K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy
The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD target. The regime of deep-inelasti...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Akhunzyanov, R. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2018transfer abstract |
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| Umfang: |
9 |
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| Übergeordnetes Werk: |
Enthalten in: Applying the Go/NoGo processing schema to a visual oddball task in older adults - Steiner, Genevieve Z. ELSEVIER, 2016, Amsterdam |
|---|---|
| Übergeordnetes Werk: |
volume:786 ; year:2018 ; day:10 ; month:11 ; pages:390-398 ; extent:9 |
| Links: |
|---|
| DOI / URN: |
10.1016/j.physletb.2018.09.052 |
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| Katalog-ID: |
ELV045127190 |
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| 024 | 7 | |a 10.1016/j.physletb.2018.09.052 |2 doi | |
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| 035 | |a (ELSEVIER)S0370-2693(18)30753-6 | ||
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| 041 | |a eng | ||
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| 084 | |a 77.50 |2 bkl | ||
| 100 | 1 | |a Akhunzyanov, R. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy |
| 264 | 1 | |c 2018transfer abstract | |
| 300 | |a 9 | ||
| 336 | |a nicht spezifiziert |b zzz |2 rdacontent | ||
| 337 | |a nicht spezifiziert |b z |2 rdamedia | ||
| 338 | |a nicht spezifiziert |b zu |2 rdacarrier | ||
| 520 | |a The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. | ||
| 520 | |a The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. | ||
| 700 | 1 | |a Alexeev, M.G. |4 oth | |
| 700 | 1 | |a Alexeev, G.D. |4 oth | |
| 700 | 1 | |a Amoroso, A. |4 oth | |
| 700 | 1 | |a Andrieux, V. |4 oth | |
| 700 | 1 | |a Anfimov, N.V. |4 oth | |
| 700 | 1 | |a Anosov, V. |4 oth | |
| 700 | 1 | |a Antoshkin, A. |4 oth | |
| 700 | 1 | |a Augsten, K. |4 oth | |
| 700 | 1 | |a Augustyniak, W. |4 oth | |
| 700 | 1 | |a Austregesilo, A. |4 oth | |
| 700 | 1 | |a Azevedo, C.D.R. |4 oth | |
| 700 | 1 | |a Badełek, B. |4 oth | |
| 700 | 1 | |a Balestra, F. |4 oth | |
| 700 | 1 | |a Ball, M. |4 oth | |
| 700 | 1 | |a Barth, J. |4 oth | |
| 700 | 1 | |a Beck, R. |4 oth | |
| 700 | 1 | |a Bedfer, Y. |4 oth | |
| 700 | 1 | |a Bernhard, J. |4 oth | |
| 700 | 1 | |a Bicker, K. |4 oth | |
| 700 | 1 | |a Bielert, E.R. |4 oth | |
| 700 | 1 | |a Birsa, R. |4 oth | |
| 700 | 1 | |a Bodlak, M. |4 oth | |
| 700 | 1 | |a Bordalo, P. |4 oth | |
| 700 | 1 | |a Bradamante, F. |4 oth | |
| 700 | 1 | |a Bressan, A. |4 oth | |
| 700 | 1 | |a Büchele, M. |4 oth | |
| 700 | 1 | |a Burtsev, V.E. |4 oth | |
| 700 | 1 | |a Capozza, L. |4 oth | |
| 700 | 1 | |a Chang, W.-C. |4 oth | |
| 700 | 1 | |a Chatterjee, C. |4 oth | |
| 700 | 1 | |a Chiosso, M. |4 oth | |
| 700 | 1 | |a Chumakov, A.G. |4 oth | |
| 700 | 1 | |a Chung, S.-U. |4 oth | |
| 700 | 1 | |a Cicuttin, A. |4 oth | |
| 700 | 1 | |a Crespo, M.L. |4 oth | |
| 700 | 1 | |a Curiel, Q. |4 oth | |
| 700 | 1 | |a Dalla Torre, S. |4 oth | |
| 700 | 1 | |a Dasgupta, S.S. |4 oth | |
| 700 | 1 | |a Dasgupta, S. |4 oth | |
| 700 | 1 | |a Denisov, O.Yu. |4 oth | |
| 700 | 1 | |a Dhara, L. |4 oth | |
| 700 | 1 | |a Donskov, S.V. |4 oth | |
| 700 | 1 | |a Doshita, N. |4 oth | |
| 700 | 1 | |a Dreisbach, Ch. |4 oth | |
| 700 | 1 | |a Dünnweber, W. |4 oth | |
| 700 | 1 | |a Dusaev, R.R. |4 oth | |
| 700 | 1 | |a Dziewiecki, M. |4 oth | |
| 700 | 1 | |a Efremov, A. |4 oth | |
| 700 | 1 | |a Eversheim, P.D. |4 oth | |
| 700 | 1 | |a Faessler, M. |4 oth | |
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| 700 | 1 | |a Finger, M. |4 oth | |
| 700 | 1 | |a Finger, M. |4 oth | |
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| 700 | 1 | |a du Fresne von Hohenesche, N. |4 oth | |
| 700 | 1 | |a Friedrich, J.M. |4 oth | |
| 700 | 1 | |a Frolov, V. |4 oth | |
| 700 | 1 | |a Gautheron, F. |4 oth | |
| 700 | 1 | |a Gavrichtchouk, O.P. |4 oth | |
| 700 | 1 | |a Gerassimov, S. |4 oth | |
| 700 | 1 | |a Giarra, J. |4 oth | |
| 700 | 1 | |a Gnesi, I. |4 oth | |
| 700 | 1 | |a Gorzellik, M. |4 oth | |
| 700 | 1 | |a Grasso, A. |4 oth | |
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| 700 | 1 | |a Grosse Perdekamp, M. |4 oth | |
| 700 | 1 | |a Grube, B. |4 oth | |
| 700 | 1 | |a Guskov, A. |4 oth | |
| 700 | 1 | |a Hahne, D. |4 oth | |
| 700 | 1 | |a Hamar, G. |4 oth | |
| 700 | 1 | |a von Harrach, D. |4 oth | |
| 700 | 1 | |a Heitz, R. |4 oth | |
| 700 | 1 | |a Herrmann, F. |4 oth | |
| 700 | 1 | |a Horikawa, N. |4 oth | |
| 700 | 1 | |a d'Hose, N. |4 oth | |
| 700 | 1 | |a Hsieh, C.-Y. |4 oth | |
| 700 | 1 | |a Huber, S. |4 oth | |
| 700 | 1 | |a Ishimoto, S. |4 oth | |
| 700 | 1 | |a Ivanov, A. |4 oth | |
| 700 | 1 | |a Iwata, T. |4 oth | |
| 700 | 1 | |a Jary, V. |4 oth | |
| 700 | 1 | |a Joosten, R. |4 oth | |
| 700 | 1 | |a Jörg, P. |4 oth | |
| 700 | 1 | |a Kabuß, E. |4 oth | |
| 700 | 1 | |a Kerbizi, A. |4 oth | |
| 700 | 1 | |a Ketzer, B. |4 oth | |
| 700 | 1 | |a Khaustov, G.V. |4 oth | |
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| 700 | 1 | |a Kisselev, Yu. |4 oth | |
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| 700 | 1 | |a Kolosov, V.N. |4 oth | |
| 700 | 1 | |a Kondo, K. |4 oth | |
| 700 | 1 | |a Konorov, I. |4 oth | |
| 700 | 1 | |a Konstantinov, V.F. |4 oth | |
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| 700 | 1 | |a Kouznetsov, O.M. |4 oth | |
