Quantum Gases. Subhadeep Gupta. UW REU Seminar, 11 July 2011

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1 Quantum Gases Subhadeep Gupta UW REU Seminar, 11 July 2011

2 Ultracold Atoms, Mixtures, and Molecules Subhadeep Gupta UW REU Seminar, 11 July 2011

3 Ultracold Atoms High sensitivity (large signal to noise, long interrogation times in a well known atomic system) Precision measurements (fund const, fund sym, clocks) Sensing (accelerations, gravity gradients) Many-body aspects Quantum Fluids Condensed Matter Physics Nuclear Physics Quantum Engineering (Potentials and Interactions) Quantum Information Science Quantum Simulation Ultracold Molecules (through mixtures) Formation of a Bose- Einstein condensate (BEC) (1995)

4 Ultracold Atoms and Molecules at UW A dual-species experiment (Li-Yb) for making and studying ultracold polar molecules and for probing quantum mixtures Development of precision BEC interferometry (Yb) for fine structure constant α and test of QED

5 Quantum Degeneracy in a gas of atoms 1 atom per quantum state N atoms V volume T temperature Number of atoms = (Δx) 3 ~ V (Δp) 3 ~ (m k B T) 3/2 (available position space) (available momentum space) h 3 Quantum Phase Space Density n h 3 ~ 1 (m k B T) 3/2 (n=n/v) Air n ~ /cm 3, T c ~ 1mK Stuff n ~ /cm 3, T c ~ 0.1K Everything (except He) is solid Dilute metastable gases n ~ /cm 3 T c ~ 1μK!! Ultracold!! and ~ non-interacting

6 Bose-Einstein Condensation (BEC) λ = N db atoms 2 V volume T temperature h π mk T nλ 3 B db << 1 3 nλ db ~ 1 n = N V Quantum Phase Space Density 3 nλ db >> 1

7 Ordinary gas Bose-Einstein condensate atoms flit around randomly atoms march in lockstep divergent incoherent many small waves many modes diffraction limited (directional) coherent one big wave single mode (monochromatic)

8 Ordinary light Laser light divergent incoherent many small waves many modes diffraction limited (directional) coherent one big wave single mode (monochromatic)

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10 ABSOLUTE TEMPERATURE (log Kelvin scale) Laser cooling Nobel 1997 Evaporative cooling surface of sun room temp. liquid Nitrogen BCS superconductors, 4 He superfluid, CMB fractional quantum Hall effect superfluid 3 He p-wave dilute B threshold dilute BEC Nobel 2001 zero-point energy of gaseous condensate (h 2 /πm) n a interaction Energy scat length (controllable)

11 Laser Cooling???

12 z Laser Cooling I σ σ P x σ+ σ+ σ y I σ+ S Magneto-Optical Trap (MOT) Workhorse of laser cooling Atom Source ~ 600 K; UHV environment hω < h abs ω em => COOLING! (Need a 2 level system)

13 Laser Cooling!!! 100μK Magneto-Optic Trap (MOT) But the room is at 300K (!)

14 Evaporative Cooling in a Conservative Trap Optical Dipole Trap ω L << ω res Depth ~ I/Δ; Heating Rate ~ I/Δ 2 mk 2-1/2 V V 0 V pre collision post collision

15 Evaporative Cooling in a Conservative Trap Optical Dipole Trap ω L << ω res Depth ~ I/Δ; Heating Rate ~ I/Δ 2 μk 2-1/2 V V 0 V pre collision post collision

16 Imaging the Atoms (Formation of a Rb BEC in a magnetic trap, UC Berkeley 2005)

17 Lower Temp T ~ 150nK (Formation of a Yb BEC in an optical trap, UW Seattle 2011)

18 Landmark achievements in ultracold atomic physics Bose-Einstein condensation (JILA, MIT, Rice.) Macroscopic coherence (Ketterle) Superfluidity / observation and study of a vortex lattice (Dalibard, Ketterle, Cornell) Superfluid to Mott-insulator quantum phase transition (Hansch)

19 Different Quantum Matters decreasing temperature classical gas cold

20 Different Quantum Matters BEC decreasing temperature T = 0 classical gas cold Fermi Sea Fermi Energy (k B T F ) Fermions are much harder to cool because identical (in all respects) fermions will not interact s-wave (a=0). Need another spin state or another species of atom.

