Rapidly rotating fermions in an anisotropic trap

Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$,...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Ghazanfari, N. [verfasserIn] Oktel, M. Ö. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2010

Schlagwörter:	Rotation Frequency Local Density Approximation Landau Level Lower Landau Level Step Structure

Übergeordnetes Werk:	Enthalten in: The European physical journal - Berlin : Springer, 1998, 59(2010), 3 vom: 26. Juni, Seite 435-441
Übergeordnetes Werk:	volume:59 ; year:2010 ; number:3 ; day:26 ; month:06 ; pages:435-441

Links:	Volltext

DOI / URN:	10.1140/epjd/e2010-00171-y

Katalog-ID:	SPR008405921

Internformat


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520			\|a Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations.
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650		4	\|a Lower Landau Level \|7 (dpeaa)DE-He213
650		4	\|a Step Structure \|7 (dpeaa)DE-He213
700	1		\|a Oktel, M. Ö. \|e verfasserin \|4 aut
773	0	8	\|i Enthalten in \|t The European physical journal \|d Berlin : Springer, 1998 \|g 59(2010), 3 vom: 26. Juni, Seite 435-441 \|w (DE-627)253722950 \|w (DE-600)1459071-2 \|x 1434-6079 \|7 nnns
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856	4	0	\|u https://dx.doi.org/10.1140/epjd/e2010-00171-y \|z lizenzpflichtig \|3 Volltext
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912			\|a GBV_ILN_63
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_206
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_267
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
912			\|a GBV_ILN_2111
912			\|a GBV_ILN_2112
912			\|a GBV_ILN_2113
912			\|a GBV_ILN_2116
912			\|a GBV_ILN_2118
912			\|a GBV_ILN_2119
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912			\|a GBV_ILN_2152
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912			\|a GBV_ILN_4306
912			\|a GBV_ILN_4307
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
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936	b	k	\|a 33.30 \|q ASE
936	b	k	\|a 33.38 \|q ASE
936	b	k	\|a 33.80 \|q ASE
951			\|a AR
952			\|d 59 \|j 2010 \|e 3 \|b 26 \|c 06 \|h 435-441