| 700 | 1 | |a Kral, Z. |4 oth | |
| 700 | 1 | |a Krämer, M. |4 oth | |
| 700 | 1 | |a Krinner, F. |4 oth | |
| 700 | 1 | |a Kroumchtein, Z.V. |4 oth | |
| 700 | 1 | |a Kulinich, Y. |4 oth | |
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| 700 | 1 | |a Kurek, K. |4 oth | |
| 700 | 1 | |a Kurjata, R.P. |4 oth | |
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| 700 | 1 | |a Kveton, A. |4 oth | |
| 700 | 1 | |a Lednev, A.A. |4 oth | |
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| 700 | 1 | |a Maggiora, A. |4 oth | |
| 700 | 1 | |a Magnon, A. |4 oth | |
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| 700 | 1 | |a Matoušek, J. |4 oth | |
| 700 | 1 | |a Matsuda, H. |4 oth | |
| 700 | 1 | |a Matsuda, T. |4 oth | |
| 700 | 1 | |a Meshcheryakov, G.V. |4 oth | |
| 700 | 1 | |a Meyer, M. |4 oth | |
| 700 | 1 | |a Meyer, W. |4 oth | |
| 700 | 1 | |a Mikhailov, Yu.V. |4 oth | |
| 700 | 1 | |a Mikhasenko, M. |4 oth | |
| 700 | 1 | |a Mitrofanov, E. |4 oth | |
| 700 | 1 | |a Mitrofanov, N. |4 oth | |
| 700 | 1 | |a Miyachi, Y. |4 oth | |
| 700 | 1 | |a Moretti, A. |4 oth | |
| 700 | 1 | |a Nagaytsev, A. |4 oth | |
| 700 | 1 | |a Nerling, F. |4 oth | |
| 700 | 1 | |a Neyret, D. |4 oth | |
| 700 | 1 | |a Nový, J. |4 oth | |
| 700 | 1 | |a Nowak, W.-D. |4 oth | |
| 700 | 1 | |a Nukazuka, G. |4 oth | |
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| 700 | 1 | |a Orlov, I. |4 oth | |
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| 700 | 1 | |a Panzieri, D. |4 oth | |
| 700 | 1 | |a Parsamyan, B. |4 oth | |
| 700 | 1 | |a Paul, S. |4 oth | |
| 700 | 1 | |a Peng, J.-C. |4 oth | |
| 700 | 1 | |a Pereira, F. |4 oth | |
| 700 | 1 | |a Pesaro, G. |4 oth | |
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| 700 | 1 | |a Peshekhonov, D.V. |4 oth | |
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| 700 | 1 | |a Pretz, J. |4 oth | |
| 700 | 1 | |a Quaresma, M. |4 oth | |
| 700 | 1 | |a Quintans, C. |4 oth | |
| 700 | 1 | |a Ramos, S. |4 oth | |
| 700 | 1 | |a Regali, C. |4 oth | |
| 700 | 1 | |a Reicherz, G. |4 oth | |
| 700 | 1 | |a Riedl, C. |4 oth | |
| 700 | 1 | |a Ryabchikov, D.I. |4 oth | |
| 700 | 1 | |a Rybnikov, A. |4 oth | |
| 700 | 1 | |a Rychter, A. |4 oth | |
| 700 | 1 | |a Salac, R. |4 oth | |
| 700 | 1 | |a Samoylenko, V.D. |4 oth | |
| 700 | 1 | |a Sandacz, A. |4 oth | |
| 700 | 1 | |a Sarkar, S. |4 oth | |
| 700 | 1 | |a Savin, I.A. |4 oth | |
| 700 | 1 | |a Sawada, T. |4 oth | |
| 700 | 1 | |a Sbrizzai, G. |4 oth | |
| 700 | 1 | |a Schiavon, P. |4 oth | |
| 700 | 1 | |a Schmieden, H. |4 oth | |
| 700 | 1 | |a Seder, E. |4 oth | |
| 700 | 1 | |a Selyunin, A. |4 oth | |
| 700 | 1 | |a Silva, L. |4 oth | |
| 700 | 1 | |a Sinha, L. |4 oth | |
| 700 | 1 | |a Sirtl, S. |4 oth | |
| 700 | 1 | |a Slunecka, M. |4 oth | |
| 700 | 1 | |a Sozzi, F. |4 oth | |
| 700 | 1 | |a Smolik, J. |4 oth | |
| 700 | 1 | |a Srnka, A. |4 oth | |
| 700 | 1 | |a Steffen, D. |4 oth | |
| 700 | 1 | |a Stolarski, M. |4 oth | |
| 700 | 1 | |a Subrt, O. |4 oth | |
| 700 | 1 | |a Sulc, M. |4 oth | |
| 700 | 1 | |a Suzuki, H. |4 oth | |
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| 700 | 1 | |a Tomsa, J. |4 oth | |
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10.1016/j.physletb.2018.09.052 doi GBV00000000000446.pica (DE-627)ELV045127190 (ELSEVIER)S0370-2693(18)30753-6 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Akhunzyanov, R. verfasserin aut K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy 2018transfer abstract 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. Alexeev, M.G. oth Alexeev, G.D. oth Amoroso, A. oth Andrieux, V. oth Anfimov, N.V. oth Anosov, V. oth Antoshkin, A. oth Augsten, K. oth Augustyniak, W. oth Austregesilo, A. oth Azevedo, C.D.R. oth Badełek, B. oth Balestra, F. oth Ball, M. oth Barth, J. oth Beck, R. oth Bedfer, Y. oth Bernhard, J. oth Bicker, K. oth Bielert, E.R. oth Birsa, R. oth Bodlak, M. oth Bordalo, P. oth Bradamante, F. oth Bressan, A. oth Büchele, M. oth Burtsev, V.E. oth Capozza, L. oth Chang, W.-C. oth Chatterjee, C. oth Chiosso, M. oth Chumakov, A.G. oth Chung, S.-U. oth Cicuttin, A. oth Crespo, M.L. oth Curiel, Q. oth Dalla Torre, S. oth Dasgupta, S.S. oth Dasgupta, S. oth Denisov, O.Yu. oth Dhara, L. oth Donskov, S.V. oth Doshita, N. oth Dreisbach, Ch. oth Dünnweber, W. oth Dusaev, R.R. oth Dziewiecki, M. oth Efremov, A. oth Eversheim, P.D. oth Faessler, M. oth Ferrero, A. oth Finger, M. oth Finger, M. oth Fischer, H. oth Franco, C. oth du Fresne von Hohenesche, N. oth Friedrich, J.M. oth Frolov, V. oth Gautheron, F. oth Gavrichtchouk, O.P. oth Gerassimov, S. oth Giarra, J. oth Gnesi, I. oth Gorzellik, M. oth Grasso, A. oth Gridin, A. oth Grosse Perdekamp, M. oth Grube, B. oth Guskov, A. oth Hahne, D. oth Hamar, G. oth von Harrach, D. oth Heitz, R. oth Herrmann, F. oth Horikawa, N. oth d'Hose, N. oth Hsieh, C.-Y. oth Huber, S. oth Ishimoto, S. oth Ivanov, A. oth Iwata, T. oth Jary, V. oth Joosten, R. oth Jörg, P. oth Kabuß, E. oth Kerbizi, A. oth Ketzer, B. oth Khaustov, G.V. oth Khokhlov, Yu.A. oth Kisselev, Yu. oth Klein, F. oth Koivuniemi, J.H. oth Kolosov, V.N. oth Kondo, K. oth Konorov, I. oth Konstantinov, V.F. oth Kotzinian, A.M. oth Kouznetsov, O.M. oth Kral, Z. oth Krämer, M. oth Krinner, F. oth Kroumchtein, Z.V. oth Kulinich, Y. oth Kunne, F. oth Kurek, K. oth Kurjata, R.P. oth Kuznetsov, I.I. oth Kveton, A. oth Lednev, A.A. oth Levchenko, E.A. oth Levorato, S. oth Lian, Y.