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Dynamics of a Resonator Coupled to a Superconducting Single-Electron Transistor Andrew Armour University of Nottingham
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Outline Introduction –Superconducting SET (SSET) –SSET + resonator SSET as an effective thermal bath –Fokker-Planck equation –Experimental results (mechanical resonator) Unstable regime –Numerical solution –Quantum optical analogy: micromaser –Semi-classical description
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Superconducting SET Gate Voltage Quasiparticle tunnelling Josephson Quasiparticle Resonance [JQP] Double Josephson Quasiparticle Resonance [DJQP] Hadley et al., PRB 58 15317 Drain Source Voltage Superconducting island coupled by tunnel junctions to superconducting leads +V g
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JQP resonance Drain source/Gate voltages tuned to: 1. Bring Cooper pair transfer across one jn resonant 2. Allow quasiparticle decays across other jn Current flows via coherent Cooper pair tunnelling+ Incoherent quasiparticle tunnelling QP CP I0I0 EE
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LaHaye et al, Science 304, 74 Naik et al., Nature 443, 193 Nanomechanical resonator & SSET Motion of resonator affects SSET current SET suggested as ultra-sensitive displacement detector –White Jap. J. Appl. Phys. Pt2 32, L1571 –Blencowe and Wybourne APL 77, 3845 Devices fabricated so far have frequencies ~20MHz fluctuations in island charge acts back on resonator: alters dynamics
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Superconducting resonator Can also fabricate superconducting strip-line resonators: Coupling to a Cooper-pair box achieved Resonators can be very high frequency >GHz A. Wallraff et al. Nature 431 162
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SSET-Resonator System Three charge states involved in JQP cycle: |0>, |1> and |2> Resonator, frequency , couples to charge on SET island with strength Charge states |0> and |2> differ in energy by E (zero at centre of resonance) Coherent Josephson tunnelling parameterised by E J links states |0> and |2>
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Effect of resonator’s thermalized surroundings: Characterized through a damping rate, ext and an average number of resonator quanta n Bath Quantum master equation Quasi-particle tunnelling from island to leads: 2 processes occur, |2>|1> and |1>|0> but we assume the rate is the same, Include dissipation:
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Effective description of resonator Can obtain effective description of resonator dynamics by taking Wigner transform of the master equation and tracing out electrical degrees of freedom Obtain a Fokker-Planck equation: Assumes resonator does not strongly affect SSET: requires weak-coupling and small resonator motion For now, will also assume the resonator is slow: << Blencowe, Imbers and AA, New J. Phys. 7 236 Clerk and Bennett New J. Phys. 7 238
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Resonator Damping Effective damping due to SET: Negative damping tells us that resonator motion will not be captured by Fokker-Planck equation for long times Negative damping Positive damping EE
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Effective SET temperature Quasiparticle tunnelling rate Detuning from centre of JQP resonance ‘Negative Temperature’ Positive Temperature Temperature changes sign at resonance Can obtain simple analytic expression: Minimum in T SET set by quasiparticle decay rate cf: Doppler cooling EE
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Experimental Results Naik, Buu, LaHaye, and Schwab (Cornell) Nanomechanical Beam JQP bias point SSET gate Infer resonator properties from SSET charge noise power around mechanical frequency: known to provide good thermometry for resonator [ LaHaye et al.,Science 304 74 ] SSET island
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Back-action: Cooling & Heating Cooling Coupling: Naik et al., Nature 443 193 Theory: T SET ~220mK But damping does not match theory so well
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What happens to the resonator steady-state in the ‘unstable’ regime: Bath + SET <0 For ‘slow’ resonator can also include feedback effects in Fokker-Planck equation Can evaluate steady-state of the system by numerical evaluation of the master equation eigenvector with zero eigenvalue Instabilities turn out to be result of largely classical resonances: semi-classical description also useful Dynamic Instability Clerk and Bennett New J. Phys. 7 238; PRB 74 201301 Rodrigues, Imbers and AA PRL 98 067204 Rodrigues, Imbers, Harvey and AA cond-mat/0703150
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Steady-state Wigner functions “Bistable”Limit-CycleFixed point + 0 EE Resonator pumped by energy transferred from Cooper pairs: E>0: CP can take energy from resonator E<0: CP can give energy to resonator Far from resonance: little current, so little pumping and external damping stabilizes resonator
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Resonator moments I. Slow resonator limit: /<<1 Non-equilibrium/Kinetic phase transitions: Order-parameter: n mp Fixed point -> Limit cycle: Continuous Bistability: Discontinuous F=( - 2 )/ 2
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Resonator moments II. EEEE F As increases, resonance lines emerge: E=nh Most interesting behaviour for /~1: ~Mutual interaction strongest ~Non-classical states emerge even at low coupling -2 -1 0 +1 F<1 region
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Analogue: Micromaser Pump parameter= (N ex ) 1/2 x coupling strength x interaction time N ex =no. atoms passing through cavity during field lifetime n/n max Stream of two-level atoms pass through a cavity resonator: can identify non- equilibrium phase transitions resonator state can be number-squeezed (F<1) Filipowicz et al PRA 43 3077; Wellens et al Chem. Phys. 268 131 N ex
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SSET-resonator system Only 1 st transition is sharp: sharpness of transitions depends on current which decreases with Traces of further transitions seen in n mp Well-defined region where F<1 /=1; n Bath =0
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Semi-classical dynamics Equations of motion for 1 st moments of system –Semi-classical approx.: Weak , Bath resonator amplitude changes slowly: –Periodic electronic motion calculated for fixed resonator amplitude –leads to amplitude-dependent effective damping: –Good match with full quantum numerics for weak-coupling –Analytical expression available in low-E J limit
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Limit cycles satisfy condition: Maxima in SSET due to commensurability of electrical & mechanical oscillations Electrical oscillations: frequency 1/2 A Increasing compresses SSET oscillations leads to bifurcations Origin of instabilities
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Conclusions Despite linear-coupling SSET-resonator system shows a rich non-linear dynamics Cooling behaviour seen on ‘red detuned’ side of resonance ‘Blue detuned’ region shows rich variety of behaviours similar to micromaser Semi-classical description works (surprisingly) well Investigate dynamics further through current noise, quantum trajectories
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Acknowledgements Collaborators –Jara Imbers, Denzil Rodrigues Tom Harvey (Nottingham) –Miles Blencowe (Dartmouth) –Akshay Naik, Olivier Buu, Matt LaHaye, Keith Schwab (Cornell) –Aashish Clerk (McGill) Funding
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