Abstract

Optically addressable paramagnetic defects in wide-band-gap semiconductors are promising platforms for quantum communications and sensing. The presence of avoided crossings between the electronic levels of these defects can substantially alter their quantum dynamics and be both detrimental and beneficial for quantum information applications. Avoided crossings give rise to clock transitions, which can significantly improve protection from magnetic noise and favorably increase coherence time. However, the reduced coupling between electronic and nuclear spins at an avoided crossing may be detrimental to applications where nuclear spins act as quantum memories. Here we present a combined theoretical and experimental study of the quantum dynamics of paramagnetic defects interacting with a nuclear spin bath at avoided crossings. We develop a computational approach based on a generalization of the cluster expansion technique, which can account for processes beyond pure dephasing and describe the dynamics of any solid-state spin-qubits near avoided crossings. Using this approach and experimental validation, we determine the change in nature and source of noise at avoided crossings for divacancies in SiC. We find that we can condition the clock transition of the divacancies in SiC on multiple adjacent nuclear spins states. In our experiments, we demonstrate that one can suppress the effects of fluctuating charge impurities with depletion techniques, leading to an increased coherence time at clock transition, limited purely by magnetic noise. Combined with ab-initio predictions of spin Hamiltonian parameters, the proposed theoretical approach paves the way to designing the coherence properties of spin qubits from first principles.

Highlights

  • In search of solid-state qubits, electron spin defects in wide-band-gap semiconductors have been extensively explored as robust quantum systems offering both long coherence times [1] and optical readout [2] capabilities for quantum information [3] and quantum sensing [4] applications

  • We investigate the dynamics of a spin qubit by studying the evolution of the central spin interacting with the nuclear spin bath

  • Under charge depleted conditions, the measured coherence time is substantially increased and the experimentally observed Ramsey precession at zero field agrees well with the theoretical prediction of the generalized CCE (gCCE)

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Summary

INTRODUCTION

In search of solid-state qubits, electron spin defects in wide-band-gap semiconductors have been extensively explored as robust quantum systems offering both long coherence times [1] and optical readout [2] capabilities for quantum information [3] and quantum sensing [4] applications. In order to design optimal qubits, it is critical to understand and control the interaction between the central electronic spin and the nuclear spin bath The latter determines, at least in part, the coherence time of qubits, as observed in many solid-state color centers [5,6,7,8], but it offers a platform for robust multiqubit registers for the development of quantum networks [9,10,11,12]. We investigate the adiabatic dynamics of a qubit interacting with nuclear baths at clock transitions and near ground-state level anticrossings (GSLACs) both theoretically and experimentally. We show experimentally that the impact of the nuclear bath on the qubit dynamics can be isolated by employing a charge depletion technique, which leads to an increase of spin coherence time of clock transition qubits by suppressing electric noise.

Spin defect Hamiltonian
Cluster-correlation expansion method for avoided crossings
DECOHERENCE AT GROUND-STATE LEVEL ANTICROSSINGS
DECOHERENCE AT CLOCK TRANSITIONS
Impact of nuclear spin coupling
NATURE OF NUCLEAR NOISE IN SOLID-STATE QUBITS
ENGINEERING QUBIT PROTECTION AT A CLOCK TRANSITION
CONCLUSIONS
Impact of the magnetic field on the initial qubit state of basal divacancy
Determining the experimental configurations
Initialization of strongly coupled nuclear spins
Findings
Single defect coherence time at different transverse ZFS
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