-S. oth Lichtenstadt, J. oth Longo, R. oth Lyubovitskij, V.E. oth Maggiora, A. oth Magnon, A. oth Makins, N. oth Makke, N. oth Mallot, G.K. oth Mamon, S.A. oth Marchand, C. oth Marianski, B. oth Martin, A. oth Marzec, J. oth Matoušek, J. oth Matsuda, H. oth Matsuda, T. oth Meshcheryakov, G.V. oth Meyer, M. oth Meyer, W. oth Mikhailov, Yu.V. oth Mikhasenko, M. oth Mitrofanov, E. oth Mitrofanov, N. oth Miyachi, Y. oth Moretti, A. oth Nagaytsev, A. oth Nerling, F. oth Neyret, D. oth Nový, J. oth Nowak, W.-D. oth Nukazuka, G. oth Nunes, A.S. oth Olshevsky, A.G. oth Orlov, I. oth Ostrick, M. oth Panzieri, D. oth Parsamyan, B. oth Paul, S. oth Peng, J.-C. oth Pereira, F. oth Pesaro, G. oth Pešek, M. oth Pešková, M. oth Peshekhonov, D.V. oth Pierre, N. oth Platchkov, S. oth Pochodzalla, J. oth Polyakov, V.A. oth Pretz, J. oth Quaresma, M. oth Quintans, C. oth Ramos, S. oth Regali, C. oth Reicherz, G. oth Riedl, C. oth Ryabchikov, D.I. oth Rybnikov, A. oth Rychter, A. oth Salac, R. oth Samoylenko, V.D. oth Sandacz, A. oth Sarkar, S. oth Savin, I.A. oth Sawada, T. oth Sbrizzai, G. oth Schiavon, P. oth Schmieden, H. oth Seder, E. oth Selyunin, A. oth Silva, L. oth Sinha, L. oth Sirtl, S. oth Slunecka, M. oth Sozzi, F. oth Smolik, J. oth Srnka, A. oth Steffen, D. oth Stolarski, M. oth Subrt, O. oth Sulc, M. oth Suzuki, H. oth Szabelski, A. oth Szameitat, T. oth Sznajder, P. oth Tasevsky, M. oth Tessaro, S. oth Tessarotto, F. oth Thiel, A. oth Tomsa, J. oth Tosello, F. oth Tskhay, V. oth Uhl, S. oth Vasilishin, B.I. oth Vauth, A. oth Veit, B.M. oth Veloso, J. oth Vidon, A. oth Virius, M. oth Wallner, S. oth Wilfert, M. oth Windmolders, R. oth Zaremba, K. oth Zavada, P. oth Zavertyaev, M. oth Zemlyanichkina, E. oth Ziembicki, M. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:786 year:2018 day:10 month:11 pages:390-398 extent:9 https://doi.org/10.1016/j.physletb.2018.09.052 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 786 2018 10 1110 390-398 9 |
| spelling |
10.1016/j.physletb.2018.09.052 doi GBV00000000000446.pica (DE-627)ELV045127190 (ELSEVIER)S0370-2693(18)30753-6 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Akhunzyanov, R. verfasserin aut K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy 2018transfer abstract 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. Alexeev, M.G. oth Alexeev, G.D. oth Amoroso, A. oth Andrieux, V. oth Anfimov, N.V. oth Anosov, V. oth Antoshkin, A. oth Augsten, K. oth Augustyniak, W. oth Austregesilo, A. oth Azevedo, C.D.R. oth Badełek, B. oth Balestra, F. oth Ball, M. oth Barth, J. oth Beck, R. oth Bedfer, Y. oth Bernhard, J. oth Bicker, K. oth Bielert, E.R. oth Birsa, R. oth Bodlak, M. oth Bordalo, P. oth Bradamante, F. oth Bressan, A. oth Büchele, M. oth Burtsev, V.E. oth Capozza, L. oth Chang, W.-C. oth Chatterjee, C. oth Chiosso, M. oth Chumakov, A.G. oth Chung, S.-U. oth Cicuttin, A. oth Crespo, M.L. oth Curiel, Q. oth Dalla Torre, S. oth Dasgupta, S.S. oth Dasgupta, S. oth Denisov, O.Yu. oth Dhara, L. oth Donskov, S.V. oth Doshita, N. oth Dreisbach, Ch. oth Dünnweber, W. oth Dusaev, R.R. oth Dziewiecki, M. oth Efremov, A. oth Eversheim, P.D. oth Faessler, M. oth Ferrero, A. oth Finger, M. oth Finger, M. oth Fischer, H. oth Franco, C. oth du Fresne von Hohenesche, N. oth Friedrich, J.M. oth Frolov, V. oth Gautheron, F. oth Gavrichtchouk, O.P. oth Gerassimov, S. oth Giarra, J. oth Gnesi, I. oth Gorzellik, M. oth Grasso, A. oth Gridin, A. oth Grosse Perdekamp, M. oth Grube, B. oth Guskov, A. oth Hahne, D. oth Hamar, G. oth von Harrach, D. oth Heitz, R. oth Herrmann, F. oth Horikawa, N. oth d'Hose, N. oth Hsieh, C.-Y. oth Huber, S. oth Ishimoto, S. oth Ivanov, A. oth Iwata, T. oth Jary, V. oth Joosten, R. oth Jörg, P. oth Kabuß, E. oth Kerbizi, A. oth Ketzer, B. oth Khaustov, G.V. oth Khokhlov, Yu.A. oth Kisselev, Yu. oth Klein, F. oth Koivuniemi, J.H. oth Kolosov, V.N. oth Kondo, K. oth Konorov, I. oth Konstantinov, V.F. oth Kotzinian, A.M. oth Kouznetsov, O.M. oth Kral, Z. oth Krämer, M. oth Krinner, F. oth Kroumchtein, Z.V. oth Kulinich, Y. oth Kunne, F. oth Kurek, K. oth Kurjata, R.P. oth Kuznetsov, I.I. oth Kveton, A. oth Lednev, A.A. oth Levchenko, E.A. oth Levorato, S. oth Lian, Y.-S. oth Lichtenstadt, J. oth Longo, R. oth Lyubovitskij, V.E. oth Maggiora, A. oth Magnon, A. oth Makins, N. oth Makke, N. oth Mallot, G.K. oth Mamon, S.A. oth Marchand, C. oth Marianski, B. oth Martin, A. oth Marzec, J. oth Matoušek, J. oth Matsuda, H. oth Matsuda, T. oth Meshcheryakov, G.V. oth Meyer, M. oth Meyer, W. oth Mikhailov, Yu.V. oth Mikhasenko, M. oth Mitrofanov, E. oth Mitrofanov, N. oth Miyachi, Y. oth Moretti, A. oth Nagaytsev, A. oth Nerling, F. oth Neyret, D. oth Nový, J. oth Nowak, W.-D. oth Nukazuka, G. oth Nunes, A.S. oth Olshevsky, A.G. oth Orlov, I. oth Ostrick, M. oth Panzieri, D. oth Parsamyan, B. oth Paul, S. oth Peng, J.-C. oth Pereira, F. oth Pesaro, G. oth Pešek, M. oth Pešková, M. oth Peshekhonov, D.V. oth Pierre, N. oth Platchkov, S. oth Pochodzalla, J. oth Polyakov, V.A. oth Pretz, J. oth Quaresma, M. oth Quintans, C. oth Ramos, S. oth Regali, C. oth Reicherz, G. oth Riedl, C. oth Ryabchikov, D.I. oth Rybnikov, A. oth Rychter, A. oth Salac, R. oth Samoylenko, V.D. oth Sandacz, A. oth Sarkar, S. oth Savin, I.A. oth Sawada, T. oth Sbrizzai, G. oth Schiavon, P. oth Schmieden, H. oth Seder, E. oth Selyunin, A. oth Silva, L. oth Sinha, L. oth Sirtl, S. oth Slunecka, M. oth Sozzi, F. oth Smolik, J. oth Srnka, A. oth Steffen, D. oth Stolarski, M. oth Subrt, O. oth Sulc, M. oth Suzuki, H. oth Szabelski, A. oth Szameitat, T. oth Sznajder, P. oth Tasevsky, M. oth Tessaro, S. oth Tessarotto, F. oth Thiel, A. oth Tomsa, J. oth Tosello, F. oth Tskhay, V. oth Uhl, S. oth Vasilishin, B.I. oth Vauth, A. oth Veit, B.M. oth Veloso, J. oth Vidon, A. oth Virius, M. oth Wallner, S. oth Wilfert, M. oth Windmolders, R. oth Zaremba, K. oth Zavada, P. oth Zavertyaev, M. oth Zemlyanichkina, E. oth Ziembicki, M. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:786 year:2018 day:10 month:11 pages:390-398 extent:9 https://doi.org/10.1016/j.physletb.2018.09.052 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 786 2018 10 1110 390-398 9 |
