. Diakonos and S. di Luise and Wojciech A. Dominik and Jacques Dumarchez and K. Dynowski and Ralph Engel and Antonio Ereditato and Grigorii Feofilov and Zolt{\'a}n Fodor and A. A. Garibov and Marek Gaździcki and Marina Golubeva and Katarzyna Grebieszkow and A. Grzeszczuk and Fedor Guber and A. Haesler and Takuya Hasegawa and Alexander E. Herv{\'e} and M. Hierholzer and Sergey Igolkin and Alexander Ivashkin and S. R. Johnson and Kre{\vs}o Kadija and A. S. Kapoyannis and Emil Kaptur and John B. Kisiel and Tsunehiro Kobayashi and V. Kolesnikov and Dimitar Kolev and Valery Kondratiev and Alexander Korzenev and Katarzyna Kowalik and S. Kowalski and Michal Koziel and Alexei Krasnoperov and Magdalena Kuich and Alexey Kurepin and D. Larsen and Andr{\'a}s L{\'a}szl{\'o} and Maciej Piotr Lewicki and V. Lyubushkin and Maja Ma{\'c}kowiak-Pawłowska and B. Maksiak and Alexander I. Malakhov and D. Mani{\'c} and A. Marcinek and Alysia Marino and K. M{\'a}rton and H. J. Mathes and Tomasz Matulewicz and Victor Anatolievich Matveev and Georgy Melkumov and B. Messerly and Geoffrey B. Mills and S. V. Morozov and Stanisław Mr{\'o}wczyński and Yoshikazu Nagai and Takeshi Nakadaira and M. Naskręt and M. Nirkko and Koichiro Nishikawa and Apostolos D. Panagiotou and Vittorio Paolone and Matej Pavin and O. Petukhov and C. Pistillo and Roman Planeta and Boris A. Popov and Magdalena Posiadała-Zezula and S. Puławski and Jovan Puzovi{\'c} and W. Rauch and Melody Ravonel and Asmita Redij and Rainer Arno Ernst Renfordt and Elzbieta Richter-Was and Arnaud Robert and Dieter R{\"o}hrich and Ewa Rondio and Markus Roth and Andr{\'e} Rubbia and Brant Rumberger and A. A. Rustamov and Maciej Rybczynski and Andrey Sadovsky and Ken Sakashita and R. Sarnecki and Katarzyna Schmidt and T. Sekiguchi and Ilya Selyuzhenkov and Andrey Seryakov and Peter Seyboth and Davide Sgalaberna and Masaru Shibata and Marcin Slodkowski and Paweł Staszel and Grzegorz Stefanek and Joanna Stepaniak and Herbert Str{\"o}bele and T. Susa and Marek Szuba and Masahiro Tada and Arkadij Taranenko and Angelika Tefelska and Dariusz Tefelski and V. V. Tereshchenko and Roumen Tsenov and Ludwik Turko and R. Ulrich and Michael Unger and Maria Vassiliou and Darko Veberi{\vc} and Vladimir Vechernin and Gyorgy Vesztergombi and Leonid Vinogradov and Andrzej Wilczek and Zbigniew Włodarczyk and A. Wojtaszek-Szwar{\'c} and Oskar Wyszynski and Kevin Yarritu and Laura Zambelli and Eric D. Zimmerman and Megan Friend and Vyacheslav Galymov and Mark Patrick Hartz and Takahiro Hiraki and Atsuko Kondo Ichikawa and Hiroshi Kubo and Kodai Matsuoka and Akira Murakami and Tsuyoshi Nakaya and Kyohei Suzuki and Martin Tzanov and M. Yu}, journal={The European Physical Journal C}, year={2016}, volume={76}, pages={1-27} } • N. Abgrall, +155 authors M. Yu • Published 2016 • Physics • The European Physical Journal C Measurements of particle emission from a replica of the T2K 90 cm-long carbon target were performed in the NA61/SHINE experiment at CERN SPS, using data collected during a high-statistics run in 2009. An efficient use of the long-target measurements for neutrino flux predictions in T2K requires dedicated reconstruction and analysis techniques. Fully-corrected differential yields of$$\pi ^\pm $$π±-mesons from the surface of the T2K replica target for incoming 31 GeV/c protons are presented. A… Expand 23 Citations Measurement of the production cross section of 31 GeV/c protons on carbon via beam attenuation in a 90-cm-long target The production cross section of 30.92 GeV/c protons on carbon is measured by the NA61/SHINE spectrometer at the CERN SPS by means of beam attenuation in a copy (replica) of the 90-cm-long target ofExpand Transverse Momentum Distributions of Pions, Kaons and Protons in p − p Interactions at 2.76 TeV • Physics • 2019 The spectra and particle yield ratios of π±, K± meson, protons and anti-protons in proton-proton (p − p) interactions at s=2.76$$ \sqrt{s}=2.76 $$TeV are presented. CRMC generators: EPOS-LHC,Expand Hadron production measurements at NA61/SHINE for precise determination of accelerator neutrino fluxes The total systematic uncertainty of the neutrino flux in accelerator-based neutrino experiments is dominated by the Monte Carlo modeling of hadronic interactions. Direct hadron productionExpand Recent hadron production measurements performed by the NA61/SHINE collaboration NA61/SHINE is a fixed target experiment which uses secondary beams produced at the CERN SPS. Hadron-hadron interactions have been recorded at beam momenta between 13 and 350 GeV/c with aExpand Study of Hadrons Produced in Proton—Carbon Interactions at 120 GeV/c Using Hadron-Production Models • Physics • 2019 