Indexfelder

author_variant	n g ng m ö o mö möo
matchkey_str	article:14346079:2010----::ailrttnfriniaai
hierarchy_sort_str	2010
bklnumber	33.30 33.38 33.80
publishDate	2010
allfields	10.1140/epjd/e2010-00171-y doi (DE-627)SPR008405921 (SPR)e2010-00171-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Ghazanfari, N. verfasserin aut Rapidly rotating fermions in an anisotropic trap 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations. Rotation Frequency (dpeaa)DE-He213 Local Density Approximation (dpeaa)DE-He213 Landau Level (dpeaa)DE-He213 Lower Landau Level (dpeaa)DE-He213 Step Structure (dpeaa)DE-He213 Oktel, M. Ö. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 59(2010), 3 vom: 26. Juni, Seite 435-441 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:59 year:2010 number:3 day:26 month:06 pages:435-441 https://dx.doi.org/10.1140/epjd/e2010-00171-y 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_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_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_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_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 59 2010 3 26 06 435-441
spelling	10.1140/epjd/e2010-00171-y doi (DE-627)SPR008405921 (SPR)e2010-00171-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Ghazanfari, N. verfasserin aut Rapidly rotating fermions in an anisotropic trap 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations. Rotation Frequency (dpeaa)DE-He213 Local Density Approximation (dpeaa)DE-He213 Landau Level (dpeaa)DE-He213 Lower Landau Level (dpeaa)DE-He213 Step Structure (dpeaa)DE-He213 Oktel, M. Ö. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 59(2010), 3 vom: 26. Juni, Seite 435-441 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:59 year:2010 number:3 day:26 month:06 pages:435-441 https://dx.doi.org/10.1140/epjd/e2010-00171-y 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_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_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_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_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 59 2010 3 26 06 435-441
allfields_unstemmed	10.1140/epjd/e2010-00171-y doi (DE-627)SPR008405921 (SPR)e2010-00171-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Ghazanfari, N. verfasserin aut Rapidly rotating fermions in an anisotropic trap 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations. Rotation Frequency (dpeaa)DE-He213 Local Density Approximation (dpeaa)DE-He213 Landau Level (dpeaa)DE-He213 Lower Landau Level (dpeaa)DE-He213 Step Structure (dpeaa)DE-He213 Oktel, M. Ö. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 59(2010), 3 vom: 26. Juni, Seite 435-441 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:59 year:2010 number:3 day:26 month:06 pages:435-441 https://dx.doi.org/10.1140/epjd/e2010-00171-y 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_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_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_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_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 59 2010 3 26 06 435-441
allfieldsGer	10.1140/epjd/e2010-00171-y doi (DE-627)SPR008405921 (SPR)e2010-00171-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Ghazanfari, N. verfasserin aut Rapidly rotating fermions in an anisotropic trap 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations. Rotation Frequency (dpeaa)DE-He213 Local Density Approximation (dpeaa)DE-He213 Landau Level (dpeaa)DE-He213 Lower Landau Level (dpeaa)DE-He213 Step Structure (dpeaa)DE-He213 Oktel, M. Ö. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 59(2010), 3 vom: 26. Juni, Seite 435-441 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:59 year:2010 number:3 day:26 month:06 pages:435-441 https://dx.doi.org/10.1140/epjd/e2010-00171-y 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_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_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_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_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 59 2010 3 26 06 435-441
allfieldsSound	10.1140/epjd/e2010-00171-y doi (DE-627)SPR008405921 (SPR)e2010-00171-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Ghazanfari, N. verfasserin aut Rapidly rotating fermions in an anisotropic trap 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations. Rotation Frequency (dpeaa)DE-He213 Local Density Approximation (dpeaa)DE-He213 Landau Level (dpeaa)DE-He213 Lower Landau Level (dpeaa)DE-He213 Step Structure (dpeaa)DE-He213 Oktel, M. Ö. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 59(2010), 3 vom: 26. Juni, Seite 435-441 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:59 year:2010 number:3 day:26 month:06 pages:435-441 https://dx.doi.org/10.1140/epjd/e2010-00171-y 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_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_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_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_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 59 2010 3 26 06 435-441
language	English
source	Enthalten in The European physical journal 59(2010), 3 vom: 26. Juni, Seite 435-441 volume:59 year:2010 number:3 day:26 month:06 pages:435-441
sourceStr	Enthalten in The European physical journal 59(2010), 3 vom: 26. Juni, Seite 435-441 volume:59 year:2010 number:3 day:26 month:06 pages:435-441
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Rotation Frequency Local Density Approximation Landau Level Lower Landau Level Step Structure
dewey-raw	530
isfreeaccess_bool	false
container_title	The European physical journal
authorswithroles_txt_mv	Ghazanfari, N. @@aut@@ Oktel, M. Ö. @@aut@@
publishDateDaySort_date	2010-06-26T00:00:00Z
hierarchy_top_id	253722950
dewey-sort	3530
id	SPR008405921
language_de	englisch
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We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. 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author	Ghazanfari, N.
spellingShingle	Ghazanfari, N. ddc 530 bkl 33.30 bkl 33.38 bkl 33.80 misc Rotation Frequency misc Local Density Approximation misc Landau Level misc Lower Landau Level misc Step Structure Rapidly rotating fermions in an anisotropic trap
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topic_title	530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Rapidly rotating fermions in an anisotropic trap Rotation Frequency (dpeaa)DE-He213 Local Density Approximation (dpeaa)DE-He213 Landau Level (dpeaa)DE-He213 Lower Landau Level (dpeaa)DE-He213 Step Structure (dpeaa)DE-He213
topic	ddc 530 bkl 33.30 bkl 33.38 bkl 33.80 misc Rotation Frequency misc Local Density Approximation misc Landau Level misc Lower Landau Level misc Step Structure
topic_unstemmed	ddc 530 bkl 33.30 bkl 33.38 bkl 33.80 misc Rotation Frequency misc Local Density Approximation misc Landau Level misc Lower Landau Level misc Step Structure
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title	Rapidly rotating fermions in an anisotropic trap
ctrlnum	(DE-627)SPR008405921 (SPR)e2010-00171-y-e
title_full	Rapidly rotating fermions in an anisotropic trap
author_sort	Ghazanfari, N.
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title_sort	rapidly rotating fermions in an anisotropic trap
title_auth	Rapidly rotating fermions in an anisotropic trap
abstract	Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations.
abstractGer	Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations.
abstract_unstemmed	Abstract. We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. The crossoverbetween the two regimes is smooth where the step structure betweenthe Landau level edges turn into Friedel oscillations.
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container_issue	3
title_short	Rapidly rotating fermions in an anisotropic trap
url	https://dx.doi.org/10.1140/epjd/e2010-00171-y
remote_bool	true
author2	Oktel, M. Ö.
author2Str	Oktel, M. Ö.
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isOA_txt	false
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doi_str	10.1140/epjd/e2010-00171-y
up_date	2024-07-03T20:48:51.827Z
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We consider a cold gas of non-interacting fermions in atwo-dimensional harmonic trap with two different trappingfrequencies $\omega_x$≤$\omega_y$, and discuss the effect ofrotation on the density profile. Depending on the rotation frequencyΩ, and the trap anisotropy $\omega_y$/$\omega_x$, the densityprofile assumes two qualitatively different shapes. For smallanisotropy, the density consists of elliptical plateaus of constantdensity, corresponding to Landau levels and is well described by atwo-dimensional local density approximation. For large anisotropy,the density profile is Gaussian in the strong confining directionand semicircular with prominent Friedel oscillations in the weakdirection. In this regime, a one-dimensional local densityapproximation is well suited to describe the system. 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Rapidly rotating fermions in an anisotropic trap

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