| allfields_unstemmed |
10.1016/j.physletb.2018.09.052 doi GBV00000000000446.pica (DE-627)ELV045127190 (ELSEVIER)S0370-2693(18)30753-6 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Akhunzyanov, R. verfasserin aut K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy 2018transfer abstract 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. Alexeev, M.G. oth Alexeev, G.D. oth Amoroso, A. oth Andrieux, V. oth Anfimov, N.V. oth Anosov, V. oth Antoshkin, A. oth Augsten, K. oth Augustyniak, W. oth Austregesilo, A. oth Azevedo, C.D.R. oth Badełek, B. oth Balestra, F. oth Ball, M. oth Barth, J. oth Beck, R. oth Bedfer, Y. oth Bernhard, J. oth Bicker, K. oth Bielert, E.R. oth Birsa, R. oth Bodlak, M. oth Bordalo, P. oth Bradamante, F. oth Bressan, A. oth Büchele, M. oth Burtsev, V.E. oth Capozza, L. oth Chang, W.-C. oth Chatterjee, C. oth Chiosso, M. oth Chumakov, A.G. oth Chung, S.-U. oth Cicuttin, A. oth Crespo, M.L. oth Curiel, Q. oth Dalla Torre, S. oth Dasgupta, S.S. oth Dasgupta, S. oth Denisov, O.Yu. oth Dhara, L. oth Donskov, S.V. oth Doshita, N. oth Dreisbach, Ch. oth Dünnweber, W. oth Dusaev, R.R. oth Dziewiecki, M. oth Efremov, A. oth Eversheim, P.D. oth Faessler, M. oth Ferrero, A. oth Finger, M. oth Finger, M. oth Fischer, H. oth Franco, C. oth du Fresne von Hohenesche, N. oth Friedrich, J.M. oth Frolov, V. oth Gautheron, F. oth Gavrichtchouk, O.P. oth Gerassimov, S. oth Giarra, J. oth Gnesi, I. oth Gorzellik, M. oth Grasso, A. oth Gridin, A. oth Grosse Perdekamp, M. oth Grube, B. oth Guskov, A. oth Hahne, D. oth Hamar, G. oth von Harrach, D. oth Heitz, R. oth Herrmann, F. oth Horikawa, N. oth d'Hose, N. oth Hsieh, C.-Y. oth Huber, S. oth Ishimoto, S. oth Ivanov, A. oth Iwata, T. oth Jary, V. oth Joosten, R. oth Jörg, P. oth Kabuß, E. oth Kerbizi, A. oth Ketzer, B. oth Khaustov, G.V. oth Khokhlov, Yu.A. oth Kisselev, Yu. oth Klein, F. oth Koivuniemi, J.H. oth Kolosov, V.N. oth Kondo, K. oth Konorov, I. oth Konstantinov, V.F. oth Kotzinian, A.M. oth Kouznetsov, O.M. oth Kral, Z. oth Krämer, M. oth Krinner, F. oth Kroumchtein, Z.V. oth Kulinich, Y. oth Kunne, F. oth Kurek, K. oth Kurjata, R.P. oth Kuznetsov, I.I. oth Kveton, A. oth Lednev, A.A. oth Levchenko, E.A. oth Levorato, S. oth Lian, Y.-S. oth Lichtenstadt, J. oth Longo, R. oth Lyubovitskij, V.E. oth Maggiora, A. oth Magnon, A. oth Makins, N. oth Makke, N. oth Mallot, G.K. oth Mamon, S.A. oth Marchand, C. oth Marianski, B. oth Martin, A. oth Marzec, J. oth Matoušek, J. oth Matsuda, H. oth Matsuda, T. oth Meshcheryakov, G.V. oth Meyer, M. oth Meyer, W. oth Mikhailov, Yu.V. oth Mikhasenko, M. oth Mitrofanov, E. oth Mitrofanov, N. oth Miyachi, Y. oth Moretti, A. oth Nagaytsev, A. oth Nerling, F. oth Neyret, D. oth Nový, J. oth Nowak, W.-D. oth Nukazuka, G. oth Nunes, A.S. oth Olshevsky, A.G. oth Orlov, I. oth Ostrick, M. oth Panzieri, D. oth Parsamyan, B. oth Paul, S. oth Peng, J.-C. oth Pereira, F. oth Pesaro, G. oth Pešek, M. oth Pešková, M. oth Peshekhonov, D.V. oth Pierre, N. oth Platchkov, S. oth Pochodzalla, J. oth Polyakov, V.A. oth Pretz, J. oth Quaresma, M. oth Quintans, C. oth Ramos, S. oth Regali, C. oth Reicherz, G. oth Riedl, C. oth Ryabchikov, D.I. oth Rybnikov, A. oth Rychter, A. oth Salac, R. oth Samoylenko, V.D. oth Sandacz, A. oth Sarkar, S. oth Savin, I.A. oth Sawada, T. oth Sbrizzai, G. oth Schiavon, P. oth Schmieden, H. oth Seder, E. oth Selyunin, A. oth Silva, L. oth Sinha, L. oth Sirtl, S. oth Slunecka, M. oth Sozzi, F. oth Smolik, J. oth Srnka, A. oth Steffen, D. oth Stolarski, M. oth Subrt, O. oth Sulc, M. oth Suzuki, H. oth Szabelski, A. oth Szameitat, T. oth Sznajder, P. oth Tasevsky, M. oth Tessaro, S. oth Tessarotto, F. oth Thiel, A. oth Tomsa, J. oth Tosello, F. oth Tskhay, V. oth Uhl, S. oth Vasilishin, B.I. oth Vauth, A. oth Veit, B.M. oth Veloso, J. oth Vidon, A. oth Virius, M. oth Wallner, S. oth Wilfert, M. oth Windmolders, R. oth Zaremba, K. oth Zavada, P. oth Zavertyaev, M. oth Zemlyanichkina, E. oth Ziembicki, M. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:786 year:2018 day:10 month:11 pages:390-398 extent:9 https://doi.org/10.1016/j.physletb.2018.09.052 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 786 2018 10 1110 390-398 9 |
| allfieldsGer |
