Is theS-meson a baryonium state?
Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \b...
Ausführliche Beschreibung
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| Autor*in: |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1979 |
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| Umfang: |
4 |
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| Reproduktion: |
Springer Online Journal Archives 1860-2002 |
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| Übergeordnetes Werk: |
in: The European physical journal - 1998, 2(1979) vom: Apr., Seite 351-354 |
| Übergeordnetes Werk: |
volume:2 ; year:1979 ; month:04 ; pages:351-354 ; extent:4 |
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| 520 | |a Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . | ||
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(DE-627)NLEJ206217218 DE-627 ger DE-627 rakwb eng Is theS-meson a baryonium state? 1979 4 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . Springer Online Journal Archives 1860-2002 Kluyver, J. C. oth in The European physical journal 1998 2(1979) vom: Apr., Seite 351-354 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:2 year:1979 month:04 pages:351-354 extent:4 http://dx.doi.org/10.1007/BF01545898 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 2 1979 4 351-354 4 |
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(DE-627)NLEJ206217218 DE-627 ger DE-627 rakwb eng Is theS-meson a baryonium state? 1979 4 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . Springer Online Journal Archives 1860-2002 Kluyver, J. C. oth in The European physical journal 1998 2(1979) vom: Apr., Seite 351-354 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:2 year:1979 month:04 pages:351-354 extent:4 http://dx.doi.org/10.1007/BF01545898 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 2 1979 4 351-354 4 |
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(DE-627)NLEJ206217218 DE-627 ger DE-627 rakwb eng Is theS-meson a baryonium state? 1979 4 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . Springer Online Journal Archives 1860-2002 Kluyver, J. C. oth in The European physical journal 1998 2(1979) vom: Apr., Seite 351-354 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:2 year:1979 month:04 pages:351-354 extent:4 http://dx.doi.org/10.1007/BF01545898 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 2 1979 4 351-354 4 |
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(DE-627)NLEJ206217218 DE-627 ger DE-627 rakwb eng Is theS-meson a baryonium state? 1979 4 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . Springer Online Journal Archives 1860-2002 Kluyver, J. C. oth in The European physical journal 1998 2(1979) vom: Apr., Seite 351-354 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:2 year:1979 month:04 pages:351-354 extent:4 http://dx.doi.org/10.1007/BF01545898 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 2 1979 4 351-354 4 |
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(DE-627)NLEJ206217218 DE-627 ger DE-627 rakwb eng Is theS-meson a baryonium state? 1979 4 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . Springer Online Journal Archives 1860-2002 Kluyver, J. C. oth in The European physical journal 1998 2(1979) vom: Apr., Seite 351-354 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:2 year:1979 month:04 pages:351-354 extent:4 http://dx.doi.org/10.1007/BF01545898 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 2 1979 4 351-354 4 |
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in The European physical journal 2(1979) vom: Apr., Seite 351-354 volume:2 year:1979 month:04 pages:351-354 extent:4 |
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Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . |
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Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . |
| abstract_unstemmed |
Abstract If theS-meson is assumed to be a baryonium state composed of an isospin one diquark and antidiquark, it will be produced in $$\bar pp$$ reactions as a mixture ofI=0 andI=1 baryonium states. The experimentally observed large ratio of the cross sections of the reactions $$\bar pp \to S \to \bar pp$$ and $$\bar pp \to S^0 \to \bar nn$$ is then explained on basis of quark additivity and conservation of isospin in thes-channel. The model predicts: $$\sigma (\bar pp \to S^0 \to \bar pp):\sigma (\bar pp \to S^0 \to \bar nn):\sigma (\bar pn \to S^ - \to \bar pn) = 25:1:16$$ . |
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