arXiv subjects

Alexander Kruchkov

Publications and source records attributed to Alexander Kruchkov.

14 recordsLinked to original sources

arXiv2025

Quantum correlations curvature, memory functions, and fundamental bounds

We investigate fundamental bounds on the curvature of quantum correlation functions in imaginary time. Focusing first on topological phases, we show that quantum geometry can qualitatively modify the imaginary-time decay of correlations, leading to nontrivial curvature behavior beyond simple exponential scaling. More generally, we show a universal bound on correlation curvature that holds for interacting systems in thermal equilibrium, and establish connection to leading invariants of the memory-function formalism. Our results identify imaginary-time curvature as a robust probe of intrinsic quantum timescales.

quant-ph↗

arXiv2025

Topological control of quantum speed limits

Quantum Fisher Information (QFI) is a measure quantifying the sensitivity of a quantum state with respect to changes in tuning parameters in quantum metrology, and defining quantum speed limits. We show that even if the quantum state is completely dispersionless, QFI in this state remains momentum-resolved. We compute the QFI for topological phases at integer filling and demonstrate that each momentum-resolved term is fundamentally bounded by quantum geometric and topological invariants, with maximum QFI controlled by topological invariants (Chern number $|C|$). We also finds bounds on quantum speed limit which scales as $\sqrt{|C|}$ in a (dispersionless) topological phase. We conclude that quantum platforms of high Chern numbers $|C| \gg 1$, such as those featuring twisted multilayered van der Waals heterostructures, significantly enhance capacity for quantum Fisher information, and provide practical control over quantum speed limits.

quant-ph↗

arXiv2024

Entanglement entropy in lattice models with quantum metric

We revisit the connection between entanglement entropy and quantum metric in topological lattice systems, and provide an elegant and concise proof of this connection. In gapped two-dimensional lattice models with well-defined tight-binding Hamiltonians, we show that the entanglement entropy is intimately related to the quantum metric of electronic states.

cond-mat.str-el↗

arXiv2024

Magneto-Thermoelectric Transport in Graphene Quantum Dot with Strong Correlations

Disorder at the etched edges of graphene quantum dots (GQD) enables random all-to-all interactions between localized charges in partially-filled Landau levels, providing a potential platform to realize the Sachdev-Ye-Kitaev (SYK) model. We use quantum Hall edge states in the graphene electrodes to measure electrical conductance and thermoelectric power across the GQD. We observe a rapid diminishing of electric conductance fluctuations and slowly decreasing thermoelectric power across the GQD with increasing temperature, consistent with recent theoretical predictions for the SYK regime.

cond-mat.mes-hall↗

arXiv2023

Spectral sum rules reflect topological and quantum-geometric invariants

Topological invariants are fundamental characteristics reflecting global properties of quantum systems, yet their exploration has predominantly been limited to the static (DC) transport and transverse (Hall) channel. In this work, we extend the spectral sum rules for frequency-resolved electric conductivity $\sigma (\omega)$ in topological systems, and show that the sum rule for the longitudinal channel is expressed through topological and quantum-geometric invariants. We find that for dispersionless (flat) Chern bands, the rule is expressed as, $ \int_{-\infty}^{+\infty} d\omega \, \text{Re}(\sigma_{xx} + \sigma_{yy}) = C \Delta e^2$, where $C$ is the Chern number, $\Delta$ the topological gap, and $e$ the electric charge. In scenarios involving dispersive Chern bands, the rule is defined by the invariant of the quantum metric, and Luttinger invariant, $\int_{-\infty}^{+\infty} d\omega \, \text{Re}(\sigma_{xx} + \sigma_{yy}) = 2 \pi e^2 \Delta \sum_{\boldsymbol{k}} \text{Tr} \, \mathcal{G}_{ij}(\boldsymbol{k})$+(Luttinger invariant), where $\text{Tr} \, \mathcal {G}_{ij}$ is invariant of the Fubini-Study metric (defining spread of Wannier orbitals). We further discuss the physical role of topological and quantum-geometric invariants in spectral sum rules. Our approach is adaptable across varied topologies and system dimensionalities.

