novel probes for fermionic gases
DESCRIPTION
Novel Probes for Fermionic Gases. J. Meineke, T. Müller, B. Zimmermann, D. Stadler J.-P. Brantut, H. Moritz, T. Esslinger ETH Zürich. Experimental setup. Microscope objectives. 6 Li atoms. Microscope setup. Microscope setup. High-resolution imaging system: - PowerPoint PPT PresentationTRANSCRIPT
Novel Probes for Fermionic GasesNovel Probes for Fermionic Gases
J. Meineke, T. Müller, B. Zimmermann, D. Stadler
J.-P. Brantut, H. Moritz, T. Esslinger
ETH Zürich
J. Meineke, T. Müller, B. Zimmermann, D. Stadler
J.-P. Brantut, H. Moritz, T. Esslinger
ETH Zürich
Experimental setup
6Li atomsMicroscopeobjectives
Microscope setup
Microscope setup
High-resolution imaging system:
• resolution: 660nm (FWHM) for =671nm
• NA = 0.53, magnification factor: 54
Microscopic manipulation
flexible micro-tweezers
Atoms in micro-traps
a=2.5 m 6.9 m
Square lattice Ring lattice
B. Zimmermann, T. Müller, J. Meineke, T. Esslinger, H. Moritz, New Journal of Physics 13, 043007 (2011)
Imaging through the microscope
500m
“standard” imaging
20μm
high resolution imaging
Information on• correlations, quantum statistics?• temperature, susceptibilities?• entanglement?
Microscopic probing …
… of in-situ density fluctuations
Quantum statistics and fluctuations
Suppressed density fluctuations in a degenerate Fermi gasdue to Pauli principle!
...
2
11
3
23 V
N NN 2
thermal higher order quantum correction
thermal quantum degenerate
probe volume
For 1D Bose gases: J. Esteve et al., PRL 96,130403 (2006) & J. Armijo et al., PRL 105, 230402 (2010)For 2D Bose gases: C.-L. Hung, X. Zhang, Na. Gemelke, C. Chin, Nature 470, 236 (2011)
Measurement of density fluctuations
• Account for photon shot noise and imaging effects
• Calculate mean and variance over many realizations
different realizations absorption imaging
Fluctuation in gas on a pixel
Effect of imaging resolution
Manifestation of antibunching
Our work at ETH Zürich:PRL 105, 040401 (2010)
Indication for the level oflocal quantum degeneracy
Similar work at MIT in TOF:PRL 105, 040402 (2010)
Thermodynamic properties
Fluctuation-dissipation theorem:2N
NTkB
densityfluctuations
model independent measurement of temperature
Compressibility κ
local density approximation
1)(
rr
rN
Q. Zhou and T. L. Ho, arXiv: 0908.3015, to appear in PRL; κ in SF-MI: N. Gemelke, X. Zhang, C.-L. Hung, C. Chin, Nature 460, 995 (2009).
20
0
NN
UU
TkB
Fluctuation-based thermometry
Temperature: Conventional Fluctuation-based
degenerate 20530 nK 14531 nK
thermal 1,6 0.2 K 1,1 0.06 K
N
UU
TkN B
00
2
T. Müller , B. Zimmermann, J. Meineke, J.-P. Brantut, T. Esslinger, H. Moritz, Phys. Rev. Lett. 105, 040401 (2010)
Local Spin-FluctuationsLocal Spin-Fluctuations
hm2i = h(n1 ¡ n2)2i = hn21i +hn2
2i ¡ 2hn1n2i
hn1n2i = hª y"ª "ª
y#ª #i
Two-component quantum gas
Atom-Light InterfaceAtom-Light Interface
Hammerer et al., Rev. Mod. Phys. 82, 1041 (2010)
X̂ out = X̂ in + ·p2M̂z
Light
Atoms
Atom-Light InterfaceAtom-Light Interface
Bruun et al., PRL 102, 030401 (2009)
hX̂ 2outi = 1
2 + ·2hM̂
2z i
Measuring Spin-PolarizationMeasuring Spin-Polarization
Measuring Spin-PolarizationMeasuring Spin-Polarization
Á / (n1 ¡ n2)| {z }m
Spin-polarization
Speckle: Sanner et al., PRL 106, 010402 (2011)
Phase
The InterferometerThe Interferometer
The InterferometerThe Interferometer
PerformancePerformance
Single component: Phase-shift proportional to atomic density
PerformancePerformance
Photon shot-noise limited
ResultsResults
Distribution of Spin-PolarizationDistribution of Spin-Polarization
Weakly interacting gas
Distribution of Spin-PolarizationDistribution of Spin-Polarization
Weakly interacting gas
Distribution of Spin-PolarizationDistribution of Spin-Polarization
Weakly interacting gas
Distribution of Spin-PolarizationDistribution of Spin-Polarization
Strong repulsive interactions
Suppression of Spin-FluctuationsSuppression of Spin-Fluctuations
±m2
±m2thermal
• Relative suppression
• Agrees with theory for noninteracting Fermions
• Analogous to suppression of density-fluctutations due to
antibunching
9.2dB
Spin-SusceptibilitySpin-Susceptibility
kBTÂ=±M 2 ) kBTÂcol =A±m2
spin-susceptibility  = @(n1¡ n2)@(¹ 1¡ ¹ 2)
Measurements of spin-susceptibility: Salomon, Zwierlein, Ketterle
Spin-SusceptibilitySpin-Susceptibility
kBTÂ=±M 2 ) kBTÂcol =A±m2
spin-susceptibility  = @(n1¡ n2)@(¹ 1¡ ¹ 2)
EntanglementEntanglement
EntanglementEntanglement
~J =P
~¾i
¢ J 2z
hN i ¸ 23 ) A±m2
ncol¸ 2
3Wiesniak et al., NJP 7, 258 (2005); Toth et al., PRA 79, 042334 (2009)
EntanglementEntanglement
~J =P
~¾i
¢ J 2z
hN i ¸ 23 ) A±m2
ncol¸ 2
3
ncol (¹m¡ 2)
Am
2 (
μm
-2)
Wiesniak et al., NJP 7, 258 (2005); Toth et al., PRA 79, 042334 (2009)
fluctuationscorrelationsfluctuationscorrelations
Novel ProbesNovel Probes
thermodynamicproperties
thermodynamicproperties
mesoscopicsystems
mesoscopicsystems
Microscopic access
TeamworkTeamwork
DavidStadler
TorbenMüller
SebastianKrinner
Jean-PhilippeBrantut
Henning Moritz
Tilman Esslinger
JakobMeineke
Data ProcessingData Processing
Novel Probes for Fermionic GasesNovel Probes for Fermionic Gases
J. Meineke, T. Müller, B. Zimmermann, D. Stadler
J.-P. Brantut, H. Moritz, T. Esslinger
ETH Zürich
J. Meineke, T. Müller, B. Zimmermann, D. Stadler
J.-P. Brantut, H. Moritz, T. Esslinger
ETH Zürich