The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c.
Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the expon...
Ausführliche Beschreibung
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Englisch |
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1970 |
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Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
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Übergeordnetes Werk: |
in: Physics Letters B - Amsterdam : Elsevier, 33(1970), 6, Seite 438-440 |
Übergeordnetes Werk: |
volume:33 ; year:1970 ; number:6 ; pages:438-440 |
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NLEJ181184729 |
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245 | 1 | 4 | |a The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. |
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520 | |a Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. | ||
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700 | 1 | |a Bellm, T.H.J. |4 oth | |
700 | 1 | |a De Jonge, H. |4 oth | |
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(DE-627)NLEJ181184729 (DE-599)GBVNLZ181184729 DE-627 ger DE-627 rakwb eng The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. 1970 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Bellm, T.H.J. oth De Jonge, H. oth De Lijser, E. oth Manuel, P. oth Meyer, R.W. oth Tenner, A.G. oth Vons, P. oth Voorthuis, H. oth Heinen, P. oth Tiecke, H.G.J.M. oth Van de Walle, R.T. oth Winzeler, H. oth in Physics Letters B Amsterdam : Elsevier 33(1970), 6, Seite 438-440 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:33 year:1970 number:6 pages:438-440 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(70)90625-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 33 1970 6 438-440 |
spelling |
(DE-627)NLEJ181184729 (DE-599)GBVNLZ181184729 DE-627 ger DE-627 rakwb eng The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. 1970 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Bellm, T.H.J. oth De Jonge, H. oth De Lijser, E. oth Manuel, P. oth Meyer, R.W. oth Tenner, A.G. oth Vons, P. oth Voorthuis, H. oth Heinen, P. oth Tiecke, H.G.J.M. oth Van de Walle, R.T. oth Winzeler, H. oth in Physics Letters B Amsterdam : Elsevier 33(1970), 6, Seite 438-440 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:33 year:1970 number:6 pages:438-440 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(70)90625-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 33 1970 6 438-440 |
allfields_unstemmed |
(DE-627)NLEJ181184729 (DE-599)GBVNLZ181184729 DE-627 ger DE-627 rakwb eng The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. 1970 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Bellm, T.H.J. oth De Jonge, H. oth De Lijser, E. oth Manuel, P. oth Meyer, R.W. oth Tenner, A.G. oth Vons, P. oth Voorthuis, H. oth Heinen, P. oth Tiecke, H.G.J.M. oth Van de Walle, R.T. oth Winzeler, H. oth in Physics Letters B Amsterdam : Elsevier 33(1970), 6, Seite 438-440 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:33 year:1970 number:6 pages:438-440 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(70)90625-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 33 1970 6 438-440 |
allfieldsGer |
(DE-627)NLEJ181184729 (DE-599)GBVNLZ181184729 DE-627 ger DE-627 rakwb eng The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. 1970 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Bellm, T.H.J. oth De Jonge, H. oth De Lijser, E. oth Manuel, P. oth Meyer, R.W. oth Tenner, A.G. oth Vons, P. oth Voorthuis, H. oth Heinen, P. oth Tiecke, H.G.J.M. oth Van de Walle, R.T. oth Winzeler, H. oth in Physics Letters B Amsterdam : Elsevier 33(1970), 6, Seite 438-440 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:33 year:1970 number:6 pages:438-440 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(70)90625-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 33 1970 6 438-440 |
allfieldsSound |
(DE-627)NLEJ181184729 (DE-599)GBVNLZ181184729 DE-627 ger DE-627 rakwb eng The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. 1970 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Bellm, T.H.J. oth De Jonge, H. oth De Lijser, E. oth Manuel, P. oth Meyer, R.W. oth Tenner, A.G. oth Vons, P. oth Voorthuis, H. oth Heinen, P. oth Tiecke, H.G.J.M. oth Van de Walle, R.T. oth Winzeler, H. oth in Physics Letters B Amsterdam : Elsevier 33(1970), 6, Seite 438-440 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:33 year:1970 number:6 pages:438-440 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(70)90625-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 33 1970 6 438-440 |
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The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. |
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The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. |
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The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. |
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The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. |
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real part of the elastic scattering amplitude in the coulomb interference region of 4.2 gev/c k^- mesons on protons and a comparison with k^+p scattering at 5 gev/c. |
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The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. |
abstract |
Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. |
abstractGer |
Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. |
abstract_unstemmed |
Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb. |
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The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c. |
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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">NLEJ181184729</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706144944.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1970 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ181184729</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ181184729</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="4"><subfield code="a">The real part of the elastic scattering amplitude in the Coulomb interference region of 4.2 GeV/c K^- mesons on protons and a comparison with K^+p scattering at 5 GeV/c.</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1970</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">Using the same method as applied before to 5 GeV/c K^+p scattering we analyzed 4.2 GeV/c K^-p elastic scattering down to t values of 0.01 (GeV/c)^2. About 5500 events yielded the following results: the ratio of real to imaginary part of the nuclear amplitude α = 0.20 +/- 0.07, the slope of the exponential A = 8.6 +/- 0.2 (GeV/c)^-^2, the total elastic nuclear cross-section σ"e"l = 4.3 +/- 0.1 mb and the total cross-section σ"T = 25.0 +/- 0.7 mb.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Elsevier Journal Backfiles on ScienceDirect 1907 - 2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Bellm, T.H.J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">De Jonge, H.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">De Lijser, E.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Manuel, P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Meyer, R.W.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Tenner, A.G.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Vons, P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Voorthuis, H.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Heinen, P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Tiecke, H.G.J.M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Van de Walle, R.T.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Winzeler, H.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Physics Letters B</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">33(1970), 6, Seite 438-440</subfield><subfield code="w">(DE-627)NLEJ177212217</subfield><subfield code="w">(DE-600)1466612-1</subfield><subfield code="x">0370-2693</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:33</subfield><subfield code="g">year:1970</subfield><subfield code="g">number:6</subfield><subfield code="g">pages:438-440</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0370-2693(70)90625-8</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_H</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SDJ</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">33</subfield><subfield code="j">1970</subfield><subfield code="e">6</subfield><subfield code="h">438-440</subfield></datafield></record></collection>
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