10.1016/j.physletb.2018.09.052 doi GBV00000000000446.pica (DE-627)ELV045127190 (ELSEVIER)S0370-2693(18)30753-6 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Akhunzyanov, R. verfasserin aut K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy 2018transfer abstract 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. Alexeev, M.G. oth Alexeev, G.D. oth Amoroso, A. oth Andrieux, V. oth Anfimov, N.V. oth Anosov, V. oth Antoshkin, A. oth Augsten, K. oth Augustyniak, W. oth Austregesilo, A. oth Azevedo, C.D.R. oth Badełek, B. oth Balestra, F. oth Ball, M. oth Barth, J. oth Beck, R. oth Bedfer, Y. oth Bernhard, J. oth Bicker, K. oth Bielert, E.R. oth Birsa, R. oth Bodlak, M. oth Bordalo, P. oth Bradamante, F. oth Bressan, A. oth Büchele, M. oth Burtsev, V.E. oth Capozza, L. oth Chang, W.-C. oth Chatterjee, C. oth Chiosso, M. oth Chumakov, A.G. oth Chung, S.-U. oth Cicuttin, A. oth Crespo, M.L. oth Curiel, Q. oth Dalla Torre, S. oth Dasgupta, S.S. oth Dasgupta, S. oth Denisov, O.Yu. oth Dhara, L. oth Donskov, S.V. oth Doshita, N. oth Dreisbach, Ch. oth Dünnweber, W. oth Dusaev, R.R. oth Dziewiecki, M. oth Efremov, A. oth Eversheim, P.D. oth Faessler, M. oth Ferrero, A. oth Finger, M. oth Finger, M. oth Fischer, H. oth Franco, C. oth du Fresne von Hohenesche, N. oth Friedrich, J.M. oth Frolov, V. oth Gautheron, F. oth Gavrichtchouk, O.P. oth Gerassimov, S. oth Giarra, J. oth Gnesi, I. oth Gorzellik, M. oth Grasso, A. oth Gridin, A. oth Grosse Perdekamp, M. oth Grube, B. oth Guskov, A. oth Hahne, D. oth Hamar, G. oth von Harrach, D. oth Heitz, R. oth Herrmann, F. oth Horikawa, N. oth d'Hose, N. oth Hsieh, C.-Y. oth Huber, S. oth Ishimoto, S. oth Ivanov, A. oth Iwata, T. oth Jary, V. oth Joosten, R. oth Jörg, P. oth Kabuß, E. oth Kerbizi, A. oth Ketzer, B. oth Khaustov, G.V. oth Khokhlov, Yu.A. oth Kisselev, Yu. oth Klein, F. oth Koivuniemi, J.H. oth Kolosov, V.N. oth Kondo, K. oth Konorov, I. oth Konstantinov, V.F. oth Kotzinian, A.M. oth Kouznetsov, O.M. oth Kral, Z. oth Krämer, M. oth Krinner, F. oth Kroumchtein, Z.V. oth Kulinich, Y. oth Kunne, F. oth Kurek, K. oth Kurjata, R.P. oth Kuznetsov, I.I. oth Kveton, A. oth Lednev, A.A. oth Levchenko, E.A. oth Levorato, S. oth Lian, Y.-S. oth Lichtenstadt, J. oth Longo, R. oth Lyubovitskij, V.E. oth Maggiora, A. oth Magnon, A. oth Makins, N. oth Makke, N. oth Mallot, G.K. oth Mamon, S.A. oth Marchand, C. oth Marianski, B. oth Martin, A. oth Marzec, J. oth Matoušek, J. oth Matsuda, H. oth Matsuda, T. oth Meshcheryakov, G.V. oth Meyer, M. oth Meyer, W. oth Mikhailov, Yu.V. oth Mikhasenko, M. oth Mitrofanov, E. oth Mitrofanov, N. oth Miyachi, Y. oth Moretti, A. oth Nagaytsev, A. oth Nerling, F. oth Neyret, D. oth Nový, J. oth Nowak, W.-D. oth Nukazuka, G. oth Nunes, A.S. oth Olshevsky, A.G. oth Orlov, I. oth Ostrick, M. oth Panzieri, D. oth Parsamyan, B. oth Paul, S. oth Peng, J.-C. oth Pereira, F. oth Pesaro, G. oth Pešek, M. oth Pešková, M. oth Peshekhonov, D.V. oth Pierre, N. oth Platchkov, S. oth Pochodzalla, J. oth Polyakov, V.A. oth Pretz, J. oth Quaresma, M. oth Quintans, C. oth Ramos, S. oth Regali, C. oth Reicherz, G. oth Riedl, C. oth Ryabchikov, D.I. oth Rybnikov, A. oth Rychter, A. oth Salac, R. oth Samoylenko, V.D. oth Sandacz, A. oth Sarkar, S. oth Savin, I.A. oth Sawada, T. oth Sbrizzai, G. oth Schiavon, P. oth Schmieden, H. oth Seder, E. oth Selyunin, A. oth Silva, L. oth Sinha, L. oth Sirtl, S. oth Slunecka, M. oth Sozzi, F. oth Smolik, J. oth Srnka, A. oth Steffen, D. oth Stolarski, M. oth Subrt, O. oth Sulc, M. oth Suzuki, H. oth Szabelski, A. oth Szameitat, T. oth Sznajder, P. oth Tasevsky, M. oth Tessaro, S. oth Tessarotto, F. oth Thiel, A. oth Tomsa, J. oth Tosello, F. oth Tskhay, V. oth Uhl, S. oth Vasilishin, B.I. oth Vauth, A. oth Veit, B.M. oth Veloso, J. oth Vidon, A. oth Virius, M. oth Wallner, S. oth Wilfert, M. oth Windmolders, R. oth Zaremba, K. oth Zavada, P. oth Zavertyaev, M. oth Zemlyanichkina, E. oth Ziembicki, M. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:786 year:2018 day:10 month:11 pages:390-398 extent:9 https://doi.org/10.1016/j.physletb.2018.09.052 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 786 2018 10 1110 390-398 9 |
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10.1016/j.physletb.2018.09.052 doi GBV00000000000446.pica (DE-627)ELV045127190 (ELSEVIER)S0370-2693(18)30753-6 DE-627 ger DE-627 rakwb eng 610 VZ 77.50 bkl Akhunzyanov, R. verfasserin aut K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy 2018transfer abstract 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. Alexeev, M.G. oth Alexeev, G.D. oth Amoroso, A. oth Andrieux, V. oth Anfimov, N.V. oth Anosov, V. oth Antoshkin, A. oth Augsten, K. oth Augustyniak, W. oth Austregesilo, A. oth Azevedo, C.D.R. oth Badełek, B. oth Balestra, F. oth Ball, M. oth Barth, J. oth Beck, R. oth Bedfer, Y. oth Bernhard, J. oth Bicker, K. oth Bielert, E.R. oth Birsa, R. oth Bodlak, M. oth Bordalo, P. oth Bradamante, F. oth Bressan, A. oth Büchele, M. oth Burtsev, V.E. oth Capozza, L. oth Chang, W.-C. oth Chatterjee, C. oth Chiosso, M. oth Chumakov, A.G. oth Chung, S.-U. oth Cicuttin, A. oth Crespo, M.L. oth Curiel, Q. oth Dalla Torre, S. oth Dasgupta, S.S. oth Dasgupta, S. oth Denisov, O.Yu. oth Dhara, L. oth Donskov, S.V. oth Doshita, N. oth Dreisbach, Ch. oth Dünnweber, W. oth Dusaev, R.R. oth Dziewiecki, M. oth Efremov, A. oth Eversheim, P.D. oth Faessler, M. oth Ferrero, A. oth Finger, M. oth Finger, M. oth Fischer, H. oth Franco, C. oth du Fresne von Hohenesche, N. oth Friedrich, J.M. oth Frolov, V. oth Gautheron, F. oth Gavrichtchouk, O.P. oth Gerassimov, S. oth Giarra, J. oth Gnesi, I. oth Gorzellik, M. oth Grasso, A. oth Gridin, A. oth Grosse Perdekamp, M. oth Grube, B. oth Guskov, A. oth Hahne, D. oth Hamar, G. oth von Harrach, D. oth Heitz, R. oth Herrmann, F. oth Horikawa, N. oth d'Hose, N. oth Hsieh, C.