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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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Published in:arXiv.org 2020-03
Main Authors: 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, 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
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container_title arXiv.org
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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 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 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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, \(z&gt;0.5\). 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 \(Q^2\) &gt; 1 (GeV/\(c\))\(^2\) for the photon virtuality and \(W &gt; 5\) GeV/\(c^2\) for the invariant mass of the produced hadronic system. The range in Bjorken-\(x\) is restricted to \(0.01 &lt; x &lt; 0.40\). 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>
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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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