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] Elster, Ch. [verfasserIn] Polyzou, W. N. [verfasserIn] |
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| Format: |
E-Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2012 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Few-body systems - Wien [u.a.] : Springer, 1986, 54(2012), 12 vom: 09. Aug., Seite 2207-2225 |
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| 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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| Katalog-ID: |
SPR007052677 |
|---|
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| 084 | |a 31.00 |2 bkl | ||
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| 100 | 1 | |a Veerasamy, S. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction |
| 264 | 1 | |c 2012 | |
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| 337 | |a Computermedien |b c |2 rdamedia | ||
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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. | ||
| 650 | 4 | |a Partial Wave |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Time Reversal |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Quadrature Point |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Transition Matrix Element |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Wolfenstein Parameter |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Elster, Ch. |e verfasserin |4 aut | |
| 700 | 1 | |a Polyzou, W. N. |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Few-body systems |d Wien [u.a.] : Springer, 1986 |g 54(2012), 12 vom: 09. Aug., Seite 2207-2225 |w (DE-627)25372323X |w (DE-600)1459107-8 |x 1432-5411 |7 nnns |
| 773 | 1 | 8 | |g volume:54 |g year:2012 |g number:12 |g day:09 |g month:08 |g pages:2207-2225 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s00601-012-0476-1 |z lizenzpflichtig |3 Volltext |
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| 952 | |d 54 |j 2012 |e 12 |b 09 |c 08 |h 2207-2225 | ||
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2012 |
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31.00 33.00 |
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| allfields |
10.1007/s00601-012-0476-1 doi (DE-627)SPR007052677 (SPR)s00601-012-0476-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 (dpeaa)DE-He213 Time Reversal (dpeaa)DE-He213 Quadrature Point (dpeaa)DE-He213 Transition Matrix Element (dpeaa)DE-He213 Wolfenstein Parameter (dpeaa)DE-He213 Elster, Ch. verfasserin aut Polyzou, W. N. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://dx.doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 54 2012 12 09 08 2207-2225 |
| spelling |
10.1007/s00601-012-0476-1 doi (DE-627)SPR007052677 (SPR)s00601-012-0476-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 (dpeaa)DE-He213 Time Reversal (dpeaa)DE-He213 Quadrature Point (dpeaa)DE-He213 Transition Matrix Element (dpeaa)DE-He213 Wolfenstein Parameter (dpeaa)DE-He213 Elster, Ch. verfasserin aut Polyzou, W. N. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://dx.doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 54 2012 12 09 08 2207-2225 |
| allfields_unstemmed |
10.1007/s00601-012-0476-1 doi (DE-627)SPR007052677 (SPR)s00601-012-0476-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 (dpeaa)DE-He213 Time Reversal (dpeaa)DE-He213 Quadrature Point (dpeaa)DE-He213 Transition Matrix Element (dpeaa)DE-He213 Wolfenstein Parameter (dpeaa)DE-He213 Elster, Ch. verfasserin aut Polyzou, W. N. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://dx.doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 54 2012 12 09 08 2207-2225 |
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10.1007/s00601-012-0476-1 doi (DE-627)SPR007052677 (SPR)s00601-012-0476-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 (dpeaa)DE-He213 Time Reversal (dpeaa)DE-He213 Quadrature Point (dpeaa)DE-He213 Transition Matrix Element (dpeaa)DE-He213 Wolfenstein Parameter (dpeaa)DE-He213 Elster, Ch. verfasserin aut Polyzou, W. N. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://dx.doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 54 2012 12 09 08 2207-2225 |
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10.1007/s00601-012-0476-1 doi (DE-627)SPR007052677 (SPR)s00601-012-0476-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Veerasamy, S. verfasserin aut Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 (dpeaa)DE-He213 Time Reversal (dpeaa)DE-He213 Quadrature Point (dpeaa)DE-He213 Transition Matrix Element (dpeaa)DE-He213 Wolfenstein Parameter (dpeaa)DE-He213 Elster, Ch. verfasserin aut Polyzou, W. N. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 54(2012), 12 vom: 09. Aug., Seite 2207-2225 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 https://dx.doi.org/10.1007/s00601-012-0476-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4320 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 54 2012 12 09 08 2207-2225 |
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Enthalten in Few-body systems 54(2012), 12 vom: 09. Aug., Seite 2207-2225 volume:54 year:2012 number:12 day:09 month:08 pages:2207-2225 |
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Partial Wave Time Reversal Quadrature Point Transition Matrix Element Wolfenstein Parameter |
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Few-body systems |
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Veerasamy, S. @@aut@@ Elster, Ch. @@aut@@ Polyzou, W. N. @@aut@@ |
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| author |
Veerasamy, S. |
| spellingShingle |
Veerasamy, S. ddc 530 bkl 31.00 bkl 33.00 misc Partial Wave misc Time Reversal misc Quadrature Point misc Transition Matrix Element misc Wolfenstein Parameter Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction |
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Veerasamy, S. |
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530 - Physics |
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1432-5411 |
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530 ASE 31.00 bkl 33.00 bkl Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction Partial Wave (dpeaa)DE-He213 Time Reversal (dpeaa)DE-He213 Quadrature Point (dpeaa)DE-He213 Transition Matrix Element (dpeaa)DE-He213 Wolfenstein Parameter (dpeaa)DE-He213 |
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ddc 530 bkl 31.00 bkl 33.00 misc Partial Wave misc Time Reversal misc Quadrature Point misc Transition Matrix Element misc Wolfenstein Parameter |
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ddc 530 bkl 31.00 bkl 33.00 misc Partial Wave misc Time Reversal misc Quadrature Point misc Transition Matrix Element misc Wolfenstein Parameter |
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ddc 530 bkl 31.00 bkl 33.00 misc Partial Wave misc Time Reversal misc Quadrature Point misc Transition Matrix Element misc Wolfenstein Parameter |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Few-body systems |
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Few-body systems |
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Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction |
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(DE-627)SPR007052677 (SPR)s00601-012-0476-1-e |
| title_full |
Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction |
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Veerasamy, S. |
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Few-body systems |
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Few-body systems |
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eng |
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2012 |
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2207 |
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Veerasamy, S. Elster, Ch. Polyzou, W. N. |
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54 |
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530 ASE 31.00 bkl 33.00 bkl |
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Elektronische Aufsätze |
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Veerasamy, S. |
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10.1007/s00601-012-0476-1 |
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530 |
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verfasserin |
| title_sort |
two-nucleon scattering without partial waves using a momentum space argonne v18 interaction |
| title_auth |
Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction |
| abstract |
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. |
| abstractGer |
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. |
| abstract_unstemmed |
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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12 |
| title_short |
Two-Nucleon Scattering Without Partial Waves Using a Momentum Space Argonne V18 Interaction |
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https://dx.doi.org/10.1007/s00601-012-0476-1 |
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Elster, Ch Polyzou, W. N. |
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Elster, Ch Polyzou, W. N. |
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| doi_str |
10.1007/s00601-012-0476-1 |
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2024-07-04T01:52:22.506Z |
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| score |
7.3996515 |