-Y. oth Huber, S. oth Ishimoto, S. oth Ivanov, A. oth Iwata, T. oth Jary, V. oth Joosten, R. oth Jörg, P. oth Kabuß, E. oth Kerbizi, A. oth Ketzer, B. oth Khaustov, G.V. oth Khokhlov, Yu.A. oth Kisselev, Yu. oth Klein, F. oth Koivuniemi, J.H. oth Kolosov, V.N. oth Kondo, K. oth Konorov, I. oth Konstantinov, V.F. oth Kotzinian, A.M. oth Kouznetsov, O.M. oth Kral, Z. oth Krämer, M. oth Krinner, F. oth Kroumchtein, Z.V. oth Kulinich, Y. oth Kunne, F. oth Kurek, K. oth Kurjata, R.P. oth Kuznetsov, I.I. oth Kveton, A. oth Lednev, A.A. oth Levchenko, E.A. oth Levorato, S. oth Lian, Y.-S. oth Lichtenstadt, J. oth Longo, R. oth Lyubovitskij, V.E. oth Maggiora, A. oth Magnon, A. oth Makins, N. oth Makke, N. oth Mallot, G.K. oth Mamon, S.A. oth Marchand, C. oth Marianski, B. oth Martin, A. oth Marzec, J. oth Matoušek, J. oth Matsuda, H. oth Matsuda, T. oth Meshcheryakov, G.V. oth Meyer, M. oth Meyer, W. oth Mikhailov, Yu.V. oth Mikhasenko, M. oth Mitrofanov, E. oth Mitrofanov, N. oth Miyachi, Y. oth Moretti, A. oth Nagaytsev, A. oth Nerling, F. oth Neyret, D. oth Nový, J. oth Nowak, W.-D. oth Nukazuka, G. oth Nunes, A.S. oth Olshevsky, A.G. oth Orlov, I. oth Ostrick, M. oth Panzieri, D. oth Parsamyan, B. oth Paul, S. oth Peng, J.-C. oth Pereira, F. oth Pesaro, G. oth Pešek, M. oth Pešková, M. oth Peshekhonov, D.V. oth Pierre, N. oth Platchkov, S. oth Pochodzalla, J. oth Polyakov, V.A. oth Pretz, J. oth Quaresma, M. oth Quintans, C. oth Ramos, S. oth Regali, C. oth Reicherz, G. oth Riedl, C. oth Ryabchikov, D.I. oth Rybnikov, A. oth Rychter, A. oth Salac, R. oth Samoylenko, V.D. oth Sandacz, A. oth Sarkar, S. oth Savin, I.A. oth Sawada, T. oth Sbrizzai, G. oth Schiavon, P. oth Schmieden, H. oth Seder, E. oth Selyunin, A. oth Silva, L. oth Sinha, L. oth Sirtl, S. oth Slunecka, M. oth Sozzi, F. oth Smolik, J. oth Srnka, A. oth Steffen, D. oth Stolarski, M. oth Subrt, O. oth Sulc, M. oth Suzuki, H. oth Szabelski, A. oth Szameitat, T. oth Sznajder, P. oth Tasevsky, M. oth Tessaro, S. oth Tessarotto, F. oth Thiel, A. oth Tomsa, J. oth Tosello, F. oth Tskhay, V. oth Uhl, S. oth Vasilishin, B.I. oth Vauth, A. oth Veit, B.M. oth Veloso, J. oth Vidon, A. oth Virius, M. oth Wallner, S. oth Wilfert, M. oth Windmolders, R. oth Zaremba, K. oth Zavada, P. oth Zavertyaev, M. oth Zemlyanichkina, E. oth Ziembicki, M. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:786 year:2018 day:10 month:11 pages:390-398 extent:9 https://doi.org/10.1016/j.physletb.2018.09.052 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 786 2018 10 1110 390-398 9 |
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Akhunzyanov, R. @@aut@@ Alexeev, M.G. @@oth@@ Alexeev, G.D. @@oth@@ Amoroso, A. @@oth@@ Andrieux, V. @@oth@@ Anfimov, N.V. @@oth@@ Anosov, V. @@oth@@ Antoshkin, A. @@oth@@ Augsten, K. @@oth@@ Augustyniak, W. @@oth@@ Austregesilo, A. @@oth@@ Azevedo, C.D.R. @@oth@@ Badełek, B. @@oth@@ Balestra, F. @@oth@@ Ball, M. @@oth@@ Barth, J. @@oth@@ Beck, R. @@oth@@ Bedfer, Y. @@oth@@ Bernhard, J. @@oth@@ Bicker, K. @@oth@@ Bielert, E.R. @@oth@@ Birsa, R. @@oth@@ Bodlak, M. @@oth@@ Bordalo, P. @@oth@@ Bradamante, F. @@oth@@ Bressan, A. @@oth@@ Büchele, M. @@oth@@ Burtsev, V.E. @@oth@@ Capozza, L. @@oth@@ Chang, W.-C. @@oth@@ Chatterjee, C. @@oth@@ Chiosso, M. @@oth@@ Chumakov, A.G. @@oth@@ Chung, S.-U. @@oth@@ Cicuttin, A. @@oth@@ Crespo, M.L. @@oth@@ Curiel, Q. @@oth@@ Dalla Torre, S. @@oth@@ Dasgupta, S.S. @@oth@@ Dasgupta, S. @@oth@@ Denisov, O.Yu. @@oth@@ Dhara, L. @@oth@@ Donskov, S.V. @@oth@@ Doshita, N. @@oth@@ Dreisbach, Ch. @@oth@@ Dünnweber, W. @@oth@@ Dusaev, R.R. @@oth@@ Dziewiecki, M. @@oth@@ Efremov, A. @@oth@@ Eversheim, P.D. @@oth@@ Faessler, M. @@oth@@ Ferrero, A. @@oth@@ Finger, M. @@oth@@ Fischer, H. @@oth@@ Franco, C. @@oth@@ du Fresne von Hohenesche, N. @@oth@@ Friedrich, J.M. @@oth@@ Frolov, V. @@oth@@ Gautheron, F. @@oth@@ Gavrichtchouk, O.P. @@oth@@ Gerassimov, S. @@oth@@ Giarra, J. @@oth@@ Gnesi, I. @@oth@@ Gorzellik, M. @@oth@@ Grasso, A. @@oth@@ Gridin, A. @@oth@@ Grosse Perdekamp, M. @@oth@@ Grube, B. @@oth@@ Guskov, A. @@oth@@ Hahne, D. @@oth@@ Hamar, G. @@oth@@ von Harrach, D. @@oth@@ Heitz, R. @@oth@@ Herrmann, F. @@oth@@ Horikawa, N. @@oth@@ d'Hose, N. @@oth@@ Hsieh, C.-Y. @@oth@@ Huber, S. @@oth@@ Ishimoto, S. @@oth@@ Ivanov, A. @@oth@@ Iwata, T. @@oth@@ Jary, V. @@oth@@ Joosten, R. @@oth@@ Jörg, P. @@oth@@ Kabuß, E. @@oth@@ Kerbizi, A. @@oth@@ Ketzer, B. @@oth@@ Khaustov, G.V. @@oth@@ Khokhlov, Yu.A. @@oth@@ Kisselev, Yu. @@oth@@ Klein, F. @@oth@@ Koivuniemi, J.H. @@oth@@ Kolosov, V.N. @@oth@@ Kondo, K. @@oth@@ Konorov, I. @@oth@@ Konstantinov, V.F. @@oth@@ Kotzinian, A.M. @@oth@@ Kouznetsov, O.M. @@oth@@ Kral, Z. @@oth@@ Krämer, M. @@oth@@ Krinner, F. @@oth@@ Kroumchtein, Z.V. @@oth@@ Kulinich, Y. @@oth@@ Kunne, F. @@oth@@ Kurek, K. @@oth@@ Kurjata, R.P. @@oth@@ Kuznetsov, I.I. @@oth@@ Kveton, A. @@oth@@ Lednev, A.A. @@oth@@ Levchenko, E.A. @@oth@@ Levorato, S. @@oth@@ Lian, Y.-S. @@oth@@ Lichtenstadt, J. @@oth@@ Longo, R. @@oth@@ Lyubovitskij, V.E. @@oth@@ Maggiora, A. @@oth@@ Magnon, A. @@oth@@ Makins, N. @@oth@@ Makke, N. @@oth@@ Mallot, G.K. @@oth@@ Mamon, S.A. @@oth@@ Marchand, C. @@oth@@ Marianski, B. @@oth@@ Martin, A. @@oth@@ Marzec, J. @@oth@@ Matoušek, J. @@oth@@ Matsuda, H. @@oth@@ Matsuda, T. @@oth@@ Meshcheryakov, G.V. @@oth@@ Meyer, M. @@oth@@ Meyer, W. @@oth@@ Mikhailov, Yu.V. @@oth@@ Mikhasenko, M. @@oth@@ Mitrofanov, E. @@oth@@ Mitrofanov, N. @@oth@@ Miyachi, Y. @@oth@@ Moretti, A. @@oth@@ Nagaytsev, A. @@oth@@ Nerling, F. @@oth@@ Neyret, D. @@oth@@ Nový, J. @@oth@@ Nowak, W.