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Antiproton over proton and K\(^-\) over K\(^+\) multiplicity ratios at high \(z\) in DIS
The \(\bar{\rm p} \) over p multiplicity ratio is measured in deep-inelastic scattering for the first time using (anti-) protons carrying a large fraction of the virtual-photon energy, \(z>0.5\). The data were obtained by the COMPASS Collaboration using a 160 GeV muon beam impinging on an isoscal...
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creator | Amoroso, A Anosov, V Azevedo, C D R Balestra, F Barth, J Beck, R Bernhard, J Bodlak, M Bressan, A Buechele, M Burtsev, V E Chiosso, M S -U Chung Correia, P M M Crespo, M L Donskov, S V Doshita, N Dusaev, R R Faccioli, P Faessler, M Finger, M Finger, M Franco, C Friedrich, J M Gavrichtchouk, O P Gorzellik, M Gridin, A Grube, B Guskov, A D von Harrach Herrmann, F Horikawa, N C -Y Hsieh Ishimoto, S Iwata, T Joosten, R Joerg, P Ketzer, B Khaustov, G V Kolosov, V N Konorov, I Konstantinov, V F Kotzinian, A M Kouznetsov, O M Koval, A Kral, Z Kunne, F Kurek, K Lavickova, K Levorato, S Y -S Lian P -J Lin Makke, N Mallot, G K Marianski, B Martin, A Matousek, J Matsuda, T Mattson, G Meshcheryakov, G V Meyer, W Mikhasenko, M Mitrofanov, E Moretti, A Naim, C Novy, J Nukazuka, G Nunes, A S Ostrick, M Panzieri, D Paul, S Peskova, M Platchkov, S Pochodzalla, J Pretz, J Quaresma, M Reicherz, G Ryabchikov, D I Rychter, A Sandacz, A Savin, I A Schmieden, H Sinha, L Slunecka, M Srnka, A Steffen, D Sznajder, P Tessaro, S Tessarotto, F Thiel, A Tomsa, J Townsend, A Tskhay, V Veloso, J Vidon, A Wagner, M Zaremba, K Zavada, P Zavertyaev, M Zemko, M |
description | The \(\bar{\rm p} \) over p multiplicity ratio is measured in deep-inelastic scattering for the first time using (anti-) protons carrying a large fraction of the virtual-photon energy, \(z>0.5\). The data were obtained by the COMPASS Collaboration using a 160 GeV muon beam impinging on an isoscalar \(^6\)LiD target. The regime of deep-inelastic scattering is ensured by requiring \(Q^2\) > 1 (GeV/\(c\))\(^2\) for the photon virtuality and \(W > 5\) GeV/\(c^2\) for the invariant mass of the produced hadronic system. The range in Bjorken-\(x\) is restricted to \(0.01 < x < 0.40\). Protons and antiprotons are identified in the momentum range \(20 \div 60\) GeV/\(c\). In the whole studied \(z\)-region, the \(\bar{\rm p}\) over p multiplicity ratio is found to be below the lower limit expected from calculations based on leading-order perturbative Quantum Chromodynamics (pQCD). Extending our earlier analysis of the K\(^-\) over K\(^+\) multiplicity ratio by including now events with larger virtual-photon energies, this ratio becomes closer to the expectation of next-to-leading order pQCD. The results of both analyses strengthen our earlier conclusion that the phase space available for hadronisation should be taken into account in the pQCD formalism. |
doi_str_mv | 10.48550/arxiv.2003.11791 |