Double differential yield of π±, K±, protons, and antiprotons as a function of laboratory momentum is presented using hadron production models. This study is done in several polar angle intervalsExpand New results from T2K The T2K experiment is a 295-km long-baseline neutrino experiment in Japan employing an off-axis muon neutrino beam with a ~ 0.6 GeV peak energy. The beam, produced from 30-GeV protons at the J-PARCExpand Measurements of$$\pi ^\pm $$π±,$$K^\pm $$K± and proton double differential yields from the surface of the T2K replica target for incoming 31 GeV/c protons with the NA61/SHINE spectrometer at the CERN SPS Measurements of the$$\pi ^\pm $$π±,$$K^\pm $$K±, and proton double differential yields emitted from the surface of the 90-$$\hbox {cm}$$cm-long carbon target (T2K replica) were performed for theExpand Hadron production measurements of the EMPATHIC group Long-baseline neutrino experiments produce neutrinos by colliding a beam onto a target. Hadrons produced in the target can be magnetically focused into a beam that decays in flight, yielding aExpand Research and Development for Near Detector Systems Towards Long Term Evolution of Ultra-precise Long-baseline Neutrino Experiments With the discovery of non-zero value of \theta_{13} mixing angle, the next generation of long-baseline neutrino (LBN) experiments offers the possibility of obtaining statistically significantExpand Long baseline neutrino oscillation experiments with accelerators in Japan • Physics • 2020 The development of long baseline neutrino oscillation experiments with accelerators in Japan is reviewed. Accelerator experiments can optimize experimental conditions, such as the beam and theExpand #### References SHOWING 1-10 OF 20 REFERENCES Cross Sections and Charged Pion Spectra in Proton-Carbon Interactions at 31 GeV/c • Physics • 2011 As neutrino long baseline experiments enter a new domain of precision, the careful study of systematic errors due to poor knowledge of production cross sections for pions and kaons require moreExpand Measurement of Production Properties of Positively Charged Kaons in Proton-Carbon Interactions at 31 GeV/c Spectra of positively charged kaons in p+C interactions at 31 GeV/c were measured with the NA61/SHINE spectrometer at the CERN SPS. The analysis is based on the full set of data collected in 2007Expand Measurements of production properties of K S 0 mesons and Λ hyperons in proton-carbon interactions at 31 GeV/ c Spectra of KS0 mesons and Λ hyperons were measured in p + C interactions at 31 GeV/c with the large acceptance NA61/SHINE spectrometer at the CERN SPS. The data were collected with an isotropicExpand Pion emission from the T2K replica target: Method, results and application Abstract The T2K long-baseline neutrino oscillation experiment in Japan needs precise predictions of the initial neutrino flux. The highest precision can be reached based on detailed measurements ofExpand Measurement of negatively charged pion spectra in inelastic p+p interactions at$$p_{\mathbf {lab}}= $$plab= 20, 31, 40, 80 and 158 GeV/c We present experimental results on inclusive spectra and mean multiplicities of negatively charged pions produced in inelastic p+p interactions at incident projectile momenta of 20, 31, 40, 80 andExpand T2K neutrino flux prediction The Tokai-to-Kamioka (T2K) experiment studies neutrino oscillations using an off-axis muon neutrino beam with a peak energy of about 0.6 GeV that originates at the Japan Proton Accelerator ResearchExpand Measurements of neutrino oscillation in appearance and disappearance channels by the T2K experiment with 6.6E20 protons on target We report on measurements of neutrino oscillation using data from the T2K long-baseline neutrino experiment collected between 2010 and 2013. In an analysis of muon neutrino disappearance alone, weExpand Measurements of$$\pi ^{\pm }$$π±,$$K^{\pm }$$K±,$$K^0_S$$KS0,$$\varLambda$\$Λ and proton production in proton–carbon interactions at 31 GeV/c with the NA61/SHINE spectrometer at the CERN SPS
Measurements of hadron production in p + C interactions at 31 GeV/c are performed using the NA61/SHINE spectrometer at the CERN SPS. The analysis is based on the full set of data collected in 2009Expand
The T2K Experiment
The T2K experiment is a long-baseline neutrino oscillation experiment. Its main goal is to measure the last unknown lepton sector mixing angle {\theta}_{13} by observing {\nu}_e appearance in aExpand
The NA49 large acceptance hadron detector
Abstract The NA49 detector is a wide acceptance spectrometer for the study of hadron production in p+p, p+A, and A+A collisions at the CERN SPS. The main components are 4 large-volume TPCs forExpand