-D. @@oth@@ Nukazuka, G. @@oth@@ Nunes, A.S. @@oth@@ Olshevsky, A.G. @@oth@@ Orlov, I. @@oth@@ Ostrick, M. @@oth@@ Panzieri, D. @@oth@@ Parsamyan, B. @@oth@@ Paul, S. @@oth@@ Peng, J.-C. @@oth@@ Pereira, F. @@oth@@ Pesaro, G. @@oth@@ Pešek, M. @@oth@@ Pešková, M. @@oth@@ Peshekhonov, D.V. @@oth@@ Pierre, N. @@oth@@ Platchkov, S. @@oth@@ Pochodzalla, J. @@oth@@ Polyakov, V.A. @@oth@@ Pretz, J. @@oth@@ Quaresma, M. @@oth@@ Quintans, C. @@oth@@ Ramos, S. @@oth@@ Regali, C. @@oth@@ Reicherz, G. @@oth@@ Riedl, C. @@oth@@ Ryabchikov, D.I. @@oth@@ Rybnikov, A. @@oth@@ Rychter, A. @@oth@@ Salac, R. @@oth@@ Samoylenko, V.D. @@oth@@ Sandacz, A. @@oth@@ Sarkar, S. @@oth@@ Savin, I.A. @@oth@@ Sawada, T. @@oth@@ Sbrizzai, G. @@oth@@ Schiavon, P. @@oth@@ Schmieden, H. @@oth@@ Seder, E. @@oth@@ Selyunin, A. @@oth@@ Silva, L. @@oth@@ Sinha, L. @@oth@@ Sirtl, S. @@oth@@ Slunecka, M. @@oth@@ Sozzi, F. @@oth@@ Smolik, J. @@oth@@ Srnka, A. @@oth@@ Steffen, D. @@oth@@ Stolarski, M. @@oth@@ Subrt, O. @@oth@@ Sulc, M. @@oth@@ Suzuki, H. @@oth@@ Szabelski, A. @@oth@@ Szameitat, T. @@oth@@ Sznajder, P. @@oth@@ Tasevsky, M. @@oth@@ Tessaro, S. @@oth@@ Tessarotto, F. @@oth@@ Thiel, A. @@oth@@ Tomsa, J. @@oth@@ Tosello, F. @@oth@@ Tskhay, V. @@oth@@ Uhl, S. @@oth@@ Vasilishin, B.I. @@oth@@ Vauth, A. @@oth@@ Veit, B.M. @@oth@@ Veloso, J. @@oth@@ Vidon, A. @@oth@@ Virius, M. @@oth@@ Wallner, S. @@oth@@ Wilfert, M. @@oth@@ Windmolders, R. @@oth@@ Zaremba, K. @@oth@@ Zavada, P. @@oth@@ Zavertyaev, M. @@oth@@ Zemlyanichkina, E. @@oth@@ Ziembicki, M. @@oth@@ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">ELV045127190</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230626010600.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">190205s2018 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1016/j.physletb.2018.09.052</subfield><subfield code="2">doi</subfield></datafield><datafield tag="028" ind1="5" ind2="2"><subfield code="a">GBV00000000000446.pica</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)ELV045127190</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(ELSEVIER)S0370-2693(18)30753-6</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">610</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">77.50</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Akhunzyanov, R.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2018transfer abstract</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">9</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Alexeev, M.G.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Alexeev, G.D.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Amoroso, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Andrieux, V.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Anfimov, N.V.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Anosov, V.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" 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K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy |
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K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy |
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Applying the Go/NoGo processing schema to a visual oddball task in older adults |
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k<ce:sup loc="post">−</ce:sup> over k<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in dis with a large fraction of the virtual-photon energy |
| title_auth |
K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy |
| abstract |
The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. |
| abstractGer |
The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. |
| abstract_unstemmed |
The K − over K + multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction z of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. This suggests that within the perturbative quantum chromodynamics formalism an additional correction may be required, which takes into account the phase space available for hadronisation. |
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| title_short |
K<ce:sup loc="post">−</ce:sup> over K<ce:sup loc="post">+</ce:sup> multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy |
| url |
https://doi.org/10.1016/j.physletb.2018.09.052 |
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Alexeev, M.G. Alexeev, G.D. Amoroso, A. Andrieux, V. Anfimov, N.V. Anosov, V. Antoshkin, A. Augsten, K. Augustyniak, W. Austregesilo, A. Azevedo, C.D.R. Badełek, B. Balestra, F. Ball, M. Barth, J. Beck, R. Bedfer, Y. Bernhard, J. Bicker, K. Bielert, E.R. Birsa, R. Bodlak, M. Bordalo, P. Bradamante, F. Bressan, A. Büchele, M. Burtsev, V.E. Capozza, L. Chang, W.-C. Chatterjee, C. Chiosso, M. Chumakov, A.G. Chung, S.-U. Cicuttin, A. Crespo, M.L. Curiel, Q. Dalla Torre, S. Dasgupta, S.S. Dasgupta, S. Denisov, O.Yu Dhara, L. Donskov, S.V. Doshita, N. Dreisbach, Ch Dünnweber, W. Dusaev, R.R. Dziewiecki, M. Efremov, A. Eversheim, P.D. Faessler, M. Ferrero, A. Finger, M. Fischer, H. Franco, C. du Fresne von Hohenesche, N. Friedrich, J.M. Frolov, V. Gautheron, F. Gavrichtchouk, O.P. Gerassimov, S. Giarra, J. Gnesi, I. Gorzellik, M. Grasso, A. Gridin, A. Grosse Perdekamp, M. Grube, B. Guskov, A. Hahne, D. Hamar, G. von Harrach, D. Heitz, R. Herrmann, F. Horikawa, N. d'Hose, N. Hsieh, C.