Large-angle production of charged pions with incident pion beams on nuclear targets

Measurements of the double-differential π± production cross section in the range of momentum 100≤p≤800 MeV/c and angle 0.35≤θ≤2.15 rad using π± beams incident on beryllium, aluminum, carbon, copper, tin, tantalum, and lead targets are presented. The data were taken with the large-acceptance hadron p...

Full description

Bibliographic Details
Main Authors: Apollonio, M, Artamonov, A, Bagulya, A, Barr, G, Blondel, A, Bobisut, F, Bogomilov, M, Bonesini, M, Booth, C, Borghi, S, Bunyatov, S, Burguet-Castell, J, Catanesi, MG, Cervera-Villanueva, A, Chimenti, P, Coney, L, Di Capua, E, Dore, U, Dumarchez, J, Edgecock, R, Ellis, M, Ferri, F, Gastaldi, U, Giani, S, Giannini, G
Format: Journal article
Language:English
Published: 2009
_version_ 1826265909109456896
author Apollonio, M
Artamonov, A
Bagulya, A
Barr, G
Blondel, A
Bobisut, F
Bogomilov, M
Bonesini, M
Booth, C
Borghi, S
Bunyatov, S
Burguet-Castell, J
Catanesi, MG
Cervera-Villanueva, A
Chimenti, P
Coney, L
Di Capua, E
Dore, U
Dumarchez, J
Edgecock, R
Ellis, M
Ferri, F
Gastaldi, U
Giani, S
Giannini, G
author_facet Apollonio, M
Artamonov, A
Bagulya, A
Barr, G
Blondel, A
Bobisut, F
Bogomilov, M
Bonesini, M
Booth, C
Borghi, S
Bunyatov, S
Burguet-Castell, J
Catanesi, MG
Cervera-Villanueva, A
Chimenti, P
Coney, L
Di Capua, E
Dore, U
Dumarchez, J
Edgecock, R
Ellis, M
Ferri, F
Gastaldi, U
Giani, S
Giannini, G
author_sort Apollonio, M
collection OXFORD
description Measurements of the double-differential π± production cross section in the range of momentum 100≤p≤800 MeV/c and angle 0.35≤θ≤2.15 rad using π± beams incident on beryllium, aluminum, carbon, copper, tin, tantalum, and lead targets are presented. The data were taken with the large-acceptance hadron production (HARP) detector in the T9 beam line of the CERN Proton Synchrotron. The secondary pions were produced by beams in a momentum range from 3 to 12.9GeV/c hitting a solid target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using a small-radius cylindrical time projection chamber placed inside a solenoidal magnet. Incident particles were identified by an elaborate system of beam detectors. Results are obtained for the double-differential cross sections d2σ/dp dθ at six incident-beam momenta. Data at 3,5,8, and 12GeV/c are available for all targets, while additional data at 8.9 and 12.9GeV/c were taken in positive particle beams on Be and Al targets, respectively. The measurements are compared with several generators of GEANT4 and the MARS Monte Carlo simulation. © 2009 The American Physical Society.
first_indexed 2024-03-06T20:30:58Z
format Journal article
id oxford-uuid:31050a0b-40c5-47e5-9554-23cd51db5407
institution University of Oxford
language English
last_indexed 2024-03-06T20:30:58Z
publishDate 2009
record_format dspace
spelling oxford-uuid:31050a0b-40c5-47e5-9554-23cd51db54072022-03-26T13:05:18ZLarge-angle production of charged pions with incident pion beams on nuclear targetsJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:31050a0b-40c5-47e5-9554-23cd51db5407EnglishSymplectic Elements at Oxford2009Apollonio, MArtamonov, ABagulya, ABarr, GBlondel, ABobisut, FBogomilov, MBonesini, MBooth, CBorghi, SBunyatov, SBurguet-Castell, JCatanesi, MGCervera-Villanueva, AChimenti, PConey, LDi Capua, EDore, UDumarchez, JEdgecock, REllis, MFerri, FGastaldi, UGiani, SGiannini, GMeasurements of the double-differential π± production cross section in the range of momentum 100≤p≤800 MeV/c and angle 0.35≤θ≤2.15 rad using π± beams incident on beryllium, aluminum, carbon, copper, tin, tantalum, and lead targets are presented. The data were taken with the large-acceptance hadron production (HARP) detector in the T9 beam line of the CERN Proton Synchrotron. The secondary pions were produced by beams in a momentum range from 3 to 12.9GeV/c hitting a solid target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using a small-radius cylindrical time projection chamber placed inside a solenoidal magnet. Incident particles were identified by an elaborate system of beam detectors. Results are obtained for the double-differential cross sections d2σ/dp dθ at six incident-beam momenta. Data at 3,5,8, and 12GeV/c are available for all targets, while additional data at 8.9 and 12.9GeV/c were taken in positive particle beams on Be and Al targets, respectively. The measurements are compared with several generators of GEANT4 and the MARS Monte Carlo simulation. © 2009 The American Physical Society.
spellingShingle Apollonio, M
Artamonov, A
Bagulya, A
Barr, G
Blondel, A
Bobisut, F
Bogomilov, M
Bonesini, M
Booth, C
Borghi, S
Bunyatov, S
Burguet-Castell, J
Catanesi, MG
Cervera-Villanueva, A
Chimenti, P
Coney, L
Di Capua, E
Dore, U
Dumarchez, J
Edgecock, R
Ellis, M
Ferri, F
Gastaldi, U
Giani, S
Giannini, G
Large-angle production of charged pions with incident pion beams on nuclear targets
title Large-angle production of charged pions with incident pion beams on nuclear targets
title_full Large-angle production of charged pions with incident pion beams on nuclear targets
title_fullStr Large-angle production of charged pions with incident pion beams on nuclear targets
title_full_unstemmed Large-angle production of charged pions with incident pion beams on nuclear targets
title_short Large-angle production of charged pions with incident pion beams on nuclear targets
title_sort large angle production of charged pions with incident pion beams on nuclear targets
work_keys_str_mv AT apolloniom largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT artamonova largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT bagulyaa largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT barrg largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT blondela largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT bobisutf largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT bogomilovm largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT bonesinim largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT boothc largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT borghis largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT bunyatovs largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT burguetcastellj largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT catanesimg largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT cerveravillanuevaa largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT chimentip largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT coneyl largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT dicapuae largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT doreu largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT dumarchezj largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT edgecockr largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT ellism largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT ferrif largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT gastaldiu largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT gianis largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets
AT gianninig largeangleproductionofchargedpionswithincidentpionbeamsonnucleartargets