cond-mat.str-el↗

arXiv2023

Noise probing of topological band gaps in dispersionless quantum states

We uncover a useful connection between the integrated current noise $S(\omega)$ and the topological band gap in dispersionless quantum states, $\int d \omega [ \mathcal S^{\text{flat}}_{xx} + \mathcal S^{\text{flat}}_{yy} ] = C e^2 \Delta^2$ (in units $\hbar$$=$$1$), where $C$ is the Chern number, $e$ is electric charge, and $\Delta$ is the topological band gap. This relationship may serve as a working principle for a new experimental probe of topological band gaps in flat band materials. Possible applications include moir\'e systems, such as twisted bilayer graphene and twisted transition metal dichalcogenides, where a band gap measurement in meV regime presents an experimental challenge.

cond-mat.str-el↗

arXiv2023

Unconventional superfluidity and quantum geometry of topological bosons

We investigate superfluidity of bosons in gapped topological bands and discover a new phase that has no counterparts in the previous literature. This phase is characterized by a highly unconventional modulation of the order parameter, breaking the crystallographic symmetry, and for which the condensation momentum is neither zero nor any other high-symmetry vector of the Brillouin zone. This unconventional structure impacts the spectrum of Bogoliubov excitations and, consequently, the speed of sound in the system. Even in the case of perfectly flat bands, the speed of sound and Bogoliubov excitations remain nonvanishing, provided that the underlying topology and quantum geometry are nontrivial. Furthermore, we derive detailed expressions for the superfluid weight using the Popov hydrodynamic formalism for superfluidity and provide estimates for the Berezinskii-Kosterlitz-Thouless temperature, which is significantly enhanced by the nontriviality of the underlying quantum metric. These results are applicable to generic topological bosonic bands, with or without dispersion. To illustrate our findings, we employ the Haldane model with a tunable bandwidth, including the narrow lowest-band case. Within this model, we also observe a re-entrant superfluid behavior: As the Haldane's magnetic flux is varied, the Berezinskii-Kosterlitz-Thouless transition temperature initially decreases to almost zero, only to resurface with renewed vigor.

cond-mat.quant-gas↗

arXiv2023

Anomalous conductivity of $\mathcal{PT}$-symmetric Fermi liquids

We consider a non-Hermitian yet $\mathcal{PT}$-symmetric Fermi liquid ($\mathcal{PT}$-FL) in external electric fields. Due to $\mathcal{PT}$-symmetry, the system exhibits real spectrum, Fermi surface and electric conductivity are well-defined through propagators. We find that, in contrast to the conventional Fermi liquids (FL), the $\mathcal{PT}$-FL can exhibit a zero resistance state in the longitudinal ($xx$) channel. Moreover, the temperature dependence of the resistivity anomaly violates the conventional FL scaling (it is not limited by $T^2$). These findings open route to further exploration of transport anomalies beyond the conventional paradigm.

cond-mat.str-el↗

arXiv2022

Quantum transport in dispersionless electronic bands

Flat electronic bands are counterintuitive: with the electron velocity vanishing, our conventional notions of quasiparticle transport are no longer valid. We here study the quantum transport in the generalized families of perfectly flat bands [PRB 105, L241102 (2022)], and find that while the conventional contributions indeed vanish, the quantum-geometric contribution gives rise to the enhanced electronic transport. This contribution is connected to the Wannier orbital quantization in the perfectly flat bands, and is present only for geometrically-nontrivial bands (for example, flat Chern bands). We find similar expressions for thermal conductance, thermoelectric response, and superfluid weight in the flat bands. In particular, we report the anomalous thermopower associated with flat topological bands reaching values as large as $\frac{k_B}{e}\ln 2$$\approx$60 $\mu$V/k, the quantum unit of thermopower, not expected in conventional dispersive bands.

cond-mat.str-el↗

arXiv2022

Engineering SYK interactions in disordered graphene flakes under realistic experimental conditions

We model SYK (Sachdev-Ye-Kitaev) interactions in disordered graphene flakes up to 300 000 atoms ($\sim$100 nm in diameter) subjected to an out-of-plane magnetic field $B$ of 5-20 Tesla within the tight-binding formalism. We investigate two sources of disorder: (i) irregularities at the system boundaries, and (ii) bulk vacancies, -- for a combination of which we find conditions which could be favorable for the formation of the phase with SYK features under realistic experimental conditions above the liquid helium temperature.

cond-mat.str-el↗

arXiv2022

Re-entrant magic-angle phenomena in twisted bilayer graphene in integer magnetic fluxes

