1.0 10 01 switching probability 0.8 0.6 00 0.4 0.2 0.0 11 0 100 Josephson qubits P. Bertet SPEC, CEA Saclay (France), Quantronics group 200 300 swap duration (ns) 400 Introduction : Josephson circuits for quantum physics From a fundamental question (25 years ago) …. CAN MACROSCOPIC « MAN-MADE » ELECTRICAL CIRCUITS BEHAVE QUANTUM-MECHANICALLY ???? M.H. Devoret, J.M. Martinis and J. Clarke, PRL 85, 1908 (1985) M.H. Devoret, J.M. Martinis and J. Clarke, PRL 85, 1543 (1985) YES THEY CAN Discrete energy levels … to genuine quantum information and quantum optics on a chip … AND MUCH MORE TO COME !! M. Hofheinz et al., Nature (2009) Q. state engineering and M. Neeley et al., Nature (2011) Tomography 3-qubit entanglement Outline Lecture 1: Basics of superconducting qubits Lecture 2: Qubit readout and circuit quantum electrodynamics Lecture 3: 2-qubit gates and quantum processor architectures Outline Lecture 1: Basics of superconducting qubits 1) Introduction: Hamiltonian of an electrical circuit 2) The Cooper-pair box 3) Decoherence of superconducting qubits Lecture 2: Qubit readout and circuit quantum electrodynamics Lecture 3: 2-qubit gates and quantum processor architectures Real atoms rˆ , pˆ i V (r ) Hydrogen atom e 2 quantization 4 0 r Energy (a.u) |3> |2> |1> E01=E1-E0=hn01 « two-level atom » |0> x (a.u.) I.1) Introduction Hˆ 2 pˆ 2m V ( rˆ ) Real atoms rˆ , pˆ i V (r ) Hydrogen atom e 2 quantization 2 pˆ Hˆ 4 0 r 2m E ( t ) E 0 cos 2n t H I (t ) d E (t ) laser + spontaneous emission G Spectroscopy (weak field) V ( rˆ ) Optical Bloch equations Rabi oscillations (short pulses, strong field at n=n01) n01 |0> |0> FWHM G/2 fR P(1) P(1) (a.u) 1 |1> Frequency n (a.u) I.1) Introduction 1 2 0 0 1 Time (a.u) d E0 h (t ) Electrical harmonic oscillator x k k 0 m 0 Q (t ) f 1 +q -q LC m H ( x, p ) kx 2 2 p 2 H ( , Q ) |4> |3> |2> |1> |0> Q 2 2C Quantum regime ?? 0 X,f I.1) Introduction 2 ˆ , Qˆ i xˆ , pˆ i E 2L 2m t V ( t ') dt ' t i ( t ') dt ' LC oscillator in the quantum regime ? 2 conditions : E kT 0 |4> |3> |2> |1> |0> X,f E |4> |3> |2> |1> |0> At T=30mK : hn 0 8 kT Q 1 OK if dissipation negligible X,f I.1) Introduction C pF n 0 5G H z Typic : L n H Superconductors at T<<Tc Microwave superconducting resonators Q=4 1010 at 51GHz and at 1K Tc(Nb)=9.2K Quantum regime S. Kuhr et al., APL 90, 164101 (2006) T<<Tc : dissipation negligble at GHz frequencies I.1) Introduction Necessity of anharmonicity |4> |3> |2> |1> |0> E f +q -q 0 X,f How to prepare |1> ? Need non-linear and non dissipative element : Josephson junction I.1) Introduction Basics of the Josephson junction (t ) Q (t ) The building block of superconducting qubits θ= /2e θR N = Q /2 e Josephson DC relation : I I C sin d 2 e dt Q C B. Josephson, Phys. Lett. 1, 251 (1962) P.W. Anderson & J.M. Rowell, Phys. Rev. 10, 230 (1963) S. Shapiro, Phys. Rev. 11, 80 (1963) I.1) Introduction V ( t ') dt ' t i ( t ') dt ' m od(2 )= θ R -θ L 0, 2 θL Josephson AC relation : V t (t ) Basics of the Josephson junction Q (t ) The building block of superconducting qubits θ= /2e t V ( t ') dt ' t i ( t ') dt ' m od(2 )= θ R -θ L 0, 2 θL θR N = Q /2 e Josephson DC relation : I I C sin d Josephson AC relation : V 2 e dt NON-LINEAR INDUCTANCE POTENTIAL ENERGY I.1) Introduction LJ ( I ) E J ( ) IC 2e Classical variables ?? Q C 2 eI C 1 I / I C 2 cos E J cos Hamiltonian of an arbitrary circuit = = HAMILTONIAN ??? Correct procedure described in : M. H. Devoret, p. 351 in Quantum fluctuations (Les Houches 1995) G. Burkard et al., Phys. Rev. B 69, 064503 (2004) G. Wendin and V. Shumeiko, cond-mat/0508729 M.H. Devoret, lectures at Collège de France (2008) accessible online Hamiltonian of an arbitrary circuit = = HAMILTONIAN ??? 1) Identify the relevant independent circuit variables 2) Write the circuit Lagrangian 3) Determine the canonical conjugate variables and the Hamiltonian Hamiltonian of an arbitrary circuit node branch = = Identifying the relevant independent circuit variables 1) Choose reference node (ground) Hamiltonian of an arbitrary circuit = = Identifying the relevant independent circuit variables 1) Choose reference node (ground) 2) Choose « spanning tree » (no loop) Hamiltonian of an arbitrary circuit d c = a b e = Identifying the relevant independent circuit variables 1) Choose reference node (ground) 2) Choose « spanning tree » (no loop) 3) Define « tree branch fluxes » i ( t ) t V ( t ') dt ' Hamiltonian of an arbitrary circuit = 3 c a = 2 b d e 1 5 Identifying the relevant independent circuit variables 1) Choose reference node (ground) 2) Choose « spanning tree » (no loop) 3) Define « tree branch fluxes » i ( t ) 4= b + d t V ( t ') dt ' 4) Define node fluxes = sum of branch fluxes from ground Hamiltonian of an arbitrary circuit 3 = c a 2 b d e 1 = Write Lagrangian 4= b + d 5 L ( i , i ) L el ( i ) L p o t ( i ) taking into account constraints imposed by external biases (fluxes or charges) 1 2 L pot E J cos 2 1 ext 1 2 ext 2L 2 Hamiltonian of an arbitrary circuit 3 = c a 2 b Conjugate variables : Qi 5 L i Classical Hamiltonian H ( i , Q i ) Quantum Hamiltonian 4= b + d e 1 = or d Q H ( ˆ i , Qˆ i ) nˆ i Qˆ i / 2 e ˆ with ˆ H ( i , n i ) ˆi ˆ i ( 2 e / ) i i With L ˆ , Qˆ i i i ˆi , nˆ i i Different types of qubits Cooper-pair boxes NIST Santa Barbara 0 .1 1 5 0 50 Charge qubit/Quantronium/Transmon -1 I.2) Cooper-Pair Box 0 /(rad) 1 4 100mm2 .04mm2 Ep (a.u) Ep (a.u) Shape Of the Potential Energy .01 to 0.04 mm2 10 Ep (a.u) Junctions sizes Phase qubits TU Delft MIT Berkeley NEC Saclay Chalmers NEC Yale ETH Zurich E J / EC Flux qubits -2 0 m/ 2 -2 0 (rad) 2 4 Different types of qubits Cooper-pair boxes NIST Santa