Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction
Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Veerasamy, S. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2012 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer-Verlag 2012 |
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| Übergeordnetes Werk: |
Enthalten in: Few body systems - Springer Vienna, 1986, 54(2012), 12 vom: 09. Aug., Seite 2207-2225 |
|---|---|
| Übergeordnetes Werk: |
volume:54 ; year:2012 ; number:12 ; day:09 ; month:08 ; pages:2207-2225 |
| Links: |
|---|
| DOI / URN: |
10.1007/s00601-012-0476-1 |
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OLC207177258X |
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| 520 | |a Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. The choice of on and off-shell spin-momentum basis elements is made so that the coefficients of the on-shell spin-momentum basis vectors are simply related to the corresponding off-shell coefficients. | ||
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10.1007/s00601-012-0476-1 doi (DE-627)OLC207177258X (DE-He213)s00601-012-0476-1-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2012 Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. The choice of on and off-shell spin-momentum basis elements is made so that the coefficients of the on-shell spin-momentum basis vectors are simply related to the corresponding off-shell coefficients. Partial Wave Time Reversal Quadrature Point Transition Matrix Element Wolfenstein Parameter Elster, Ch. aut Polyzou, W. N. aut Enthalten in Few body systems Springer Vienna, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)129862819 (DE-600)283895-3 (DE-576)015175154 0177-7963 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 33.00 VZ AR 54 2012 12 09 08 2207-2225 |
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10.1007/s00601-012-0476-1 doi (DE-627)OLC207177258X (DE-He213)s00601-012-0476-1-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2012 Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. The choice of on and off-shell spin-momentum basis elements is made so that the coefficients of the on-shell spin-momentum basis vectors are simply related to the corresponding off-shell coefficients. Partial Wave Time Reversal Quadrature Point Transition Matrix Element Wolfenstein Parameter Elster, Ch. aut Polyzou, W. N. aut Enthalten in Few body systems Springer Vienna, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)129862819 (DE-600)283895-3 (DE-576)015175154 0177-7963 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 33.00 VZ AR 54 2012 12 09 08 2207-2225 |
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10.1007/s00601-012-0476-1 doi (DE-627)OLC207177258X (DE-He213)s00601-012-0476-1-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2012 Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. The choice of on and off-shell spin-momentum basis elements is made so that the coefficients of the on-shell spin-momentum basis vectors are simply related to the corresponding off-shell coefficients. Partial Wave Time Reversal Quadrature Point Transition Matrix Element Wolfenstein Parameter Elster, Ch. aut Polyzou, W. N. aut Enthalten in Few body systems Springer Vienna, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)129862819 (DE-600)283895-3 (DE-576)015175154 0177-7963 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 33.00 VZ AR 54 2012 12 09 08 2207-2225 |
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10.1007/s00601-012-0476-1 doi (DE-627)OLC207177258X (DE-He213)s00601-012-0476-1-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2012 Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. The choice of on and off-shell spin-momentum basis elements is made so that the coefficients of the on-shell spin-momentum basis vectors are simply related to the corresponding off-shell coefficients. Partial Wave Time Reversal Quadrature Point Transition Matrix Element Wolfenstein Parameter Elster, Ch. aut Polyzou, W. N. aut Enthalten in Few body systems Springer Vienna, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)129862819 (DE-600)283895-3 (DE-576)015175154 0177-7963 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 33.00 VZ AR 54 2012 12 09 08 2207-2225 |
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Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. The choice of on and off-shell spin-momentum basis elements is made so that the coefficients of the on-shell spin-momentum basis vectors are simply related to the corresponding off-shell coefficients. © Springer-Verlag 2012 |
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Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. The choice of on and off-shell spin-momentum basis elements is made so that the coefficients of the on-shell spin-momentum basis vectors are simply related to the corresponding off-shell coefficients. © Springer-Verlag 2012 |
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Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. The choice of on and off-shell spin-momentum basis elements is made so that the coefficients of the on-shell spin-momentum basis vectors are simply related to the corresponding off-shell coefficients. © Springer-Verlag 2012 |
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10.1007/s00601-012-0476-1 |
| up_date |
2024-07-04T04:11:56.674Z |
| _version_ |
1803620258075901952 |
| fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC207177258X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230502125614.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s2012 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s00601-012-0476-1</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC207177258X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s00601-012-0476-1-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="084" ind1=" " ind2=" "><subfield code="a">33.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Veerasamy, S.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2012</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">© Springer-Verlag 2012</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract We test the operator form of the Fourier transform of the Argonne V18 potential by computing selected scattering observables and all Wolfenstein parameters for a variety of energies. These are compared to the GW-DAC database and to partial wave calculations. We represent the interaction and transition operators as expansions in a spin-momentum basis. In this representation the Lippmann–Schwinger equation becomes a six channel integral equation in two variables. Our calculations use different numbers of spin-momentum basis elements to represent the on- and off-shell transition operators. This is because different numbers of independent spin-momentum basis elements are required to expand the on- and off-shell transition operators. 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N.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Few body systems</subfield><subfield code="d">Springer Vienna, 1986</subfield><subfield code="g">54(2012), 12 vom: 09. 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7.399436 |