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Facundo Arreyes

Publications and source records attributed to Facundo Arreyes.

5 recordsLinked to original sources

Dirac Fermion Scattering and Pseudospin Polarization in Structurally Asymmetric Graphene Wormholes

We study the quantum transport of massless Dirac fermions through two asymptotically flat graphene sheets connected by a structurally asymmetric catenoid wormhole in $(2+1)$-dimensional curved spacetime. Analytic scattering basis functions are derived: Hankel functions of integer order (in the half-flux sector) in the flat sheets and Gauss hypergeometric functions in the curved throat. We construct a transfer matrix via piecewise numerical matching, verifying unitarity up to numerical precision. The transmission probability rises monotonically to unity at high energies. Global transmission exhibits mirror degeneracy under inversion of structural asymmetry, but local observables depend on incidence direction. The manifold's spin connection acts as a Hermitian coupling inducing an $A/B$ sublattice imbalance at the throat. Structural asymmetry induces a local pseudospin imbalance. A larger curvature radius enhances $P_z$ polarization via a larger geometric phase; abrupt incidence suppresses it. Sub-barrier modes exhibit a negative transmission phase time, compatible with Hartman-type wave-packet reshaping.

cond-mat.mes-hall

Entanglement (1+2) QED in a double layer of Dirac Materials

We investigate the momentum-space entanglement between two Dirac quasiparticles in a double-layer honeycomb lattice coupled via a planar electromagnetic cavity. We model the low-energy excitations as massive Dirac fermions in $(1+2)$ dimensions and derive the Bethe-Salpeter equation using the ladder approximation. We use a Born-level approximation around a free two-body quasiparticle state, where the interaction is mediated by the cavity photon propagator. From the reduced sublattice density matrix, we compute a momentum-resolved von Neumann entropy. Within the perturbatively controlled regime, the entropy remains small, while phenomenological self-energy dressing drives a crossover to strong enhancement of the entanglement entropy. Stationary entanglement is obtained only when the quasiparticle coherence time exceeds the photon propagation time between the layers. The maximum-entropy regime appears to be a viable method for achieving Bell-like states. These results demonstrate how self-energy renormalization, virtual particle exchange, and spinor geometry combine to reshape the entanglement landscape of Dirac materials.

quant-ph

Entanglement formation in two-dimensional materials within microcavity

In this work, the entanglement generation between two hexagonal-lattice layers embedded in a microcavity is studied, accounting for both electromagnetic coupling and intrinsic spin-orbit interaction (SOI). Utilizing a short-time dynamical approach, we perform a perturbative Taylor expansion of the reduced density matrix to characterize the bipartite quantum correlations between the hexagonal layers. We demonstrate that the system undergoes a rapid transition from a localized product state in the conduction bands at t = 0 to a coherent superposition of valence and conduction band states. Our results indicate that the degree of entanglement is highly sensitive to the interlayer photon propagator, which contains the geometric ratios of the layer positions and the height cavity, and the specific Fermi energy and SOI signatures of the respective layers. We show the emergence of spacelike-separated quantum correlations in the ultra-short evolution regime, suggesting that heterostructures in cavities may be suitable to develop experiments for a deep understanding of spacelike-separated quantum effects.

quant-ph

Entanglement harvesting in buckled honeycomb lattices by vacuum fluctuations in a microcavity

We study the entanglement harvesting between two identical buckled honeycomb lattices placed inside a planar microcavity. By applying time dependent perturbation theory, we obtain quantum correlations between both layers induced by the cavity field. Considering the vacuum state as the initial state of the cavity field and tracing out the time-evolved degrees of freedom, we analyze the entanglement formation using the concurrence measure. We show that the concurrence depends on the virtual photon exchanged and the positions of the layer through the interlayer photon propagator. Furthermore, we find that the formation of entanglement between equal energy electrons tends to be enhanced when they move in perpendicular directions. Our results indicate that a buckled honeycomb structure and a large spin-orbit interaction favor the entanglement harvesting.

cond-mat.mes-hall

Coulomb drag between two graphene layers at different temperatures

We theoretically study the Coulomb drag in graphene when there is a temperature difference between the layers. Within the degenerate limit for equal layer densities, we find that this can lead to significant deviations from the usual quadratic temperature dependence of the drag resistivity. The exact behavior depends strongly on the phase space available for intraband scattering, and is not symmetrical when the temperatures of the layers are interchanged. In particular, when one layer is at a much higher temperature $T$ than the other, the drag resistivity behaves as $ρ_D\sim T/d^5$, where $d$ is the interlayer separation. The magnitude of the drag in this limit is always larger when the active layer is at the higher temperature.

cond-mat.mes-hall