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The data were obtained by the COMPASS Collaboration using a 160 GeV muon beam impinging on an isoscalar \(^6\)LiD target. The regime of deep-inelastic scattering is ensured by requiring \(Q^2\) > 1 (GeV/\(c\))\(^2\) for the photon virtuality and \(W > 5\) GeV/\(c^2\) for the invariant mass of the produced hadronic system. The range in Bjorken-\(x\) is restricted to \(0.01 < x < 0.40\). Protons and antiprotons are identified in the momentum range \(20 \div 60\) GeV/\(c\). In the whole studied \(z\)-region, the \(\bar{\rm p}\) over p multiplicity ratio is found to be below the lower limit expected from calculations based on leading-order perturbative Quantum Chromodynamics (pQCD). Extending our earlier analysis of the K\(^-\) over K\(^+\) multiplicity ratio by including now events with larger virtual-photon energies, this ratio becomes closer to the expectation of next-to-leading order pQCD. The results of both analyses strengthen our earlier conclusion that the phase space available for hadronisation should be taken into account in the pQCD formalism.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2003.11791</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Antiparticles ; Antiprotons ; Inelastic scattering ; Muons ; Particle beams ; Photons ; Protons ; Quantum chromodynamics ; Quarks</subject><ispartof>arXiv.org, 2020-03</ispartof><rights>2020. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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M</creatorcontrib><title>Antiproton over proton and K\(^-\) over K\(^+\) multiplicity ratios at high \(z\) in DIS</title><title>arXiv.org</title><description>The \(\bar{\rm p} \) over p multiplicity ratio is measured in deep-inelastic scattering for the first time using (anti-) protons carrying a large fraction of the virtual-photon energy, \(z>0.5\). The data were obtained by the COMPASS Collaboration using a 160 GeV muon beam impinging on an isoscalar \(^6\)LiD target. The regime of deep-inelastic scattering is ensured by requiring \(Q^2\) > 1 (GeV/\(c\))\(^2\) for the photon virtuality and \(W > 5\) GeV/\(c^2\) for the invariant mass of the produced hadronic system. The range in Bjorken-\(x\) is restricted to \(0.01 < x < 0.40\). Protons and antiprotons are identified in the momentum range \(20 \div 60\) GeV/\(c\). In the whole studied \(z\)-region, the \(\bar{\rm p}\) over p multiplicity ratio is found to be below the lower limit expected from calculations based on leading-order perturbative Quantum Chromodynamics (pQCD). Extending our earlier analysis of the K\(^-\) over K\(^+\) multiplicity ratio by including now events with larger virtual-photon energies, this ratio becomes closer to the expectation of next-to-leading order pQCD. The results of both analyses strengthen our earlier conclusion that the phase space available for hadronisation should be taken into account in the pQCD formalism.</description><subject>Antiparticles</subject><subject>Antiprotons</subject><subject>Inelastic scattering</subject><subject>Muons</subject><subject>Particle beams</subject><subject>Photons</subject><subject>Protons</subject><subject>Quantum chromodynamics</subject><subject>Quarks</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNqNTUsPwTAAbiQSC36AWxOXiWz62MtRPEIcOTgsloaxLtPSdoJfr8IPcPre-QDoYeQHSRiiEVMPfvcJQtTHOB7jBnAIpdhLAkJaoKt1iRAiUUzCkDpgNxGGX5U0UkB5zxX8cSaOcJ26ey8dfP2PGFpxqSs7qPiBmydUzHCpITOw4OcCpu7LNriAs9WmA5onVum8-8M26C_m2-nSswe3OtcmK2WthI0yQhMaozHFEf2v9QbeJ0Wd</recordid><startdate>20200326</startdate><enddate>20200326</enddate><creator>Amoroso, A</creator><creator>Anosov, 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arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope></search><sort><creationdate>20200326</creationdate><title>Antiproton over proton and K\(^-\) over K\(^+\) multiplicity ratios at high \(z\) in