On kaonic hydrogen. Quantum field theoretic and relativistic covariant approach
Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The ampl...
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E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2004 |
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| Umfang: |
18 |
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| Reproduktion: |
Springer Online Journal Archives 1860-2002 |
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| Übergeordnetes Werk: |
in: The European physical journal - 1998, 21(2004) vom: Jan., Seite 11-28 |
| Übergeordnetes Werk: |
volume:21 ; year:2004 ; month:01 ; pages:11-28 ; extent:18 |
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| 245 | 1 | 0 | |a On kaonic hydrogen. Quantum field theoretic and relativistic covariant approach |
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| 520 | |a Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . | ||
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| 700 | 1 | |a Cargnelli, M. |4 oth | |
| 700 | 1 | |a Faber, M. |4 oth | |
| 700 | 1 | |a Marton, J. |4 oth | |
| 700 | 1 | |a Troitskaya, N. I. |4 oth | |
| 700 | 1 | |a Zmeskal, J. |4 oth | |
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(DE-627)NLEJ198926413 DE-627 ger DE-627 rakwb eng On kaonic hydrogen. Quantum field theoretic and relativistic covariant approach 2004 18 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . Springer Online Journal Archives 1860-2002 Ivanov, A. N. oth Cargnelli, M. oth Faber, M. oth Marton, J. oth Troitskaya, N. I. oth Zmeskal, J. oth in The European physical journal 1998 21(2004) vom: Jan., Seite 11-28 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:21 year:2004 month:01 pages:11-28 extent:18 http://dx.doi.org/10.1140/epja/i2003-10178-y GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 21 2004 1 11-28 18 |
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(DE-627)NLEJ198926413 DE-627 ger DE-627 rakwb eng On kaonic hydrogen. Quantum field theoretic and relativistic covariant approach 2004 18 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . Springer Online Journal Archives 1860-2002 Ivanov, A. N. oth Cargnelli, M. oth Faber, M. oth Marton, J. oth Troitskaya, N. I. oth Zmeskal, J. oth in The European physical journal 1998 21(2004) vom: Jan., Seite 11-28 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:21 year:2004 month:01 pages:11-28 extent:18 http://dx.doi.org/10.1140/epja/i2003-10178-y GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 21 2004 1 11-28 18 |
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(DE-627)NLEJ198926413 DE-627 ger DE-627 rakwb eng On kaonic hydrogen. Quantum field theoretic and relativistic covariant approach 2004 18 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . Springer Online Journal Archives 1860-2002 Ivanov, A. N. oth Cargnelli, M. oth Faber, M. oth Marton, J. oth Troitskaya, N. I. oth Zmeskal, J. oth in The European physical journal 1998 21(2004) vom: Jan., Seite 11-28 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:21 year:2004 month:01 pages:11-28 extent:18 http://dx.doi.org/10.1140/epja/i2003-10178-y GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 21 2004 1 11-28 18 |
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(DE-627)NLEJ198926413 DE-627 ger DE-627 rakwb eng On kaonic hydrogen. Quantum field theoretic and relativistic covariant approach 2004 18 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . Springer Online Journal Archives 1860-2002 Ivanov, A. N. oth Cargnelli, M. oth Faber, M. oth Marton, J. oth Troitskaya, N. I. oth Zmeskal, J. oth in The European physical journal 1998 21(2004) vom: Jan., Seite 11-28 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:21 year:2004 month:01 pages:11-28 extent:18 http://dx.doi.org/10.1140/epja/i2003-10178-y GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 21 2004 1 11-28 18 |
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(DE-627)NLEJ198926413 DE-627 ger DE-627 rakwb eng On kaonic hydrogen. Quantum field theoretic and relativistic covariant approach 2004 18 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . Springer Online Journal Archives 1860-2002 Ivanov, A. N. oth Cargnelli, M. oth Faber, M. oth Marton, J. oth Troitskaya, N. I. oth Zmeskal, J. oth in The European physical journal 1998 21(2004) vom: Jan., Seite 11-28 (DE-627)NLEJ188987754 (DE-600)1459066-9 1434-601X nnns volume:21 year:2004 month:01 pages:11-28 extent:18 http://dx.doi.org/10.1140/epja/i2003-10178-y GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 21 2004 1 11-28 18 |
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Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . |
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Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . |
| abstract_unstemmed |
Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ . |
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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">NLEJ198926413</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706011604.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070527s2004 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ198926413</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="245" ind1="1" ind2="0"><subfield code="a">On kaonic hydrogen. Quantum field theoretic and relativistic covariant approach</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2004</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">18</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">Abstract. We study kaonic hydrogen, the bound K - p state A K p . Within a quantum field theoretic and relativistic covariant approach we derive the energy level displacement of the ground state of kaonic hydrogen in terms of the amplitude of K - p scattering for arbitrary relative momenta. The amplitude of low-energy K - p scattering near threshold is defined by the contributions of three resonances $\Lambda(1405)$ , $\Lambda(1800)$ and $\Sigma^0(1750)$ and a smooth elastic background. The amplitudes of inelastic channels of low-energy K - p scattering fit experimental data on the near-threshold behaviour of the cross-sections and the experimental data by the DEAR Collaboration. We use the soft-pion technique (leading order in Chiral Perturbation Theory) for the calculation of the partial width of the radiative decay of pionic hydrogen $A_{\pi p} \to n + \gamma$ and the Panofsky ratio. The theoretical prediction for the Panofsky ratio agrees well with experimental data. We apply the soft-kaon technique (leading order in Chiral Perturbation Theory) to the calculation of the partial widths of radiative decays of kaonic hydrogen $A_{Kp} \to \Lambda^0 + \gamma$ and $A_{K p} \to \Sigma^0 + \gamma$ . We show that the contribution of these decays to the width of the energy level of the ground state of kaonic hydrogen is less than 1 $\%$ .</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Springer Online Journal Archives 1860-2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ivanov, A. N.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Cargnelli, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Faber, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Marton, J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Troitskaya, N. I.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zmeskal, J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">The European physical journal</subfield><subfield code="d">1998</subfield><subfield code="g">21(2004) vom: Jan., Seite 11-28</subfield><subfield code="w">(DE-627)NLEJ188987754</subfield><subfield code="w">(DE-600)1459066-9</subfield><subfield code="x">1434-601X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:21</subfield><subfield code="g">year:2004</subfield><subfield code="g">month:01</subfield><subfield code="g">pages:11-28</subfield><subfield code="g">extent:18</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://dx.doi.org/10.1140/epja/i2003-10178-y</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SOJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">21</subfield><subfield code="j">2004</subfield><subfield code="c">1</subfield><subfield code="h">11-28</subfield><subfield code="g">18</subfield></datafield></record></collection>
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