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Excitonic BEC in in Quantum Hall Bilayers Ramin Abolfath NRCC Anton Burkov UCSB Jim Eisenstein Cal Tech. Steve Girvin Yale Yogesh Joglekar LANL Jairo Sinova.

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Presentation on theme: "Excitonic BEC in in Quantum Hall Bilayers Ramin Abolfath NRCC Anton Burkov UCSB Jim Eisenstein Cal Tech. Steve Girvin Yale Yogesh Joglekar LANL Jairo Sinova."— Presentation transcript:

1 Excitonic BEC in in Quantum Hall Bilayers Ramin Abolfath NRCC Anton Burkov UCSB Jim Eisenstein Cal Tech. Steve Girvin Yale Yogesh Joglekar LANL Jairo Sinova Texas A&M Ady Stern Weizmann Leo Radzihovsky UC Alvaro Nunez UTA Enrico Rossi UTA Giovanni Vignale UMC University of Texas at Austin May 2005

2 Reference Eisenstein and AHM Nature 432, 691 (2004)

3 Josephson Qubit Devoret Walraff & Martinis cond-mat/0411 Non-linear Non-Dissipative

4 Landau Liftshitz Gilbert

5 Excitons – Elementary Excitations of Intrinsic Semiconductors e - h h e Valence Band Conduction Band

6 Excitonic BEC and Superfluidity?

7 Electron-Hole Pairs (n’,n)=( ,  ) =Ferromagnetism (n’,n)=(c,v) = Excitonic BECs (n’,n)=(TopLayer,BottomLayer) Order Parameter Counterflow Superfluidity

8 Ga As Si AlGaAs GaAs 100 A AlGaAs Double Quantum Well - Quantum Wells

9 Ga As ultra high vacuum heated cells high quality GaAs substrate Al Molecular Beam Epitaxy Pfeiffer - Bell Labs Shayegan – Princeton

10 Electrons and Holes in the QH Regime Add magnetic field Particle-hole transformation Assemble Bilayer

11 I I e - voltmeter 0 0

12 Electron-hole Pair Current

13 Superflow in Electron-Electron Bilayers Kellogg and Eisenstein cond-mat/0401521 Hall Angle Not Large σ xx  1000 e 2 /h

14 Interlayer Voltage 0 Tunneling rate 0 Josephson-like Currents

15 Josephson Effect J.J. Dynamics eV = 0 Δ sin(φ) = I bias Correct Explanation? 0

16 Collective Dynamics & Dissipation Ferromagnets vs. Josephson Junctions vs. Bilayers J.J. Dynamics Thin Film Ferromagnet Dynamics

17 Joglekar TDHFA+SCBA  α φ >> α N Joglekar & AHM PRB (2002)

18 Thin Film Ferromagnets Buhrman & Ralph, MSU, NIST, Orsay Thin Film Ferromagnet Dynamics Spin Transfer

19 Transport Orbitals eV Condensate Orbitals K = X l 2 Coherent Edge Transport E mpl  10 -6 eV Δ QP  10 -3 eV G  e 2 /h Δ t  10 -9 eV V *  10 -6 Volts

20 Excitonic Bose Einstein Condensation in Quantum Hall Bilayers ! Macroscopic Quantum Coherence properties different from both JJ’s and thin film magnets


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