Barbara 0 .1 1 5 0 50 Charge qubit/Quantronium/Transmon -1 I.2) Cooper-Pair Box 0 /(rad) 1 4 100mm2 .04mm2 Ep (a.u) Ep (a.u) Shape Of the Potential Energy .01 to 0.04 mm2 10 Ep (a.u) Junctions sizes Phase qubits TU Delft MIT Berkeley NEC Saclay Chalmers NEC Yale ETH Zurich E J / EC Flux qubits -2 0 m/ 2 -2 0 (rad) 2 4 The Cooper-Pair Box E C ,E J Vg 1 degree of freedom θˆ , Nˆ i 1 knob Ec (2 e ) 2 « charging energy » 2C ˆ = E (N ˆ - N ) 2 - E cos ˆ H C g J The split CPB E C ,E J θ1 N1 θ Vg θ2 inductance N2 L small 2 d° of freedom θˆ , Nˆ i 1 1 θˆ , Nˆ i 2 2 or ˆ + Nˆ N 1 2 ˆ ˆ ˆ ˆ =θ 1 +θ 2 , K = 2 2 knobs 2 Hˆ = E C ( Nˆ - N g ) - E J cos ˆ 2 cos ˆ ˆ -θˆ θ ˆθ= 2 1 , Nˆ = Nˆ - Nˆ i 1 2 2 0 ˆ 2L 2 L 2 0 EJ i The split CPB E C ,E J N Vg 1 d° of freedom θˆ , Nˆ i 2 knobs 2 ˆ ˆ H = E C ( N - N g ) - E J cos cos ˆ 2 tunable E J δ= 0 Energy levels of the CPB E ˆ (N , ) = E ( N ˆ - N ) 2 - E ( )cos ˆ H g C g J Solve either in charge basis |N> ( N k k ) ( N g , ), k ( N g , ) c k ,N N N EJ 2 ˆ H = E C (N - N g ) N N 2 Diagonalize I.2) Cooper-Pair Box ... ... ... ... ... ... E C (-1 - N g ) 2 N +1 N N N +1 N ... ... ... -E J /2 0 ... 2 -E J /2 E C (0 - N g ) - E J /2 0 -E J /2 E C (1 - N g ) ... .. . ... 2 ... ... ... ... N = -1 N = 0 N =1 ... Energy levels of the CPB E ˆ (N , ) = E ( N ˆ - N ) 2 - E ( )cos ˆ H g C g J … or in phase basis |> ( 0, 2 k ( N g , ), k ( N g , ) 2 ) k d k ( ) 0 ˆ (N , ) = E ( 1 - N ) 2 - E ( ) cos H g C g J i Solve Mathieu equation EC ( I.2) Cooper-Pair Box 1 i - N g ) k ( ) - E J ( ) cos k ( ) = E k k ( ) 2 Two simple limits : (1) E J ( ) EC (charge regime) Ej Ec 0 2 2 Energy EJ/Ec=0 1 1 0 0 c0 ( N ) c 1( N ) 00 1 0.5 0.5 11 1.5 1.5 22 2 1 0 1 2 3 2 0 N 0 0.5 1 ( ) 3 3 3 Ng 0.5 0 ( ) 3 1 2.5 2.5 2 1 0 1 2 3 N 2 0 0 Two simple limits : (1) E J ( ) EC (charge regime) 2 EJ/Ec=0.1 Energy E2(Ng) 1 E1(Ng) E0(Ng) 0 Ng=0.01 0 0.5 1 1.5 2 3 Ng 2.5 1 0.5 c0 ( N ) 0 ( ) 3 2 1 0 1 2 2 0 3 1 0.5 c 1( N ) 1 ( ) 3 0 2 1 0 1 2 3 2 0 0 QUBIT Two simple limits : (1) E J ( ) EC (charge regime) 2 EJ/Ec=0.1 Energy E2(Ng) 1 E1(Ng) E0(Ng) 0 Ng=0.5 0 0.5 1 1.5 2 3 Ng 2.5 1 0.5 c0 ( N ) 0 ( ) 2 0 3 2 1 0 1 2 3 0.5 1 c 1( N ) 1 ( ) 2 0 3 0 2 1 0 1 2 3 0 QUBIT From E J ( ) E C to E J ( ) Energy EJ/Ec=0.5 EJ/Ec=2 2.0 3 1.5 2 1.0 1 0.5 0.0 0 0.5 1 1.0 0.0 Ng 0.2 0.4 0.6 0.8 1.0 2 0.0 Ng 0.2 0.4 0.6 0.8 1.0 0.8 1.0 EJ/Ec=10 EJ/Ec=5 2 2 Energy EC 0 0 2 4 2 6 4 0.0 0.2 0.4 0.6 0.8 1.0 Ng 8 0.0 0.2 0.4 0.6 STILL A QUBIT ! Ng Two simple limits : (2) E J ( ) (phase regime) EC J. Koch et al., PRA (2008) EJ/Ec=10 2 0 2 4 6 8 0.0 0.2 1.0 0.5 0.0 c0 ( N ) 0.5 1.0 1.0 0.5 c 1 ( N ) 0.0 0.5 1.0 I.2) Cooper-Pair Box 0.4 0.6 0.8 1.0 Ng 2 0 ( ) 0.5 4 2 0 2 0 4 1 ( ) 0 2 0.5 4 2 0 2 4 0 0 Experimental spectrum of a transmon J. Schreier et al., PRB (2008) One-qubit gates Ng(t)=DNgcost TRANSMON QUBIT