pith. sign in

For⟨p 2 y⟩, weproceedsimilarly, withy∈[−10L y,10L y]and∆y= ∆x

Evaluation of the in-plane moments For theHHground-state orbital, we compute ⟨p2 x⟩=ℏ 2 Z ψ(HH)∗ 0 (x) (−∂2 x)ψ (HH) 0 (x)dx ,(B2) using a uniform gridx∈[−10L x,10L x], discretized

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g-tensor Optimization in Ge/SiGe Quantum Dots

cond-mat.mes-hall · 2026-04-30 · unverdicted · novelty 4.0

A flexible optimization framework is introduced to suppress in-plane g-tensor components in SiGe-Ge-SiGe quantum wells by tuning silicon concentration, enabling gapless single-spin qubit encoding.

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  • g-tensor Optimization in Ge/SiGe Quantum Dots cond-mat.mes-hall · 2026-04-30 · unverdicted · none · ref 14

    A flexible optimization framework is introduced to suppress in-plane g-tensor components in SiGe-Ge-SiGe quantum wells by tuning silicon concentration, enabling gapless single-spin qubit encoding.