A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas
Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we fi...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Johansson, B. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1968 |
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| Schlagwörter: |
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| Anmerkung: |
© Socictà Italiana di Fisica 1968 |
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| Übergeordnetes Werk: |
Enthalten in: Il nuovo cimento - [S.l.] : Italian Physical Soc., 1965, 55(1968), 2 vom: 01. Juni, Seite 305-314 |
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| Übergeordnetes Werk: |
volume:55 ; year:1968 ; number:2 ; day:01 ; month:06 ; pages:305-314 |
| Links: |
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| DOI / URN: |
10.1007/BF02711644 |
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| Katalog-ID: |
SPR020653034 |
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| 008 | 201006s1968 xx |||||o 00| ||eng c | ||
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| 035 | |a (DE-627)SPR020653034 | ||
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| 041 | |a eng | ||
| 100 | 1 | |a Johansson, B. |e verfasserin |4 aut | |
| 245 | 1 | 2 | |a A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas |
| 264 | 1 | |c 1968 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a Computermedien |b c |2 rdamedia | ||
| 338 | |a Online-Ressource |b cr |2 rdacarrier | ||
| 500 | |a © Socictà Italiana di Fisica 1968 | ||
| 520 | |a Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. | ||
| 650 | 4 | |a Unstable Mode |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Collective Mode |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Internal Field |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Spin Density Wave |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Vertex Part |7 (dpeaa)DE-He213 | |
| 773 | 0 | 8 | |i Enthalten in |t Il nuovo cimento |d [S.l.] : Italian Physical Soc., 1965 |g 55(1968), 2 vom: 01. Juni, Seite 305-314 |w (DE-627)627248705 |w (DE-600)2556218-6 |x 1826-9877 |7 nnns |
| 773 | 1 | 8 | |g volume:55 |g year:1968 |g number:2 |g day:01 |g month:06 |g pages:305-314 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/BF02711644 |z lizenzpflichtig |3 Volltext |
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| 952 | |d 55 |j 1968 |e 2 |b 01 |c 06 |h 305-314 | ||
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1968 |
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1968 |
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10.1007/BF02711644 doi (DE-627)SPR020653034 (SPR)BF02711644-e DE-627 ger DE-627 rakwb eng Johansson, B. verfasserin aut A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas 1968 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Socictà Italiana di Fisica 1968 Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. Unstable Mode (dpeaa)DE-He213 Collective Mode (dpeaa)DE-He213 Internal Field (dpeaa)DE-He213 Spin Density Wave (dpeaa)DE-He213 Vertex Part (dpeaa)DE-He213 Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 55(1968), 2 vom: 01. Juni, Seite 305-314 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:55 year:1968 number:2 day:01 month:06 pages:305-314 https://dx.doi.org/10.1007/BF02711644 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_65 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 55 1968 2 01 06 305-314 |
| spelling |
10.1007/BF02711644 doi (DE-627)SPR020653034 (SPR)BF02711644-e DE-627 ger DE-627 rakwb eng Johansson, B. verfasserin aut A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas 1968 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Socictà Italiana di Fisica 1968 Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. Unstable Mode (dpeaa)DE-He213 Collective Mode (dpeaa)DE-He213 Internal Field (dpeaa)DE-He213 Spin Density Wave (dpeaa)DE-He213 Vertex Part (dpeaa)DE-He213 Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 55(1968), 2 vom: 01. Juni, Seite 305-314 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:55 year:1968 number:2 day:01 month:06 pages:305-314 https://dx.doi.org/10.1007/BF02711644 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_65 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 55 1968 2 01 06 305-314 |
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10.1007/BF02711644 doi (DE-627)SPR020653034 (SPR)BF02711644-e DE-627 ger DE-627 rakwb eng Johansson, B. verfasserin aut A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas 1968 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Socictà Italiana di Fisica 1968 Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. Unstable Mode (dpeaa)DE-He213 Collective Mode (dpeaa)DE-He213 Internal Field (dpeaa)DE-He213 Spin Density Wave (dpeaa)DE-He213 Vertex Part (dpeaa)DE-He213 Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 55(1968), 2 vom: 01. Juni, Seite 305-314 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:55 year:1968 number:2 day:01 month:06 pages:305-314 https://dx.doi.org/10.1007/BF02711644 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_65 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 55 1968 2 01 06 305-314 |
