Qubit-Coupled Mechanics - IFSC

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Now that mechanical structures have been cooled near the ground state, how do you prepare and measure quantum states of these structures?
Limitations of Linear Displacement Detectors Typically, displacement transducers are linear x k m Linear Detector Output is linearly proportional to x Obviously, many examples: capacitive, magnetomotive, piezoelectric, transistor current However, linear detectors generally should drive resonator into ‘classical-like’ states, coherent states of motion Coherent State |α(t)⟩ = e −iωω− α 2 (αe−iii ) n |n⟩ n! ∞ n=0 x(t) = ħ mω α cosωω
Page 1 and 2: Qubit-Coupled Mechanics Matt LaHaye
Page 3 and 4: Mechanical Systems in the Quantum R
Page 5 and 6: What do We Hope to Accomplish With
Page 7 and 8: The Future: Quantum Machines?
Page 9 and 10: What does it take to get to the qua
Page 11 and 12: Thermal Noise E Energy Spectrum The
Page 13 and 14: Chasing the Ground State Cooling th
Page 15: Approaching the Ground State: Back-
Page 19 and 20: Schematic of Coupling Between a Coo
Page 21 and 22: Schematic of Coupling Between a Coo
Page 23 and 24: The Dispersive Coupling Limit Inter
Page 25 and 26: First Realization of Qubit-Coupled
Page 27 and 28: Milestone in Quantum Measurement Na
Page 29 and 30: The Dispersive Coupling Limit *See:
Page 31 and 32: Engineering the qubit read-out: Emb
Page 33 and 34: Present Status of Our Efforts at Sy
Page 35 and 36: LC Circuit Read-out of Qubit vs. Ap
Page 37 and 38: Details of the UHF Flexural Nanomec
Page 39 and 40: LC Read-out of Qubit: Two-Tone Spec
Page 41 and 42: Two-Tone Spectroscopy - ‘Extra’

Qubit-Coupled Mechanics - IFSC

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