A quark-parton description of the deep inelastic scattering processes
Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is use...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bajpai, R P [verfasserIn] |
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| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1977 |
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| Schlagwörter: |
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| Anmerkung: |
© the Indian Academy of Sciences 1977 |
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| Übergeordnetes Werk: |
Enthalten in: Pramāna - Springer India, 1973, 9(1977), 2 vom: Aug., Seite 141-147 |
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| Übergeordnetes Werk: |
volume:9 ; year:1977 ; number:2 ; month:08 ; pages:141-147 |
| Links: |
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| DOI / URN: |
10.1007/BF02846061 |
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| Katalog-ID: |
OLC2076004025 |
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| 520 | |a Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. | ||
| 650 | 4 | |a Quark-parton model | |
| 650 | 4 | |a deep inelastic processes | |
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10.1007/BF02846061 doi (DE-627)OLC2076004025 (DE-He213)BF02846061-p DE-627 ger DE-627 rakwb eng 530 VZ Bajpai, R P verfasserin aut A quark-parton description of the deep inelastic scattering processes 1977 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1977 Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. Quark-parton model deep inelastic processes Enthalten in Pramāna Springer India, 1973 9(1977), 2 vom: Aug., Seite 141-147 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:9 year:1977 number:2 month:08 pages:141-147 https://doi.org/10.1007/BF02846061 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 9 1977 2 08 141-147 |
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10.1007/BF02846061 doi (DE-627)OLC2076004025 (DE-He213)BF02846061-p DE-627 ger DE-627 rakwb eng 530 VZ Bajpai, R P verfasserin aut A quark-parton description of the deep inelastic scattering processes 1977 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1977 Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. Quark-parton model deep inelastic processes Enthalten in Pramāna Springer India, 1973 9(1977), 2 vom: Aug., Seite 141-147 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:9 year:1977 number:2 month:08 pages:141-147 https://doi.org/10.1007/BF02846061 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 9 1977 2 08 141-147 |
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10.1007/BF02846061 doi (DE-627)OLC2076004025 (DE-He213)BF02846061-p DE-627 ger DE-627 rakwb eng 530 VZ Bajpai, R P verfasserin aut A quark-parton description of the deep inelastic scattering processes 1977 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1977 Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. Quark-parton model deep inelastic processes Enthalten in Pramāna Springer India, 1973 9(1977), 2 vom: Aug., Seite 141-147 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:9 year:1977 number:2 month:08 pages:141-147 https://doi.org/10.1007/BF02846061 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 9 1977 2 08 141-147 |
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10.1007/BF02846061 doi (DE-627)OLC2076004025 (DE-He213)BF02846061-p DE-627 ger DE-627 rakwb eng 530 VZ Bajpai, R P verfasserin aut A quark-parton description of the deep inelastic scattering processes 1977 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1977 Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. Quark-parton model deep inelastic processes Enthalten in Pramāna Springer India, 1973 9(1977), 2 vom: Aug., Seite 141-147 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:9 year:1977 number:2 month:08 pages:141-147 https://doi.org/10.1007/BF02846061 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 9 1977 2 08 141-147 |
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10.1007/BF02846061 doi (DE-627)OLC2076004025 (DE-He213)BF02846061-p DE-627 ger DE-627 rakwb eng 530 VZ Bajpai, R P verfasserin aut A quark-parton description of the deep inelastic scattering processes 1977 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1977 Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. Quark-parton model deep inelastic processes Enthalten in Pramāna Springer India, 1973 9(1977), 2 vom: Aug., Seite 141-147 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:9 year:1977 number:2 month:08 pages:141-147 https://doi.org/10.1007/BF02846061 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 9 1977 2 08 141-147 |
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Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. © the Indian Academy of Sciences 1977 |
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Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. © the Indian Academy of Sciences 1977 |
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Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. The valence quark probability distribution and the form of core quark probability distribution is fixed from the deep inelastic electroproduction data. Langacker and Suzuki prescription is used to fix thep andn quark core distribution. The differential excitation of quark currents similar to the Harari model ofe+e− annihilation process is invoked in deep inelastic electroproduction and neutrino reactions. An effective phenomenological form of the weak currents associated with new quarks and the associated nucleon structure is determined. © the Indian Academy of Sciences 1977 |
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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">OLC2076004025</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230402042252.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s1977 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02846061</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2076004025</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02846061-p</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">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Bajpai, R P</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">A quark-parton description of the deep inelastic scattering processes</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1977</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© the Indian Academy of Sciences 1977</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract A consistent description of various deep inelastic processes in a quark-parton model is presented. 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