2022
DOI: 10.48550/arxiv.2201.06181
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Charge-noise induced dephasing in silicon hole-spin qubits

Ognjen Malkoc,
Peter Stano,
Daniel Loss

Abstract: We investigate theoretically charge-noise induced spin dephasing of a hole confined in a quasi-twodimensional silicon quantum dot. Central to our treatment is accounting for higher-order corrections to the Luttinger Hamiltonian. Using experimentally reported parameters, we find that the new terms give rise to sweet-spots for the hole-spin dephasing, which are sensitive to device details: dot size and asymmetry, growth direction, and applied magnetic and electric fields. Furthermore, we estimate that the dephas… Show more

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Cited by 3 publications
(4 citation statements)
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References 77 publications
(96 reference statements)
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“…For a detailed analysis of charge noise sources for hole-spin qubits in quantum dots in diamond crystal structure materials such as Si and Ge, see Ref. [79]. A detailed analysis of all noise sources in Ge NWs is of interest but is beyond the scope of the present work.…”
Section: A Qubit Operationmentioning
confidence: 99%
“…For a detailed analysis of charge noise sources for hole-spin qubits in quantum dots in diamond crystal structure materials such as Si and Ge, see Ref. [79]. A detailed analysis of all noise sources in Ge NWs is of interest but is beyond the scope of the present work.…”
Section: A Qubit Operationmentioning
confidence: 99%
“…5a), this enhancement occurs also in long quantum dots. We emphasize that, in contrast to alternative proposals where the lifetime of the qubit is enhanced only at fine-tuned sweet-spots [38][39][40], in thin Ge CQWs the qubit is to good approximation insensitive to charge noise in a wide range of E x , thus enabling highly coherent qubits with a low sensitivity to charge noise, a major issue in state-of-the-art hole spin quantum processors [14].…”
Section: B Decoherence Of the Qubitmentioning
confidence: 92%
“…This architecture not only benefits from the large SOI of hole quantum dots, which can even be reached at lower values of electric field, but it also can be designed to be free of charge noise. In striking contrast to alternative proposals to reduce the charge noise [38][39][40], in CQWs charge noise is suppressed for a wide range of electric fields and not only at fine-tuned points in parameter space, providing a critical technological advantage compared to competing architectures. This enhancement could push spin-based quantum information processing towards new speed and coherence standards.…”
Section: Introductionmentioning
confidence: 88%
“…We now briefly recap the case when there is no spinphonon interaction ( [78]). It has been shown that in the limit of large tilt field W , time evolution of any local operator O is governed by an effective Hamiltonian H s,eff = Y (D + M )Y † such that e iHst Oe −iHst ≈ e iH s,eff t Oe −iH s,eff t , where D is the projection of H s onto the space of M [39,79,80].…”
mentioning
confidence: 99%