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Modeling a Flying Microwave Qubit
Slide 1/8 Transferring Quantum Information Using Superconducting Waveguides Kyle Keane Alexander N. Korotkov FUNDING AGENCIES Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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“INTERMEDIATE RESULTS” Kyle Keane and Alexander N. Korotkov
Introduction Slide 2/8 OPERATIONS “ALICE” “PRE-PROCESSOR” “INTERMEDIATE RESULTS” What is a Flying Qubit? Qubit that moves information between two processing or storage sites TRANSFER Why do we need them? Communication between two parties or nodes in a modular quantum computer “Flying Qubit” OPERATIONS “BOB” “PROCESSOR” “COMPUTATION” What do we look at? Microwave in a superconducting transmission line Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Kyle Keane and Alexander N. Korotkov
What has been done? Slide 3/8 Jahne, Yurke, Gavish: Proposed protocol with one tunable coupler Cirac, Zoller, Kimble, Mabuchi: ??? Braunstein, Kimble: ??? Razavi, Shapiro: ??? Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Kyle Keane and Alexander N. Korotkov
System Slide 4/8 High-Q Storage Tunable Couplers Example from UCSB Coplanar Waveguide or Phase Qubit Transmission Line 1 Superconducting Waveguide Tunable Parameter Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Kyle Keane and Alexander N. Korotkov
Main Idea Slide 5/8 SYSTEM HIGH-Q (WEAK COUPLING) This is still not a trivial problem CANCEL BACK REFLECTION Need INTERFERENCE “back into line” r B B t B r A A t A “into resonator” Transmission line Receiving resonator Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Time Dependence of Couplers
Slide 6/8 DEFINITIONS 1. WANT VOLTAGE FLOWING IN ONLY 2. EASIER TO THINK OF IT FLOWING OUT ONLY TL R TL R 3. TIME REVERSAL OF FLOWING OUT ONLY GIVES OUR NEEDED TIME DEPENDENCE 4. REQUIRES SPECIFIC CONTROL OF FIRST COUPLER TL R REQUIRES Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Achieving Near-Perfect Transfer
Slide 7/8 Qubit initially is here Qubit transferred to here Transmission Coefficients Time (t) Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Second Half = Time Reversal
Slide 8/8 Qubit initially is here Qubit transferred to here Transmission Coefficients Time (t) Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Ideal Estimates and Deviations
Slide 9/8 Qubit initially is here Qubit transferred to here Transmission Coefficients Time (t) UCSB ? ? MAX Transmission Coefficients Time (t) Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Kyle Keane and Alexander N. Korotkov
Timing Errors Slide 10/8 Transmission Coefficients Time (t) Fidelity (η) For 420 ns protocol This is 25 ns synchronized timing is very important Designed for η=0.999 Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Kyle Keane and Alexander N. Korotkov
Maximum Coupling Slide 11/8 Transmission Coefficients Time (t) Designed for η=0.999 Fidelity (η) Identical couplers are important Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Kyle Keane and Alexander N. Korotkov
Resonator Q Factor Slide 12/8 MAX Transmission Coefficients Time (t) Equal Q-factors are not very important Fidelity (η) Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Known Frequency Mismatch
Slide 13/8 Fidelity (η) Detuning (MHz) Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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Kyle Keane and Alexander N. Korotkov
Conclusions Slide 14/8 something something Other Considerations Multiple reflections Lossy materials Flying Microwave Qubit Kyle Keane and Alexander N. Korotkov
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