-Y. Huber, S. Ishimoto, S. Ivanov, A. Iwata, T. Jary, V. Joosten, R. Jörg, P. Kabuß, E. Kerbizi, A. Ketzer, B. Khaustov, G.V. Khokhlov, Yu.A. Kisselev, Yu Klein, F. Koivuniemi, J.H. Kolosov, V.N. Kondo, K. Konorov, I. Konstantinov, V.F. Kotzinian, A.M. Kouznetsov, O.M. Kral, Z. Krämer, M. Krinner, F. Kroumchtein, Z.V. Kulinich, Y. Kunne, F. Kurek, K. Kurjata, R.P. Kuznetsov, I.I. Kveton, A. Lednev, A.A. Levchenko, E.A. Levorato, S. Lian, Y.-S. Lichtenstadt, J. Longo, R. Lyubovitskij, V.E. Maggiora, A. Magnon, A. Makins, N. Makke, N. Mallot, G.K. Mamon, S.A. Marchand, C. Marianski, B. Martin, A. Marzec, J. Matoušek, J. Matsuda, H. Matsuda, T. Meshcheryakov, G.V. Meyer, M. Meyer, W. Mikhailov, Yu.V. Mikhasenko, M. Mitrofanov, E. Mitrofanov, N. Miyachi, Y. Moretti, A. Nagaytsev, A. Nerling, F. Neyret, D. Nový, J. Nowak, W.-D. Nukazuka, G. Nunes, A.S. Olshevsky, A.G. Orlov, I. Ostrick, M. Panzieri, D. Parsamyan, B. Paul, S. Peng, J.-C. Pereira, F. Pesaro, G. Pešek, M. Pešková, M. Peshekhonov, D.V. Pierre, N. Platchkov, S. Pochodzalla, J. Polyakov, V.A. Pretz, J. Quaresma, M. Quintans, C. Ramos, S. Regali, C. Reicherz, G. Riedl, C. Ryabchikov, D.I. Rybnikov, A. Rychter, A. Salac, R. Samoylenko, V.D. Sandacz, A. Sarkar, S. Savin, I.A. Sawada, T. Sbrizzai, G. Schiavon, P. Schmieden, H. Seder, E. Selyunin, A. Silva, L. Sinha, L. Sirtl, S. Slunecka, M. Sozzi, F. Smolik, J. Srnka, A. Steffen, D. Stolarski, M. Subrt, O. Sulc, M. Suzuki, H. Szabelski, A. Szameitat, T. Sznajder, P. Tasevsky, M. Tessaro, S. Tessarotto, F. Thiel, A. Tomsa, J. Tosello, F. Tskhay, V. Uhl, S. Vasilishin, B.I. Vauth, A. Veit, B.M. Veloso, J. Vidon, A. Virius, M. Wallner, S. Wilfert, M. Windmolders, R. Zaremba, K. Zavada, P. Zavertyaev, M. Zemlyanichkina, E. Ziembicki, M. |
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Alexeev, M.G. Alexeev, G.D. Amoroso, A. Andrieux, V. Anfimov, N.V. Anosov, V. Antoshkin, A. Augsten, K. Augustyniak, W. Austregesilo, A. Azevedo, C.D.R. Badełek, B. Balestra, F. Ball, M. Barth, J. Beck, R. Bedfer, Y. Bernhard, J. Bicker, K. Bielert, E.R. Birsa, R. Bodlak, M. Bordalo, P. Bradamante, F. Bressan, A. Büchele, M. Burtsev, V.E. Capozza, L. Chang, W.-C. Chatterjee, C. Chiosso, M. Chumakov, A.G. Chung, S.-U. Cicuttin, A. Crespo, M.L. Curiel, Q. Dalla Torre, S. Dasgupta, S.S. Dasgupta, S. Denisov, O.Yu Dhara, L. Donskov, S.V. Doshita, N. Dreisbach, Ch Dünnweber, W. Dusaev, R.R. Dziewiecki, M. Efremov, A. Eversheim, P.D. Faessler, M. Ferrero, A. Finger, M. Fischer, H. Franco, C. du Fresne von Hohenesche, N. Friedrich, J.M. Frolov, V. Gautheron, F. Gavrichtchouk, O.P. Gerassimov, S. Giarra, J. Gnesi, I. Gorzellik, M. Grasso, A. Gridin, A. Grosse Perdekamp, M. Grube, B. Guskov, A. Hahne, D. Hamar, G. von Harrach, D. Heitz, R. Herrmann, F. Horikawa, N. d'Hose, N. Hsieh, C.-Y. Huber, S. Ishimoto, S. Ivanov, A. Iwata, T. Jary, V. Joosten, R. Jörg, P. Kabuß, E. Kerbizi, A. Ketzer, B. Khaustov, G.V. Khokhlov, Yu.A. Kisselev, Yu Klein, F. Koivuniemi, J.H. Kolosov, V.N. Kondo, K. Konorov, I. Konstantinov, V.F. Kotzinian, A.M. Kouznetsov, O.M. Kral, Z. Krämer, M. Krinner, F. Kroumchtein, Z.V. Kulinich, Y. Kunne, F. Kurek, K. Kurjata, R.P. Kuznetsov, I.I. Kveton, A. Lednev, A.A. Levchenko, E.A. Levorato, S. Lian, Y.-S. Lichtenstadt, J. Longo, R. Lyubovitskij, V.E. Maggiora, A. Magnon, A. Makins, N. Makke, N. Mallot, G.K. Mamon, S.A. Marchand, C. Marianski, B. Martin, A. Marzec, J. Matoušek, J. Matsuda, H. Matsuda, T. Meshcheryakov, G.V. Meyer, M. Meyer, W. Mikhailov, Yu.V. Mikhasenko, M. Mitrofanov, E. Mitrofanov, N. Miyachi, Y. Moretti, A. Nagaytsev, A. Nerling, F. Neyret, D. Nový, J. Nowak, W.-D. Nukazuka, G. Nunes, A.S. Olshevsky, A.G. Orlov, I. Ostrick, M. Panzieri, D. Parsamyan, B. Paul, S. Peng, J.-C. Pereira, F. Pesaro, G. Pešek, M. Pešková, M. Peshekhonov, D.V. Pierre, N. Platchkov, S. Pochodzalla, J. Polyakov, V.A. Pretz, J. Quaresma, M. Quintans, C. Ramos, S. Regali, C. Reicherz, G. Riedl, C. Ryabchikov, D.I. Rybnikov, A. Rychter, A. Salac, R. Samoylenko, V.D. Sandacz, A. Sarkar, S. Savin, I.A. Sawada, T. Sbrizzai, G. Schiavon, P. Schmieden, H. Seder, E. Selyunin, A. Silva, L. Sinha, L. Sirtl, S. Slunecka, M. Sozzi, F. Smolik, J. Srnka, A. Steffen, D. Stolarski, M. Subrt, O. Sulc, M. Suzuki, H. Szabelski, A. Szameitat, T. Sznajder, P. Tasevsky, M. Tessaro, S. Tessarotto, F. Thiel, A. Tomsa, J. Tosello, F. Tskhay, V. Uhl, S. Vasilishin, B.I. Vauth, A. Veit, B.M. Veloso, J. Vidon, A. Virius, M. Wallner, S. Wilfert, M. Windmolders, R. Zaremba, K. Zavada, P. Zavertyaev, M. Zemlyanichkina, E. Ziembicki, M. |
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10.1016/j.physletb.2018.09.052 |
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2024-07-06T16:41:16.447Z |
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The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar 6LiD 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. Kaons are identified in the momentum range from 12 GeV/c to 40 GeV/c, thereby restricting the range in Bjorken-x to 0.01 < x < 0.40 . The z-dependence of the multiplicity ratio is studied for z > 0.75 . For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. 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For very large values of z, i.e. z > 0.8 , we observe the kaon multiplicity ratio to fall below the lower limits expected from calculations based on leading and next-to-leading order perturbative quantum chromodynamics. Also, the kaon multiplicity ratio shows a strong dependence on the missing mass of the single-kaon production process. 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