arXiv:2309.05741 · Physical review. B./Physical review. B
Conductance and thermopower fluctuations in interacting quantum dots
Henry Shackleton, Laurel E. Anderson, Philip Kim, Subir Sachdev A
Abstract
We model an interacting quantum dot of electrons by a Hamiltonian with random and all-to-all single-particle hopping (of root-mean-square strength $t$) and two-particle interactions (of root-mean-square strength $J$). For $t\ensuremath{\ll}J$, such a model has a regime exhibiting the nonquasiparticle physics of the Sachdev-Ye-Kitaev (SYK) model at temperatures ${E}_{\mathrm{coh}}\ensuremath{\ll}T\ensuremath{\ll}J$, and that of a renormalized Fermi liquid at $T\ensuremath{\ll}{E}_{\mathrm{coh}}$, where ${E}_{\mathrm{coh}}={t}^{2}/J$. Extending earlier work has computed the mean thermoelectric properties of such a dot weakly coupled to two external leads, we compute the sample-to-sample fluctuations in the conductance and thermopower of such a dot, and describe several distinct regimes. In all cases, the effect of the SYK interactions is to reduce the strength of the sample-to-sample fluctuations. We also find that in the regime where the mean transport coefficients are determined only by the value of $J$ at leading order, the sample-to-sample fluctuations can be controlled by the influence of the smaller $t$.