Double $Q^2$-rescaling model and the nuclear effect of the parton distribution functions
Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Usi...
Ausführliche Beschreibung
Autor*in: |
He, Zhenmin [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1998 |
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Schlagwörter: |
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Anmerkung: |
© Springer-Verlag Berlin Heidelberg 1998 |
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Übergeordnetes Werk: |
Enthalten in: The European physical journal / C - Springer-Verlag, 1998, 4(1998), 2 vom: Juni, Seite 301-306 |
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Übergeordnetes Werk: |
volume:4 ; year:1998 ; number:2 ; month:06 ; pages:301-306 |
Links: |
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DOI / URN: |
10.1007/s100529800756 |
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Katalog-ID: |
OLC2069059022 |
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520 | |a Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. | ||
650 | 4 | |a Experimental Data | |
650 | 4 | |a Distribution Function | |
650 | 4 | |a Atomic Number | |
650 | 4 | |a Inelastic Scattering | |
650 | 4 | |a Momentum Conservation | |
700 | 1 | |a Yao, Xiaoxia |4 aut | |
700 | 1 | |a Duan, Chungui |4 aut | |
700 | 1 | |a Li, Guanglie |4 aut | |
700 | 1 | |a Peng, Hongan |4 aut | |
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10.1007/s100529800756 doi (DE-627)OLC2069059022 (DE-He213)s100529800756-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ He, Zhenmin verfasserin aut Double $Q^2$-rescaling model and the nuclear effect of the parton distribution functions 1998 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag Berlin Heidelberg 1998 Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. Experimental Data Distribution Function Atomic Number Inelastic Scattering Momentum Conservation Yao, Xiaoxia aut Duan, Chungui aut Li, Guanglie aut Peng, Hongan aut Enthalten in The European physical journal / C Springer-Verlag, 1998 4(1998), 2 vom: Juni, Seite 301-306 (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:4 year:1998 number:2 month:06 pages:301-306 https://doi.org/10.1007/s100529800756 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4029 GBV_ILN_4082 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4319 AR 4 1998 2 06 301-306 |
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10.1007/s100529800756 doi (DE-627)OLC2069059022 (DE-He213)s100529800756-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ He, Zhenmin verfasserin aut Double $Q^2$-rescaling model and the nuclear effect of the parton distribution functions 1998 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag Berlin Heidelberg 1998 Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. Experimental Data Distribution Function Atomic Number Inelastic Scattering Momentum Conservation Yao, Xiaoxia aut Duan, Chungui aut Li, Guanglie aut Peng, Hongan aut Enthalten in The European physical journal / C Springer-Verlag, 1998 4(1998), 2 vom: Juni, Seite 301-306 (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:4 year:1998 number:2 month:06 pages:301-306 https://doi.org/10.1007/s100529800756 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4029 GBV_ILN_4082 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4319 AR 4 1998 2 06 301-306 |
allfields_unstemmed |
10.1007/s100529800756 doi (DE-627)OLC2069059022 (DE-He213)s100529800756-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ He, Zhenmin verfasserin aut Double $Q^2$-rescaling model and the nuclear effect of the parton distribution functions 1998 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag Berlin Heidelberg 1998 Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. Experimental Data Distribution Function Atomic Number Inelastic Scattering Momentum Conservation Yao, Xiaoxia aut Duan, Chungui aut Li, Guanglie aut Peng, Hongan aut Enthalten in The European physical journal / C Springer-Verlag, 1998 4(1998), 2 vom: Juni, Seite 301-306 (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:4 year:1998 number:2 month:06 pages:301-306 https://doi.org/10.1007/s100529800756 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4029 GBV_ILN_4082 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4319 AR 4 1998 2 06 301-306 |
allfieldsGer |
10.1007/s100529800756 doi (DE-627)OLC2069059022 (DE-He213)s100529800756-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ He, Zhenmin verfasserin aut Double $Q^2$-rescaling model and the nuclear effect of the parton distribution functions 1998 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag Berlin Heidelberg 1998 Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. Experimental Data Distribution Function Atomic Number Inelastic Scattering Momentum Conservation Yao, Xiaoxia aut Duan, Chungui aut Li, Guanglie aut Peng, Hongan aut Enthalten in The European physical journal / C Springer-Verlag, 1998 4(1998), 2 vom: Juni, Seite 301-306 (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:4 year:1998 number:2 month:06 pages:301-306 https://doi.org/10.1007/s100529800756 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4029 GBV_ILN_4082 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4319 AR 4 1998 2 06 301-306 |
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10.1007/s100529800756 doi (DE-627)OLC2069059022 (DE-He213)s100529800756-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ He, Zhenmin verfasserin aut Double $Q^2$-rescaling model and the nuclear effect of the parton distribution functions 1998 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag Berlin Heidelberg 1998 Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. Experimental Data Distribution Function Atomic Number Inelastic Scattering Momentum Conservation Yao, Xiaoxia aut Duan, Chungui aut Li, Guanglie aut Peng, Hongan aut Enthalten in The European physical journal / C Springer-Verlag, 1998 4(1998), 2 vom: Juni, Seite 301-306 (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:4 year:1998 number:2 month:06 pages:301-306 https://doi.org/10.1007/s100529800756 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4029 GBV_ILN_4082 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4319 AR 4 1998 2 06 301-306 |
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Enthalten in The European physical journal / C 4(1998), 2 vom: Juni, Seite 301-306 volume:4 year:1998 number:2 month:06 pages:301-306 |
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Enthalten in The European physical journal / C 4(1998), 2 vom: Juni, Seite 301-306 volume:4 year:1998 number:2 month:06 pages:301-306 |
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He, Zhenmin @@aut@@ Yao, Xiaoxia @@aut@@ Duan, Chungui @@aut@@ Li, Guanglie @@aut@@ Peng, Hongan @@aut@@ |
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double $q^2$-rescaling model and the nuclear effect of the parton distribution functions |
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Double $Q^2$-rescaling model and the nuclear effect of the parton distribution functions |
abstract |
Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. © Springer-Verlag Berlin Heidelberg 1998 |
abstractGer |
Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. © Springer-Verlag Berlin Heidelberg 1998 |
abstract_unstemmed |
Abstract. In order to overcome the shortcoming of nonconservation of nuclear momentum existing in the original $Q^2$-rescaling model (O$Q^2$RM) and avoid introducing nuclear shadowing factor, we proposed a double $Q^2$-rescaling model (D$Q^2$RM) for the parton distributions of the bound nucleon. Using the experimental data of lepton-nucleus deep inelastic scattering (DIS) and the condition of the nuclear momentum conservation, the $Q^2$-rescaling parameters of various partons for Sn, Fe, Ca and C nuclei are determined. The rescaling parameters of valence quark distributions are larger than unity and gradually increase with atomic number A, on the contrary, the rescaling parameters of sea quark distributions and gluon distributions are smaller than unity, and slowly decrease with A. By using this model, the experimental data of the DIS process, the nuclear Drell-Yan process and $J/\psi$ ph otoproduction process are consistently and quite satisfactorily explained. © Springer-Verlag Berlin Heidelberg 1998 |
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