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The off-diagonal part is generated by first calculating ana- lytical expressions for all matrix elements ⟨d′, m′ L, f ′ L, m′ R, f ′ R|Hhyb|d, mL, fL, mR, fR⟩

Hamiltonian generation The diagonal part of the Hamiltonian is Hdiag =ϵnQD + U nQD↑nQD↓ + g 2 X βσ f † βσ fβσ + X β Eβ c X σ f † βσ fβσ + 2mβ − n0 !2 (A1), can be read out direc

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Generalized transmon Hamiltonian for Andreev spin qubits

cond-mat.mes-hall · 2024-02-03 · unverdicted · novelty 6.0

A flat-band approximation of the Richardson model permits exact diagonalization of the generalized transmon Hamiltonian for Andreev spin qubits, simultaneously incorporating charging energy, phase fluctuations, and spin-phase coupling.

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  • Generalized transmon Hamiltonian for Andreev spin qubits cond-mat.mes-hall · 2024-02-03 · unverdicted · none · ref 6

    A flat-band approximation of the Richardson model permits exact diagonalization of the generalized transmon Hamiltonian for Andreev spin qubits, simultaneously incorporating charging energy, phase fluctuations, and spin-phase coupling.