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Transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{NN}}$= 5.02 TeV

The transverse momentum ($p_\text{T}$) distribution for inclusive neutral pions in the very forward rapidity region has been measured, with the Large Hadron Collider forward detector (LHCf), in proton--lead collisions at nucleon-nucleon center-of-mass energies of $\sqrt{s_{NN}} = 5.02$TeV at the LHC...

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Detalles Bibliográficos
Autores principales: Adriani, O., Berti, E., Bonechi, L., Bongi, M., Castellini, G., D'Alessandro, R., Del Prete, M., Haguenauer, M., Itow, Y., Kasahara, K., Kawade, K., Makino, Y., Masuda, K., Matsubayashi, E., Menjo, H., Mitsuka, G., Muraki, Y., Papini, P., Perrot, A.-L., Pfeiffer, D., Ricciarini, S., Sako, T., Sakurai, N., Suzuki, T., Tamura, T., Tiberio, A., Torii, S., Tricomi, A., Turner, W.C.
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevC.89.065209
http://cds.cern.ch/record/1670719
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author Adriani, O.
Berti, E.
Bonechi, L.
Bongi, M.
Castellini, G.
D'Alessandro, R.
Del Prete, M.
Haguenauer, M.
Itow, Y.
Kasahara, K.
Kawade, K.
Makino, Y.
Masuda, K.
Matsubayashi, E.
Menjo, H.
Mitsuka, G.
Muraki, Y.
Papini, P.
Perrot, A.-L.
Pfeiffer, D.
Ricciarini, S.
Sako, T.
Sakurai, N.
Suzuki, T.
Tamura, T.
Tiberio, A.
Torii, S.
Tricomi, A.
Turner, W.C.
author_facet Adriani, O.
Berti, E.
Bonechi, L.
Bongi, M.
Castellini, G.
D'Alessandro, R.
Del Prete, M.
Haguenauer, M.
Itow, Y.
Kasahara, K.
Kawade, K.
Makino, Y.
Masuda, K.
Matsubayashi, E.
Menjo, H.
Mitsuka, G.
Muraki, Y.
Papini, P.
Perrot, A.-L.
Pfeiffer, D.
Ricciarini, S.
Sako, T.
Sakurai, N.
Suzuki, T.
Tamura, T.
Tiberio, A.
Torii, S.
Tricomi, A.
Turner, W.C.
author_sort Adriani, O.
collection CERN
description The transverse momentum ($p_\text{T}$) distribution for inclusive neutral pions in the very forward rapidity region has been measured, with the Large Hadron Collider forward detector (LHCf), in proton--lead collisions at nucleon-nucleon center-of-mass energies of $\sqrt{s_{NN}} = 5.02$TeV at the LHC. The $p_\text{T}$ spectra obtained in the rapidity range $-11.0 < y_\text{lab} < -8.9$ and $0 < p_\text{T} < 0.6$GeV (in the detector reference frame) show a strong suppression of the production of neutral pions after taking into account ultra-peripheral collisions. This leads to a nuclear modification factor value, relative to the interpolated $p_\text{T}$ spectra in proton-proton collisions at $\sqrt{s} = 5.02$TeV, of about 0.1--0.4. This value is compared with the predictions of several hadronic interaction Monte Carlo simulations.
