Relativistic harmonic confinement of quarks and gluons
Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the sam...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Khadkikar, S B [verfasserIn] |
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| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1985 |
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| Schlagwörter: |
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| Anmerkung: |
© Indian Academy of Sciences 1985 |
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| Übergeordnetes Werk: |
Enthalten in: Pramāna - Springer India, 1973, 24(1985), 1-2 vom: Jan., Seite 63-68 |
|---|---|
| Übergeordnetes Werk: |
volume:24 ; year:1985 ; number:1-2 ; month:01 ; pages:63-68 |
| Links: |
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| DOI / URN: |
10.1007/BF02894818 |
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| Katalog-ID: |
OLC2076012672 |
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| 520 | |a Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. | ||
| 650 | 4 | |a Relativistic harmonic confinement | |
| 650 | 4 | |a quarks | |
| 650 | 4 | |a gluons | |
| 650 | 4 | |a glue-balls | |
| 650 | 4 | |a hadrons | |
| 650 | 4 | |a masses | |
| 650 | 4 | |a magnetic moments | |
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10.1007/BF02894818 doi (DE-627)OLC2076012672 (DE-He213)BF02894818-p DE-627 ger DE-627 rakwb eng 530 VZ Khadkikar, S B verfasserin aut Relativistic harmonic confinement of quarks and gluons 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1985 Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. Relativistic harmonic confinement quarks gluons glue-balls hadrons masses magnetic moments Enthalten in Pramāna Springer India, 1973 24(1985), 1-2 vom: Jan., Seite 63-68 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:24 year:1985 number:1-2 month:01 pages:63-68 https://doi.org/10.1007/BF02894818 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 AR 24 1985 1-2 01 63-68 |
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10.1007/BF02894818 doi (DE-627)OLC2076012672 (DE-He213)BF02894818-p DE-627 ger DE-627 rakwb eng 530 VZ Khadkikar, S B verfasserin aut Relativistic harmonic confinement of quarks and gluons 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1985 Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. Relativistic harmonic confinement quarks gluons glue-balls hadrons masses magnetic moments Enthalten in Pramāna Springer India, 1973 24(1985), 1-2 vom: Jan., Seite 63-68 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:24 year:1985 number:1-2 month:01 pages:63-68 https://doi.org/10.1007/BF02894818 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 AR 24 1985 1-2 01 63-68 |
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10.1007/BF02894818 doi (DE-627)OLC2076012672 (DE-He213)BF02894818-p DE-627 ger DE-627 rakwb eng 530 VZ Khadkikar, S B verfasserin aut Relativistic harmonic confinement of quarks and gluons 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1985 Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. Relativistic harmonic confinement quarks gluons glue-balls hadrons masses magnetic moments Enthalten in Pramāna Springer India, 1973 24(1985), 1-2 vom: Jan., Seite 63-68 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:24 year:1985 number:1-2 month:01 pages:63-68 https://doi.org/10.1007/BF02894818 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 AR 24 1985 1-2 01 63-68 |
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10.1007/BF02894818 doi (DE-627)OLC2076012672 (DE-He213)BF02894818-p DE-627 ger DE-627 rakwb eng 530 VZ Khadkikar, S B verfasserin aut Relativistic harmonic confinement of quarks and gluons 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1985 Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. Relativistic harmonic confinement quarks gluons glue-balls hadrons masses magnetic moments Enthalten in Pramāna Springer India, 1973 24(1985), 1-2 vom: Jan., Seite 63-68 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:24 year:1985 number:1-2 month:01 pages:63-68 https://doi.org/10.1007/BF02894818 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 AR 24 1985 1-2 01 63-68 |
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10.1007/BF02894818 doi (DE-627)OLC2076012672 (DE-He213)BF02894818-p DE-627 ger DE-627 rakwb eng 530 VZ Khadkikar, S B verfasserin aut Relativistic harmonic confinement of quarks and gluons 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1985 Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. Relativistic harmonic confinement quarks gluons glue-balls hadrons masses magnetic moments Enthalten in Pramāna Springer India, 1973 24(1985), 1-2 vom: Jan., Seite 63-68 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:24 year:1985 number:1-2 month:01 pages:63-68 https://doi.org/10.1007/BF02894818 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 AR 24 1985 1-2 01 63-68 |
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Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. © Indian Academy of Sciences 1985 |
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Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. © Indian Academy of Sciences 1985 |
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Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. The spurious motion of the centre of confinement is accounted for in these models in exactly the same manner. We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls. © Indian Academy of Sciences 1985 |
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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">OLC2076012672</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230402042346.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s1985 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02894818</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2076012672</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02894818-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">Khadkikar, S B</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Relativistic harmonic confinement of quarks and gluons</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1985</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">© Indian Academy of Sciences 1985</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract A current confinement model for glue-balls is proposed to maintain complete similarity with relativistic harmonic oscillator model (rhm) with Lorentz scalar and vector potentials for quarks. 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We shall review some of the successes of therhm in hardronic masses, magnetic moments of baryons, nucleonic sizes and polarisability and proton-antiproton annihilation, as well as the recent results on glue-balls.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Relativistic harmonic confinement</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">quarks</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">gluons</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">glue-balls</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">hadrons</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">masses</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">magnetic moments</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Pramāna</subfield><subfield code="d">Springer India, 1973</subfield><subfield code="g">24(1985), 1-2 vom: Jan., Seite 63-68</subfield><subfield code="w">(DE-627)129403342</subfield><subfield code="w">(DE-600)186949-8</subfield><subfield code="w">(DE-576)014785102</subfield><subfield code="x">0304-4289</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:24</subfield><subfield code="g">year:1985</subfield><subfield code="g">number:1-2</subfield><subfield code="g">month:01</subfield><subfield code="g">pages:63-68</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF02894818</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_179</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">24</subfield><subfield code="j">1985</subfield><subfield code="e">1-2</subfield><subfield code="c">01</subfield><subfield code="h">63-68</subfield></datafield></record></collection>
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