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10.1007/BF02711644 doi (DE-627)SPR020653034 (SPR)BF02711644-e DE-627 ger DE-627 rakwb eng Johansson, B. verfasserin aut A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas 1968 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Socictà Italiana di Fisica 1968 Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. Unstable Mode (dpeaa)DE-He213 Collective Mode (dpeaa)DE-He213 Internal Field (dpeaa)DE-He213 Spin Density Wave (dpeaa)DE-He213 Vertex Part (dpeaa)DE-He213 Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 55(1968), 2 vom: 01. Juni, Seite 305-314 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:55 year:1968 number:2 day:01 month:06 pages:305-314 https://dx.doi.org/10.1007/BF02711644 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_65 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 55 1968 2 01 06 305-314 |
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10.1007/BF02711644 doi (DE-627)SPR020653034 (SPR)BF02711644-e DE-627 ger DE-627 rakwb eng Johansson, B. verfasserin aut A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas 1968 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Socictà Italiana di Fisica 1968 Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. Unstable Mode (dpeaa)DE-He213 Collective Mode (dpeaa)DE-He213 Internal Field (dpeaa)DE-He213 Spin Density Wave (dpeaa)DE-He213 Vertex Part (dpeaa)DE-He213 Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 55(1968), 2 vom: 01. Juni, Seite 305-314 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:55 year:1968 number:2 day:01 month:06 pages:305-314 https://dx.doi.org/10.1007/BF02711644 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_65 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 55 1968 2 01 06 305-314 |
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Enthalten in Il nuovo cimento 55(1968), 2 vom: 01. Juni, Seite 305-314 volume:55 year:1968 number:2 day:01 month:06 pages:305-314 |
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Enthalten in Il nuovo cimento 55(1968), 2 vom: 01. Juni, Seite 305-314 volume:55 year:1968 number:2 day:01 month:06 pages:305-314 |
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| author |
Johansson, B. |
| spellingShingle |
Johansson, B. misc Unstable Mode misc Collective Mode misc Internal Field misc Spin Density Wave misc Vertex Part A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas |
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A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas Unstable Mode (dpeaa)DE-He213 Collective Mode (dpeaa)DE-He213 Internal Field (dpeaa)DE-He213 Spin Density Wave (dpeaa)DE-He213 Vertex Part (dpeaa)DE-He213 |
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A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas |
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| title_full |
A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas |
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Johansson, B. |
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Il nuovo cimento |
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Il nuovo cimento |
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10.1007/BF02711644 |
| title_sort |
possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas |
| title_auth |
A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas |
| abstract |
Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. © Socictà Italiana di Fisica 1968 |
| abstractGer |
Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. © Socictà Italiana di Fisica 1968 |
| abstract_unstemmed |
Summary When arriving at the transition point from the normal state,one collective excitation above the ground state will get unstable, thereby signalling the onset of a new phase of the system. However, when studying the collective modes around thenormal state even beyond the transition point we find that a whole series of different collective modes (all of the same character) is unstable. From this set of modes we seek the «most unstable one», which we then argue could provide some information on the character of the new state. These ideas are applied to the case of a one-dimensional Fermi gas with repulsive δ-function interactions between the particles. © Socictà Italiana di Fisica 1968 |
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A possible generalized instability criterium applied to the one-dimensional δ-function interacting fermi gas |
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https://dx.doi.org/10.1007/BF02711644 |
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10.1007/BF02711644 |
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2024-07-03T17:24:44.776Z |
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| score |
7.4028063 |