2023
DOI: 10.1103/physreva.108.023307
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Momentum-resolved Floquet-engineered pair and single-particle filter in the Fermi-Hubbard model

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Cited by 2 publications
(4 citation statements)
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“…5. The general result shows similar features as the result obtained for non-resonant driving, especially the almost periodic structure that appears for large λ (see discussion in [25,26]). However, the most important difference is that for λ → 0 the impurity does not become fully transparent, but instead shows finite transmission and reflection.…”
Section: G3 Computation Of the Pair Transmissionsupporting
confidence: 80%
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“…5. The general result shows similar features as the result obtained for non-resonant driving, especially the almost periodic structure that appears for large λ (see discussion in [25,26]). However, the most important difference is that for λ → 0 the impurity does not become fully transparent, but instead shows finite transmission and reflection.…”
Section: G3 Computation Of the Pair Transmissionsupporting
confidence: 80%
“…by writing all quantities as matrices (note that W ′ 0 is also a symmetric hopping and thus, in this context, proportional to A even ): Note that this result does not depend on δu which is a consequence of the fact that for α → 0 scattering in P is independent from the details in subspace Q. Interestingly, Eq. (G.27) equals the result one would obtain by first studying the limit α → 0 for |u| not close to an integer using the Floquet-Schrieffer-Wolff transformation (see [25,26]) and then sending |u| → |u 0 | to an integer. We give a plot of the pair transmission for |u 0 | = 1 in Fig.…”
Section: G3 Computation Of the Pair Transmissionmentioning
confidence: 58%
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