Damping of zero sound in $ liquid^{3} $He
Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Toepffer, C. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1989 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer-Verlag 1989 |
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| Übergeordnetes Werk: |
Enthalten in: Zeitschrift für Physik - Springer-Verlag, 1975, 74(1989), 4 vom: Dez., Seite 429-438 |
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| Übergeordnetes Werk: |
volume:74 ; year:1989 ; number:4 ; month:12 ; pages:429-438 |
| Links: |
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| DOI / URN: |
10.1007/BF01311390 |
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| Katalog-ID: |
OLC2072274249 |
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| 520 | |a Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. | ||
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10.1007/BF01311390 doi (DE-627)OLC2072274249 (DE-He213)BF01311390-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Toepffer, C. verfasserin aut Damping of zero sound in $ liquid^{3} $He 1989 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1989 Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. Neural Network Attenuation Integral Equation Structure Factor Momentum Transfer Hiltner, P. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1975 74(1989), 4 vom: Dez., Seite 429-438 (DE-627)129415383 (DE-600)189287-3 (DE-576)014793687 0340-224X nnns volume:74 year:1989 number:4 month:12 pages:429-438 https://doi.org/10.1007/BF01311390 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_47 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4318 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 33.00 VZ AR 74 1989 4 12 429-438 |
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10.1007/BF01311390 doi (DE-627)OLC2072274249 (DE-He213)BF01311390-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Toepffer, C. verfasserin aut Damping of zero sound in $ liquid^{3} $He 1989 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1989 Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. Neural Network Attenuation Integral Equation Structure Factor Momentum Transfer Hiltner, P. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1975 74(1989), 4 vom: Dez., Seite 429-438 (DE-627)129415383 (DE-600)189287-3 (DE-576)014793687 0340-224X nnns volume:74 year:1989 number:4 month:12 pages:429-438 https://doi.org/10.1007/BF01311390 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_47 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4318 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 33.00 VZ AR 74 1989 4 12 429-438 |
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10.1007/BF01311390 doi (DE-627)OLC2072274249 (DE-He213)BF01311390-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Toepffer, C. verfasserin aut Damping of zero sound in $ liquid^{3} $He 1989 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1989 Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. Neural Network Attenuation Integral Equation Structure Factor Momentum Transfer Hiltner, P. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1975 74(1989), 4 vom: Dez., Seite 429-438 (DE-627)129415383 (DE-600)189287-3 (DE-576)014793687 0340-224X nnns volume:74 year:1989 number:4 month:12 pages:429-438 https://doi.org/10.1007/BF01311390 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_47 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4318 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 33.00 VZ AR 74 1989 4 12 429-438 |
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10.1007/BF01311390 doi (DE-627)OLC2072274249 (DE-He213)BF01311390-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Toepffer, C. verfasserin aut Damping of zero sound in $ liquid^{3} $He 1989 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1989 Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. Neural Network Attenuation Integral Equation Structure Factor Momentum Transfer Hiltner, P. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1975 74(1989), 4 vom: Dez., Seite 429-438 (DE-627)129415383 (DE-600)189287-3 (DE-576)014793687 0340-224X nnns volume:74 year:1989 number:4 month:12 pages:429-438 https://doi.org/10.1007/BF01311390 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_47 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4318 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 33.00 VZ AR 74 1989 4 12 429-438 |
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10.1007/BF01311390 doi (DE-627)OLC2072274249 (DE-He213)BF01311390-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Toepffer, C. verfasserin aut Damping of zero sound in $ liquid^{3} $He 1989 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1989 Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. Neural Network Attenuation Integral Equation Structure Factor Momentum Transfer Hiltner, P. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1975 74(1989), 4 vom: Dez., Seite 429-438 (DE-627)129415383 (DE-600)189287-3 (DE-576)014793687 0340-224X nnns volume:74 year:1989 number:4 month:12 pages:429-438 https://doi.org/10.1007/BF01311390 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_47 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4318 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 33.00 VZ AR 74 1989 4 12 429-438 |
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530 VZ 33.00 bkl Damping of zero sound in $ liquid^{3} $He Neural Network Attenuation Integral Equation Structure Factor Momentum Transfer |
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damping of zero sound in $ liquid^{3} $he |
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Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. © Springer-Verlag 1989 |
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Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. © Springer-Verlag 1989 |
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Abstract The dynamic structure factor in $ liquid^{3} $He is calculated within the framework of Dissipative Linear Response (DLR) equations. The effective interaction is represented by the Landau parameters up tol=2 and the Random Phase Approximation (RPA)-scattering amplitudes are evaluated in thes−p−d approximation. The dissipative linear response operator is calculated on the basis of RPA solutions of undamped zero sound using integral equation techniques. The dynamical structure factor has a strong resonance structure whose width agrees with measurements of the attenuation coefficient for small momentum transfers. At larger values of momentum transfer, where the dynamical structure factor has been directly measured, the Landau parameters do not give more than a qualitative agreement with the data. © Springer-Verlag 1989 |
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