Implementation of Cross-Resonance System for Implementation of Cross-Resonance System for Universal

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Transcript of Implementation of Cross-Resonance System for Implementation of Cross-Resonance System for Universal

  • Implementation of Cross-Resonance System for Universal Quantum Computing

    1215047 S. Shirai Department of Physics, Tokyo University of Science. Center of Emergent Matter Science, RIKEN.

    Introduction

    Cross-Resonance Gate

    Fabricated Sample

    Experimental Result

    Conclusion and Future Work

    Universal quantum computing

    Theory of circuit QED

    g

    Cavity + Two level system

    ωσz/2 ωra†a

    Resonator1 Q1

    Resonator + SC qubit

    "cavity" QED "circuit" QED

    g

    n=0

    n=1

    n=2

    n=3

    n=0

    n=1 n=2 n=3

    Harmonic oscillator Transmon (Charge qubit)

    LC C JosephsonJunction

    Cavity Quantum electrodynamics (cavity QED) is the study of the interaction between light and atom. The case of a single 2-level atom in the cavity is mathematically described by the Jaynes- Cummings model. On the other hand, by using the macroscopic quantum effect appearing in the superconductor, it is possible to construct a system of cavity QED by the solid element. Such a system is called a "circuit QED" system.

    Jaynes-Cummings Hamiltonian :

    Superconducting Qubit AlOxSC(Al) SC(Al)

    AlOxSC(Al) SC(Al)

    Josephson Junction

    Qubit Subspace

    ・Tunability ・Noise sorce

    BusResonator1 Resonator2 Q1 Q2

    ω2(=Q2 frequency)

    J g2g1

    fast oscillating term

    When the time evolution by microwave irradiation of the system is sufficiently long, the effect of the vibration term is reduced.

    =A(t)

    Time evolution for CNOT 0

    0011

    101 1

    0110

    010 OutputInput CNOT gate''Control bit''

    "Target bit"

    Bit flip

    Bit flip

    When the value of the control bit is 1, the gate that inverts the value of the target bit is called "Controled-NOT gate" (Simply, CNOT).

    Pulsed spectroscopy

    CNOT=[ZI]-1/2[ZX]1/2[IX]-1/2 ref. 10.1103/PhysRevB.81.134507

    We get CNOT by combining with one qubit gates.

    time

    Δt=10ns

    Qubit Drive

    Probe

    τ

    tp~2us

    ΩR

    time

    Δt=10ns

    Qubit Drive

    Probe

    td~4us

    tp~2us

    τ [ns] τ [ns]

    Qubit2

    Qubit2

    Qubit2Qubit1

    2J~40MHz

    Rabi oscillation

    Fitting function :

    τR~448 ns τR~1032 ns

    The sample could not work in the regime of CR gate. However, I could confirm the existence of coupling between qubits. Next time, I would like to fabricate the qubits with better coherence time in CR gate regime.

    Acknowledgment This work supported by JST CREST Grant Number JPMJCR1676, Japan.

    fig. truth table

    500 μm

    fig.1 example of quantum circuit

    According to the Solovay-Kitaev theorem, arbitrary N-qubit unitary operators can be approximated with ''universal gate set''.{S, H, T, CNOT} is one of universal set. CNOT gate is so-called two-qubit entangling gate. It is difficult to realize two-qubit gates compared to one-qubit gates. So, implementing a precise 2-qubit gate is one of the big challenges.

    fig. SQUID

    Φ I I

    fig. Cross-Resonance system Resonator + SC qubit are smallest set of cQED system. The above system Hamiltonian can be written as bellow.

    After performing the two-level approximation, unitary transformation and perturbative expantion are performed and the following interaction Hamiltonian is obtained while irradiating microwaves from the outside under the condition of {| J / ω1-ω2 |