DIS</title><author>Amoroso, A ; Anosov, V ; Azevedo, C D R ; Balestra, F ; Barth, J ; Beck, R ; Bernhard, J ; Bodlak, M ; Bressan, A ; Buechele, M ; Burtsev, V E ; Chiosso, M ; S -U Chung ; Correia, P M M ; Crespo, M L ; Donskov, S V ; Doshita, N ; Dusaev, R R ; Faccioli, P ; Faessler, M ; Finger, M ; Finger, M ; Franco, C ; Friedrich, J M ; Gavrichtchouk, O P ; Gorzellik, M ; Gridin, A ; Grube, B ; Guskov, A ; D von Harrach ; Herrmann, F ; Horikawa, N ; C -Y Hsieh ; Ishimoto, S ; Iwata, T ; Joosten, R ; Joerg, P ; Ketzer, B ; Khaustov, G V ; Kolosov, V N ; Konorov, I ; Konstantinov, V F ; Kotzinian, A M ; Kouznetsov, O M ; Koval, A ; Kral, Z ; Kunne, F ; Kurek, K ; Lavickova, K ; Levorato, S ; Y -S Lian ; P -J Lin ; Makke, N ; Mallot, G K ; Marianski, B ; Martin, A ; Matousek, J ; Matsuda, T ; Mattson, G ; Meshcheryakov, G V ; Meyer, W ; Mikhasenko, M ; Mitrofanov, E ; Moretti, A ; Naim, C ; Novy, J ; Nukazuka, G ; Nunes, A S ; Ostrick, M ; Panzieri, D ; Paul, S ; Peskova, M ; Platchkov, S ; Pochodzalla, J ; Pretz, J ; Quaresma, M ; Reicherz, G ; Ryabchikov, D I ; Rychter, A ; Sandacz, A ; Savin, I A ; Schmieden, H ; Sinha, L ; Slunecka, M ; Srnka, A ; Steffen, D ; Sznajder, P ; Tessaro, S ; Tessarotto, F ; Thiel, A ; Tomsa, J ; Townsend, A ; Tskhay, V ; Veloso, J ; Vidon, A ; Wagner, M ; Zaremba, K ; Zavada, P ; Zavertyaev, M ; Zemko, M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_23837093163</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Antiparticles</topic><topic>Antiprotons</topic><topic>Inelastic scattering</topic><topic>Muons</topic><topic>Particle beams</topic><topic>Photons</topic><topic>Protons</topic><topic>Quantum chromodynamics</topic><topic>Quarks</topic><toplevel>online_resources</toplevel><creatorcontrib>Amoroso, A</creatorcontrib><creatorcontrib>Anosov, V</creatorcontrib><creatorcontrib>Azevedo, C D R</creatorcontrib><creatorcontrib>Balestra, F</creatorcontrib><creatorcontrib>Barth, J</creatorcontrib><creatorcontrib>Beck, R</creatorcontrib><creatorcontrib>Bernhard, J</creatorcontrib><creatorcontrib>Bodlak, M</creatorcontrib><creatorcontrib>Bressan, A</creatorcontrib><creatorcontrib>Buechele, M</creatorcontrib><creatorcontrib>Burtsev, V E</creatorcontrib><creatorcontrib>Chiosso, M</creatorcontrib><creatorcontrib>S -U Chung</creatorcontrib><creatorcontrib>Correia, P M M</creatorcontrib><creatorcontrib>Crespo, M L</creatorcontrib><creatorcontrib>Donskov, S V</creatorcontrib><creatorcontrib>Doshita, N</creatorcontrib><creatorcontrib>Dusaev, R R</creatorcontrib><creatorcontrib>Faccioli, P</creatorcontrib><creatorcontrib>Faessler, M</creatorcontrib><creatorcontrib>Finger, M</creatorcontrib><creatorcontrib>Finger, M</creatorcontrib><creatorcontrib>Franco, C</creatorcontrib><creatorcontrib>Friedrich, J M</creatorcontrib><creatorcontrib>Gavrichtchouk, O P</creatorcontrib><creatorcontrib>Gorzellik, M</creatorcontrib><creatorcontrib>Gridin, A</creatorcontrib><creatorcontrib>Grube, B</creatorcontrib><creatorcontrib>Guskov, A</creatorcontrib><creatorcontrib>D von Harrach</creatorcontrib><creatorcontrib>Herrmann, F</creatorcontrib><creatorcontrib>Horikawa, N</creatorcontrib><creatorcontrib>C -Y Hsieh</creatorcontrib><creatorcontrib>Ishimoto, S</creatorcontrib><creatorcontrib>Iwata, T</creatorcontrib><creatorcontrib>Joosten, R</creatorcontrib><creatorcontrib>Joerg, P</creatorcontrib><creatorcontrib>Ketzer, B</creatorcontrib><creatorcontrib>Khaustov, G