2020
DOI: 10.1103/physrevb.102.180501
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Multichannel superconductivity of monolayer FeSe on SrTiO3 : Interplay of spin fluctuations and electron-phonon interaction

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Cited by 20 publications
(17 citation statements)
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“…These large repulsive peaks allow pairing with a sign-change across the BZ thus providing a mechanism for unconventional superconductivity in a manner similar to spin fluctuations. However, in contrast to the latter, where the small wavevector part of the repulsive interaction can interfere destructively to pairing [36][37][38], in our case the EPI remains attractive at smaller wavevectors and therefore can contribute to the unconventional pairing. We therefore conclude that the vertex-corrected EPI in all three prototypical examples is selfconsistently optimized so as to maximize the pairing.…”
mentioning
confidence: 56%
“…These large repulsive peaks allow pairing with a sign-change across the BZ thus providing a mechanism for unconventional superconductivity in a manner similar to spin fluctuations. However, in contrast to the latter, where the small wavevector part of the repulsive interaction can interfere destructively to pairing [36][37][38], in our case the EPI remains attractive at smaller wavevectors and therefore can contribute to the unconventional pairing. We therefore conclude that the vertex-corrected EPI in all three prototypical examples is selfconsistently optimized so as to maximize the pairing.…”
mentioning
confidence: 56%
“…This aspect of our approach differs from the related work in Ref. [37], and we argue it is crucial for unifying the incipient 𝑠 ± and forward-scattering e-ph scenarios described above.…”
Section: Introductionmentioning
confidence: 84%
“…Based on this evidence, it is quite likely that both spin fluctuations and e-ph coupling are relevant to the FeSe monolayers. Until recently [37], however, no studies have been carried out for this system where these two contributions are treated on an equal footing. Here, we address this question directly and study the effects of combined spin fluctuations and small-q e-ph coupling using a fully self-consistent ME + Fluctuation-Exchange (FLEX) formalism.…”
Section: Introductionmentioning
confidence: 99%
“…Here we discuss the EPI obtained by DFT calculations in Section III A and show how to calculate spinfluctuation kernels within the Random Phase Approximation (RPA) in Section III B. All calculations presented from here on, including Section IV, are carried out with the Uppsala Superconductivity (UppSC) code [41][42][43][44][45], partially with input from the Quantum Espresso package.…”
Section: Bosonic Interactionsmentioning
confidence: 99%