id cern-1670719
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2014
record_format invenio
spelling cern-16707192022-08-10T21:10:51Zdoi:10.1103/PhysRevC.89.065209http://cds.cern.ch/record/1670719engAdriani, O.Berti, E.Bonechi, L.Bongi, M.Castellini, G.D'Alessandro, R.Del Prete, M.Haguenauer, M.Itow, Y.Kasahara, K.Kawade, K.Makino, Y.Masuda, K.Matsubayashi, E.Menjo, H.Mitsuka, G.Muraki, Y.Papini, P.Perrot, A.-L.Pfeiffer, D.Ricciarini, S.Sako, T.Sakurai, N.Suzuki, T.Tamura, T.Tiberio, A.Torii, S.Tricomi, A.Turner, W.C.Transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{NN}}$= 5.02 TeVParticle Physics - ExperimentThe transverse momentum ($p_\text{T}$) distribution for inclusive neutral pions in the very forward rapidity region has been measured, with the Large Hadron Collider forward detector (LHCf), in proton--lead collisions at nucleon-nucleon center-of-mass energies of $\sqrt{s_{NN}} = 5.02$TeV at the LHC. The $p_\text{T}$ spectra obtained in the rapidity range $-11.0 < y_\text{lab} < -8.9$ and $0 < p_\text{T} < 0.6$GeV (in the detector reference frame) show a strong suppression of the production of neutral pions after taking into account ultra-peripheral collisions. This leads to a nuclear modification factor value, relative to the interpolated $p_\text{T}$ spectra in proton-proton collisions at $\sqrt{s} = 5.02$TeV, of about 0.1--0.4. This value is compared with the predictions of several hadronic interaction Monte Carlo simulations.The transverse momentum ($p_\text{T}$) distribution for inclusive neutral pions in the very forward rapidity region has been measured, with the Large Hadron Collider forward detector (LHCf), in proton--lead collisions at nucleon-nucleon center-of-mass energies of $\sqrt{s_{NN}} = 5.02$TeV at the LHC. The $p_\text{T}$ spectra obtained in the rapidity range $-11.0 < y_\text{lab} < -8.9$ and $0 < p_\text{T} < 0.6$GeV (in the detector reference frame) show a strong suppression of the production of neutral pions after taking into account ultra-peripheral collisions. This leads to a nuclear modification factor value, relative to the interpolated $p_\text{T}$ spectra in proton-proton collisions at $\sqrt{s} = 5.02$TeV, of about 0.1--0.4. This value is compared with the predictions of several hadronic interaction Monte Carlo simulations.<p>The transverse momentum (<inline-formula><mml:math><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">T</mml:mi></mml:msub></mml:math></inline-formula>) distribution for inclusive neutral pions in the very forward rapidity region has been measured, with the Large Hadron Collider forward detector (LHCf), in proton-lead collisions at nucleon-nucleon center-of-mass energies of <inline-formula><mml:math><mml:mrow><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi mathvariant="italic">N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mrow><mml:mn>5.02</mml:mn></mml:mrow><mml:mspace width="4pt"/><mml:mi>TeV</mml:mi></mml:mrow></mml:math></inline-formula> at the LHC. The <inline-formula><mml:math><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">T</mml:mi></mml:msub></mml:math></inline-formula> spectra obtained in the rapidity range <inline-formula><mml:math><mml:mrow><mml:mo>−</mml:mo><mml:mn>11.0</mml:mn><mml:mo>&lt;</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>lab</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mo>−</mml:mo><mml:mn>8.9</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math><mml:mrow><mml:mn>0</mml:mn><mml:mo>&lt;</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">T</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mrow><mml:mn>0.6</mml:mn></mml:mrow><mml:mspace width="4pt"/><mml:mi>GeV</mml:mi></mml:mrow></mml:math></inline-formula> (in the detector reference frame) show a strong suppression of the production of neutral pions after taking into account ultraperipheral collisions. This leads to a nuclear modification factor value, relative to the interpolated <inline-formula><mml:math><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">T</mml:mi></mml:msub></mml:math></inline-formula> spectra in proton-proton collisions at <inline-formula><mml:math><mml:mrow><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mrow><mml:mn>5.02</mml:mn></mml:mrow><mml:mspace width="4pt"/><mml:mi>TeV</mml:mi></mml:mrow></mml:math></inline-formula>, of about 0.1–0.4. This value is compared with the predictions of several hadronic interaction Monte Carlo simulations.</p>CERN-PH-EP-2014-059arXiv:1403.7845CERN-PH-EP-2014-059oai:cds.cern.ch:16707192014-03-25
spellingShingle Particle Physics - Experiment
Adriani, O.
Berti, E.
Bonechi, L.
Bongi, M.
Castellini, G.
D'Alessandro, R.
Del Prete, M.
Haguenauer, M.
Itow, Y.
Kasahara, K.
Kawade, K.
Makino, Y.
Masuda, K.
Matsubayashi, E.
Menjo, H.
Mitsuka, G.
Muraki, Y.
Papini, P.
Perrot, A.-L.
Pfeiffer, D.
Ricciarini, S.
Sako, T.
Sakurai, N.
Suzuki, T.
Tamura, T.
Tiberio, A.
Torii, S.
Tricomi, A.
Turner, W.C.
Transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{NN}}$= 5.02 TeV
title Transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{NN}}$= 5.02 TeV
title_full Transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{NN}}$= 5.02 TeV
title_fullStr Transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{NN}}$= 5.02 TeV
title_full_unstemmed Transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{NN}}$= 5.02 TeV
title_short Transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{NN}}$= 5.02 TeV
title_sort transverse momentum distribution and nuclear modification factor of forward neutral pion in proton–lead collisions at $\sqrt{s_{nn}}$= 5.02 tev
topic Particle Physics - Experiment
url https://dx.doi.org/10.1103/PhysRevC.89.065209
http://cds.cern.ch/record/1670719
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