V</creatorcontrib><creatorcontrib>Kolosov, V N</creatorcontrib><creatorcontrib>Konorov, I</creatorcontrib><creatorcontrib>Konstantinov, V F</creatorcontrib><creatorcontrib>Kotzinian, A M</creatorcontrib><creatorcontrib>Kouznetsov, O M</creatorcontrib><creatorcontrib>Koval, A</creatorcontrib><creatorcontrib>Kral, Z</creatorcontrib><creatorcontrib>Kunne, F</creatorcontrib><creatorcontrib>Kurek, K</creatorcontrib><creatorcontrib>Lavickova, K</creatorcontrib><creatorcontrib>Levorato, S</creatorcontrib><creatorcontrib>Y -S Lian</creatorcontrib><creatorcontrib>P -J Lin</creatorcontrib><creatorcontrib>Makke, N</creatorcontrib><creatorcontrib>Mallot, G K</creatorcontrib><creatorcontrib>Marianski, B</creatorcontrib><creatorcontrib>Martin, A</creatorcontrib><creatorcontrib>Matousek, J</creatorcontrib><creatorcontrib>Matsuda, T</creatorcontrib><creatorcontrib>Mattson, G</creatorcontrib><creatorcontrib>Meshcheryakov, G V</creatorcontrib><creatorcontrib>Meyer, W</creatorcontrib><creatorcontrib>Mikhasenko, M</creatorcontrib><creatorcontrib>Mitrofanov, E</creatorcontrib><creatorcontrib>Moretti, A</creatorcontrib><creatorcontrib>Naim, C</creatorcontrib><creatorcontrib>Novy, J</creatorcontrib><creatorcontrib>Nukazuka, G</creatorcontrib><creatorcontrib>Nunes, A S</creatorcontrib><creatorcontrib>Ostrick, M</creatorcontrib><creatorcontrib>Panzieri, D</creatorcontrib><creatorcontrib>Paul, S</creatorcontrib><creatorcontrib>Peskova, M</creatorcontrib><creatorcontrib>Platchkov, S</creatorcontrib><creatorcontrib>Pochodzalla, J</creatorcontrib><creatorcontrib>Pretz, J</creatorcontrib><creatorcontrib>Quaresma, M</creatorcontrib><creatorcontrib>Reicherz, G</creatorcontrib><creatorcontrib>Ryabchikov, D I</creatorcontrib><creatorcontrib>Rychter, A</creatorcontrib><creatorcontrib>Sandacz, A</creatorcontrib><creatorcontrib>Savin, I A</creatorcontrib><creatorcontrib>Schmieden, H</creatorcontrib><creatorcontrib>Sinha, L</creatorcontrib><creatorcontrib>Slunecka, M</creatorcontrib><creatorcontrib>Srnka, A</creatorcontrib><creatorcontrib>Steffen, D</creatorcontrib><creatorcontrib>Sznajder, P</creatorcontrib><creatorcontrib>Tessaro, S</creatorcontrib><creatorcontrib>Tessarotto, F</creatorcontrib><creatorcontrib>Thiel, A</creatorcontrib><creatorcontrib>Tomsa, J</creatorcontrib><creatorcontrib>Townsend, A</creatorcontrib><creatorcontrib>Tskhay, V</creatorcontrib><creatorcontrib>Veloso, J</creatorcontrib><creatorcontrib>Vidon, A</creatorcontrib><creatorcontrib>Wagner, M</creatorcontrib><creatorcontrib>Zaremba, K</creatorcontrib><creatorcontrib>Zavada, P</creatorcontrib><creatorcontrib>Zavertyaev, M</creatorcontrib><creatorcontrib>Zemko, M</creatorcontrib><collection>ProQuest SciTech 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Collection</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Amoroso, A</au><au>Anosov, V</au><au>Azevedo, C D R</au><au>Balestra, F</au><au>Barth, J</au><au>Beck, R</au><au>Bernhard, J</au><au>Bodlak, M</au><au>Bressan, A</au><au>Buechele, M</au><au>Burtsev, V E</au><au>Chiosso, M</au><au>S -U Chung</au><au>Correia, P M M</au><au>Crespo, M L</au><au>Donskov, S V</au><au>Doshita, N</au><au>Dusaev, R R</au><au>Faccioli, P</au><au>Faessler, M</au><au>Finger, M</au><au>Finger, M</au><au>Franco, C</au><au>Friedrich, J M</au><au>Gavrichtchouk, O P</au><au>Gorzellik, M</au><au>Gridin, A</au><au>Grube, B</au><au>Guskov, A</au><au>D von Harrach</au><au>Herrmann, F</au><au>Horikawa, N</au><au>C -Y Hsieh</au><au>Ishimoto, S</au><au>Iwata, T</au><au>Joosten, R</au><au>Joerg, P</au><au>Ketzer, B</au><au>Khaustov, G V</au><au>Kolosov, V N</au><au>Konorov, I</au><au>Konstantinov, V F</au><au>Kotzinian, A M</au><au>Kouznetsov, O M</au><au>Koval, A</au><au>Kral, Z</au><au>Kunne, F</au><au>Kurek, K</au><au>Lavickova, K</au><au>Levorato, S</au><au>Y -S Lian</au><au>P -J Lin</au><au>Makke, N</au><au>Mallot, G K</au><au>Marianski, B</au><au>Martin, A</au><au>Matousek, J</au><au>Matsuda, T</au><au>Mattson, G</au><au>Meshcheryakov, G V</au><au>Meyer, W</au><au>Mikhasenko, M</au><au>Mitrofanov, E</au><au>Moretti, A</au><au>Naim, C</au><au>Novy, J</au><au>Nukazuka, G</au><au>Nunes, A S</au><au>Ostrick, M</au><au>Panzieri, D</au><au>Paul, S</au><au>Peskova, M</au><au>Platchkov, S</au><au>Pochodzalla, J</au><au>Pretz, J</au><au>Quaresma, M</au><au>Reicherz, G</au><au>Ryabchikov, D I</au><au>Rychter, A</au><au>Sandacz, A</au><au>Savin, I A</au><au>Schmieden, H</au><au>Sinha, L</au><au>Slunecka, M</au><au>Srnka, A</au><au>Steffen, D</au><au>Sznajder, P</au><au>Tessaro, S</au><au>Tessarotto, F</au><au>Thiel, A</au><au>Tomsa, J</au><au>Townsend, A</au><au>Tskhay, V</au><au>Veloso, J</au><au>Vidon, A</au><au>Wagner, M</au><au>Zaremba, K</au><au>Zavada, P</au><au>Zavertyaev, M</au><au>Zemko, M</au><format>book</format><genre>document</genre><ristype>GEN</ristype><atitle>Antiproton over proton and K\(^-\) over K\(^+\) multiplicity ratios at high \(z\) in DIS</atitle><jtitle>arXiv.org</jtitle><date>2020-03-26</date><risdate>2020</risdate><eissn>2331-8422</eissn><abstract>The \(\bar{\rm p} \) over p multiplicity ratio is measured in deep-inelastic scattering for the first time using (anti-) protons carrying a large fraction of the virtual-photon energy, \(z>0.5\). The data were obtained by the COMPASS Collaboration using a 160 GeV muon beam impinging on an isoscalar \(^6\)LiD target. The regime of deep-inelastic scattering is ensured by requiring \(Q^2\) > 1 (GeV/\(c\))\(^2\) for the photon virtuality and \(W > 5\) GeV/\(c^2\) for the invariant mass of the produced hadronic system. The range in Bjorken-\(x\) is restricted to \(0.01 < x < 0.40\). Protons and antiprotons are identified in the momentum range \(20 \div 60\) GeV/\(c\). In the whole studied \(z\)-region, the \(\bar{\rm p}\) over p multiplicity ratio is found to be below the lower limit expected from calculations based on leading-order perturbative Quantum Chromodynamics (pQCD). Extending our earlier analysis of the K\(^-\) over K\(^+\) multiplicity ratio by including now events with larger virtual-photon energies, this ratio becomes closer to the expectation of next-to-leading order pQCD. The results of both analyses strengthen our earlier conclusion that the phase space available for hadronisation should be taken into account in the pQCD formalism.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2003.11791</doi><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | EISSN: 2331-8422 |
ispartof | arXiv.org, 2020-03 |
issn | 2331-8422 |
language | eng |
recordid | cdi_proquest_journals_2383709316 |
source | Publicly Available Content Database |
subjects | Antiparticles Antiprotons Inelastic scattering Muons Particle beams Photons Protons Quantum chromodynamics Quarks |
title | Antiproton over proton and K\(^-\) over K\(^+\) multiplicity ratios at high \(z\) in DIS |
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