ˆ =E N ˆ - N (t ) H C g 2 - E J cos ˆ ˆ =E N ˆ 2 - E cos ˆ - 2E D N co s tN ˆ H C J C g transmon Two-level approximation 01 ( ) 2 drive z R cos t x R 2 EC 0 N 1 DN g I.2) Cooper-Pair Box One-qubit gates =01 f0 Rotation : X TRANSMON QUBIT |0> Z Y I.2) Cooper-Pair Box |1> X One-qubit gates =01 f0 f0f Xf Rotation : X TRANSMON QUBIT |0> Z Y f Xf I.2) Cooper-Pair Box |1> X One-qubit gates =01 f0 f0f Xf Rotation : X TRANSMON QUBIT |0> Z Z rotation Y f Xf X All rotations on Bloch sphere Fidelity ? 99% J.M. Chow et al., PRL 102, 090502 (2009) I.2) Cooper-Pair Box |1> Decoherence Ng+dNg(t) d(t) Noise in Hamiltonian parameters DECOHERENCE MAJOR OBSTACLE TO QUANTUM COMPUTING I.3) Decoherence Decoherence in superconducting qubits (Ithier et al., PRB 72, 134519, 2005) Pure dephasing Relaxation (Spontaneous emission) i(t) 01 ( i ) 1 01 0 t 1 0 e 0 D , 1 0 H f (t ) e 1 T2 T1 1 G1 2 D , S ( 01 ) 2 environmental density of modes at qubit frequency I.3) Decoherence 1 01 1 i ( t ) G2 G D D ,z i ( t ) e G1 2 2 ,z G 2t G S (0 ) Low-frequency noise Decoherence Ng+dNg(t) d(t) Noise in Hamiltonian parameters DECOHERENCE Origin of the noise ??? I.3) Decoherence Decoherence Ng+dNg(t) d(t) Noise in Hamiltonian parameters R DECOHERENCE R Origin of the noise ??? 1) ELECTROMAGNETIC Low-frequency : Johnson-Nyquist due to thermal noise High-frequency : spontaneous emission (quantum noise) I.3) Decoherence Under control Decoherence e- Ng+dNg(t) Spin flips d(t) Noise in Hamiltonian parameters R DECOHERENCE R Origin of the noise ??? 2) MICROSCOPIC Low-frequency noise well studied : High-frequency (GHz) microscopic noise I.3) Decoherence Flux noise Charge noise 3 S N g ( ) (10 ) 6 2 S ( ) (10 0 ) TOTALLY UNKNOWN !! 2 Decoherence e- Ng+dNg(t) Spin flips d(t) Noise in Hamiltonian parameters R DECOHERENCE R Origin of the noise ??? 2) MICROSCOPIC Low-frequency noise well studied : CPB in charge regime Transmon High-frequency (GHz) microscopic noise I.3) Decoherence Flux noise Charge noise 3 S N g ( ) T2 T2 (10 ) 6 2 S ( ) (10 0 ) 10 100 ns T2 1 100 m s 1 10 ms T2 1 100 m s TOTALLY UNKNOWN !! 2 State-of-the-art coherence times T1=1-2ms T2=1-3ms Schreier et al., PRB 77, 180502 (2008) I.3) Decoherence Very recent breakthrough: transmon in 3D cavity H. Paik et al., quant-ph (2011) T1=60ms T2=15ms ULTIMATE LIMITS ON COHERENCE TIMES UNKNOWN YET I.3) Decoherence Fabrication techniques small junctions 1) e-beam patterning 2) development 3) first evaporation 4) oxidation 5) second evap. 6) lift-off 7) electrical test e-beam lithography e- Al/Al2O3/Al junctions O2 PMMA PMMA-MAA SiO2 I.3) Decoherence small junctions Multi angle shadow evaporation QUANTRONIUM (Saclay group) gate I.3) Decoherence 160 x160 nm FLUX-QUBIT (Delft group) I.3) Decoherence TRANSMON QUBIT (Saclay group) 40mm 2mm I.3) Decoherence END OF FIRST LECTURE