21 Landmark achievements in ultracold atomic physics Degenerate Fermi gas Molecular Bose-Einstein condensate (Jin, Hulet, Thomas, Ketterle, Grimm) Superfluidity of Fermi pairs

22 Ultracold Polar Molecules Realization of new quantum gases based on dipole-dipole interactions (1/r 3 vs 1/r 6 contact potential) Quantum Computing and Simulation Tests of fundamental symmetries Spectroscopies for clocks, time variations of fundamental constants Cold and ultracold controlled Chemistry

23 Polar (diatomic) Molecules from Ultracold Atoms

24 Polar (diatomic) Molecules from Ultracold Atoms New degrees of freedom bring with them scientific advantages New degrees of freedom bring with them technical issues (Hard to cool!) Unequal sharing of electrons Polarizable at relatively low field

25 Ultracold Atom Menu Very different mass, very different electronic structure strong dipole moment

26 Selected Molecular Constituents Studies of interacting quantum mixtures (different statistics, masses) Microscopic probes of superfluids

27 Selected Molecular Constituents New Quantum Fluid Dipolar and paramagnetic Paramagnetic ground state, heavy component candidate for electron EDM search Quantum computing candidate

28 Dual Species Apparatus Yb Oven Yb Zeeman Slower Pump Area Ultrahigh Vacuum (UHV < Torr) Li Oven Li Zeeman Slower Main Chamber AGENDA Cool and trap Li and Yb Study interacting mixture Induce controlled interactions Form molecules

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30 1 inch Dual Species Apparatus

31 Two-Species MOT Sequential Loading The 2 MOTs are optimized at different parameters of magnetic field gradient and also exhibit inelastic interactions

32 Optical Dipole Trap Crossed beam dipole trap 1064nm, up to 25 Watts 1 inch

33 Optical Dipole Trap Crossed beam dipole trap 1064nm, up to 25 Watts 1 inch

34 Ground State behavior of Li-Yb mixture B=0 It s stable! Extract a = (13± 3) a 0 (~ 0.7nm)

35 Sympathetic Cooling to below T F Small interspecies scattering length, but light Li provides high relative speed. T/T F ~ 0.7 T/T BEC ~ 4 Ivanov et al, PRL 106, (2011)

36 Simultaneous Quantum Degeneracy in alkali + spin-zero system 8ms TOF 0.7ms TOF Hansen et al, PRA (Rapid Comm), in press

37 Towards Interacting Mixtures and Molecules Search for Magnetic Feshbach Resonances Decay of Li atoms near 834 G MFR Atom loss spectroscopy

38 Precision Measurement of Fine Structure Constant α ac Josephson effect neutron interferometry h/m n Quantum Hall effect α = 2 e hc atomic physics route g-2 of electron + QED Cross-field comparisons Precision test of QED α -1 α -1 1 in ppb 98 (2000) (2008)

39 QED-free Atomic Physics Route to α motivation ppb: hydrogen spectroscopy, (Udem et al.,1997; Schwob et al.,1999) Penning trap mass spectroscopy e 2R h 2R α = = = hc c me c M M 0.7 ppb: penning trap mass spectr. (Beier et al., 2002) e h m Frequency comb ω = 1 h- rec 2 m k 2 Cs (Berkeley) Rb (Paris) BEC is a bright coherent source for atom interferometry

40 Contrast Interferometry with a BEC principle2 no sensitivity to mirror vibrations, ac stark shift, rotation, magnetic field gradients quadratic enhancement with additional momenta With Na BEC experiment 7ppm precision achieved, but inaccuracy at 200ppm, attributed to atomic interactions. The phase of the matter wave grating is encoded in oscillating contrast. Φ () t +Φ () t S T t C T t C T t (, ) = (, ) sin Φ ( t) = (, ) sin ( 8ω T + 4ω Δt) 2 rec rec The phase of the contrast signal for various T gives ω rec.

41 Contrast Interferometry with a BEC Scale Up Increase sensitivity by increasing momenta of 1 and 3 by 20-fold and increasing T Sub-ppb precision in few hours of data Use of a Yb BEC no B field sensitivity and multiple isotopes for systematic checks Atom laser has interactions careful study of this systematic effect

42 UW Ultracold Atoms Team Undergrad Students: Ben Schwyn, Charlie Fieseler Grad Students: Anders Hansen, Alex Khramov, Will Dowd, Alan Jamison, Ben Plotkin-Swing $$$ - NSF, Sloan Foundation, UW RRF, NIST