Quantum Optics with Electrical Circuits: Strong Coupling Cavity QED
Experiment Theory
Rob Schoelkopf Michel Devoret Andreas Wallraff Steven Girvin Alexandre Blais (Sherbrooke) David Schuster NSF/Keck Foundation Hannes Majer Jay Gambetta Center Luigi Frunzio Axel Andre R. Vijayaraghavan for K. Moon (Yonsei) Irfan Siddiqi Quantum Information Physics Terri Yu Michael Metcalfe Chad Rigetti Yale University R-S Huang (Ames Lab) Andrew Houck K. Sengupta (Toronto) Cliff Cheung (Harvard) Aash Clerk (McGill)
1 A Circuit Analog for Cavity QED 2g = vacuum Rabi freq. κ = cavity decay rate γ = “transverse” decay rate out
cm 2.5 λ ~ transmissionL = line “cavity”
E B DC + 5 µm 6 GHz in - ++ -
2 Blais et al., Phys. Rev. A 2004 10 µm The Chip for Circuit QED
Nb No wires Si attached Al to qubit! Nb
First coherent coupling of solid-state qubit to single photon: A. Wallraff, et al., Nature (London) 431, 162 (2004) Theory: Blais et al., Phys. Rev. A 69, 062320 (2004) 3 Advantages of 1d Cavity and Artificial Atom gd= i ERMS / Vacuum fields: Transition dipole: mode volume10−63λ de~40,000 a0
∼ 10dRydberg n=50 ERMS ~ 0.25 V/m
cm ide .5 gu 2 ave λ ~ w L = R ≥ λ e abl l c xia coa
R λ 5 µm Cooper-pair box “atom” 4 Resonator as Harmonic Oscillator
1122 L r C H =+()LI CV r 22L
Φ ≡=LI coordinate flux
ˆ † 1 V = momentum voltage Hacavity =+ ωr ()a2 ˆ † VV=+RMS ()aa
11ˆ 2 ⎛⎞1 CV00= ⎜⎟ ω 22⎝⎠2 ω VV= r ∼ 12− µ RMS 2C 5 The Artificial Atom non-dissipative ⇒ superconducting circuit element non-linear ⇒ Josephson tunnel junction
1nm +n(2e) -n(2e)
SUPERCONDUCTING Anharmonic! TUNNEL JUNCTION
ATOM Non-linear LC resonator 6 WHY SUPERCONDUCTIVITY?
E few electrons N ~ 109 total number of electrons “forest” of states N even
~ 1eV 2∆ ~ 1meV
superconducting gap ATOM SUPERCONDUCTING NANOELECTRODE7 Superconducting Tunnel Junction (The only non-linear dissipationless circuit element.)
N +1 pairs Al superconductor N pairs 8 N ∼ 10 Al2Ox tunnel barrier ∼ 1mµ N pairs Al superconductor N +1 pairs
Josephson Tunneling Splits the Bonding and Anti-bonding ‘Molecular Orbitals’ Covalently Bonded Diatomic ‘Molecule’
anti-bonding bonding
8 Bonding Anti-bonding Splitting
8 1 10 + 1 108 ψ =± ()8 ± 8 2 10 10 + 1
EEanti-bonding −=bonding EJ ∼∼4 −20 GHz 0.2 - 1.0 K Josephson coupling
↑= bonding Two-level approximation E z H =− J σ justified by large charging ↓= anti-bonding 2 energy. 9 SPLIT COOPER PAIR BOX QUBIT: THE “ARTIFICIAL ATOM” with two control knobs
E1
hν01
E0
⎡⎤nn++11n+ n ˆ 2 ⎛⎞π Φ ( ) HE=−⎢⎥C ()nNg nn−Ej cos⎜⎟ ∑ Φ 2 n ⎣⎦⎢⎥⎝⎠0
THE Hamiltonian (We mean it!) [Devoret & Martinis, QIP, 3, 351-380(2004)]10 BOX QUANTUM LEVELS AND MEASUREABLE QUANTITIES
charge E ∂E 1 Q = k k ∂U
) hν K 01 B k (
Energy current
∂Ek E0 I = k ∂Φ Φ/Φ0
CgU/2e 11 BOX QUANTUM LEVELS AND MEASUREABLE QUANTITIES
optimum working point for decoherence (sweet spot) charge E ∂E 1 Q = k = 0 k ∂U
) hν K 01 B k (
Energy current
E ∂Ek 0 Ik = = 0 ∂Φ Φ/Φ0
CgU/2e 12 BOX QUANTUM LEVELS AND MEASUREABLE QUANTITIES Walraff et al. Wilson et al. optimum working point for decoherence (sweet spot) charge capacitance E ∂E 2 1 k ∂ Ek Qk = C = ∂U k ∂U 2
) hν K 01 B k (
Energy current inductance
∂E 2 −1 E k ⎛⎞∂ Ek 0 Ik = Lk = ⎜⎟2 ∂Φ ⎝⎠∂Φ Φ/Φ0
CgU/2e 13 Siddiqi et al. Using the cavity to measure the state of the ‘atom’
qubit
V
0 State dependent polarizability of ‘atom’ pulls the cavity frequency14 cQED Dispersive Measurement
15 A. Blais, R.-S. Huang, A. Wallraff, S. M. Girvin, and RS, PRA 69, 062320 (2004) Coherent Control of Qubit in Cavity
signal for pure excited state
85 % contrast signal for gnd state
Rabi oscillations
consistent with 100% fidelity of qubit rotation High Visibility Rabi Oscillations
(i.e. inferred fidelity of operation)
Indicates no undesired entanglement with environment during operations.
A. Wallraff, D. I. Schuster, A. Blais, L. Frunzio, J. Majer, M.H. Devoret, SMG, and RJS, Phys. Rev. Letters 95, 060501 (2005). 17 Dephasing, decoherence, decay