In this work we address the re-entrance of magic-angle phenomena (band flatness and quantum-geometric transport) in twisted bilayer graphene (TBG) subjected to strong magnetic fluxes $\pm \Phi_0$, $\pm 2 \Phi_0$, $\pm 3 \Phi_0$... ($\Phi_0 = h/e$ is the flux quantum per moir\'e cell). The moir\'e translation invariance is restored at the integer fluxes, for which we calculate the TBG band structure using accurate atomistic models with lattice relaxations. Similarly to the zero-flux physics outside the magic angle condition, the reported effect breaks down rapidly with the twist. We conclude that the magic-angle physics re-emerges in high magnetic fields, witnessed by the appearance of flat electronic bands distinct from Landau levels, and manifesting non-trivial quantum geometry. We further discuss the possible flat-band quantum geometric contribution to the superfluid weight in strong magnetic fields (28 T at 1.08$^\circ$ twist), according to Peotta-T\"{o}rm\"{a} mechanism.

cond-mat.mes-hall↗

arXiv2021

Unconventional Flat Chern Bands and 2$e$ Charges in Skyrmionic Moiré Superlattices

The interplay of topological characteristics in real space and reciprocal space can lead to the emergence of unconventional topological phases. In this Letter, we implement a novel mechanism for generating higher-Chern flat bands on the basis of twisted bilayer graphene (TBG) coupled to topological magnetic structures in the form of the skyrmion lattice. In particular, we discover a scenario for generating $|C|=2$ dispersionless electronic bands when the skyrmion periodicity and the moiré periodicity are matched. Following the Wilczek argument, the statistics of the charge-carrying excitations in this case is \textit{bosonic}, characterized by electronic charge $Q =2e$, that is \textit{even} in units of electron charge $e$. The required skyrmion coupling strength triggering the topological phase transition is realistic, with its threshold estimated as low as 4~meV. The Hofstadter butterfly spectrum of this phase is different resulting in an unexpected quantum Hall conductance sequence $\pm \frac{2 e^2}{h}, \ \pm \frac{4 e^2}{h}, ...$ for TBG with skyrmion order.

cond-mat.str-el↗

arXiv2021

Origin of band flatness and constraints of higher Chern numbers

Flat bands provide a natural platform for emergent electronic states beyond Landau paradigm. Among those of particular importance are flat Chern bands, including bands of higher Chern numbers ($C$$>$$1$). We introduce a new framework for band flatness through wave functions, and classify the existing isolated flat bands in a "periodic table" according to tight binding features and wave function properties. Our flat band categorization encompasses seemingly different classes of flat bands ranging from atomic insulators to perfectly flat Chern bands and Landau Levels. The perfectly flat Chern bands satisfy Berry curvature condition $F_{xy} = \text{Tr} \, \mathcal G_{ij}$ which on the tight-binding level is fulfilled only for infinite-range models. Most of the natural Chern bands fall into category of $C=1$; the complexity of creating higher-$C$ flat bands is beyond the current technology. This is due to the breakdown of the microscopic stability for higher-$C$ flatness, seen atomistically e.g. in the increase of the hopping range bound as $\propto$$\sqrt{C} a$. Within our new formalism, we indicate strategies for bypassing higher-$C$ constraints and thus dramatically decreasing the implementation complexity.

cond-mat.str-el↗

arXiv2020

Thermoelectric power of Sachdev-Ye-Kitaev islands: Probing Bekenstein-Hawking entropy in quantum matter experiments

The Sachdev-Ye-Kitaev (SYK) model describes electrons with random and all-to-all interactions, and realizes a many-body state without quasiparticle excitations, and a non-vanishing extensive entropy $S_0$ in the zero temperature limit. Its low energy theory coincides the low energy theory of the near-extremal charged black holes with Bekenstein-Hawking entropy $S_0$. Several mesoscopic experimental configurations realizing SYK quantum dynamics over a significant intermediate temperature scale have been proposed. We investigate quantum thermoelectric transport in such configurations, and describe the low temperature crossovers out of SYK criticality into regimes with either Fermi liquid behavior, a Coulomb blockade, or criticality associated with Schwarzian quantum gravity fluctuations. Our results show that thermopower measurements can serve as a direct probe for $S_0$.

cond-mat.str-el↗