On-Demand and Tunable Andreev Conversion of Single-Electron Charge Pulses

Electron quantum optics explores coherent single-electron charge pulse propagation in electronic nanoscale circuits akin to tabletop photon setups. While past experiments focused on normal-state conductors, incorporating superconductors holds promise for exploiting the electron-hole degree of freedo...

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Detalles Bibliográficos
Autores: Burset, Pablo, Roussel, Benjamin, Moskalets, Michael, Flindt, Christian
Tipo de recurso: artículo
Estado:Versión enviada para evaluación y publicación
Fecha de publicación:2025
País:España
Institución:Consejo Superior de Investigaciones Científicas (CSIC)
Repositorio:DIGITAL.CSIC. Repositorio Institucional del CSIC
OAI Identifier:oai:dnet:digitalcsic_::2aba736994f88e88d16f2ac5bf70c3c3
Acceso en línea:http://hdl.handle.net/10261/426655
http://arxiv.org/abs/2312.13145v2
Access Level:acceso abierto
Palabra clave:Andreev reflection
Hall effect
Quantum interference effects
Quantum transport
Single-electron devices
Bogoliubov-de Gennes equations
S-matrix method in transport
Descripción
Sumario:Electron quantum optics explores coherent single-electron charge pulse propagation in electronic nanoscale circuits akin to tabletop photon setups. While past experiments focused on normal-state conductors, incorporating superconductors holds promise for exploiting the electron-hole degree of freedom in quantum sensing applications and quantum information processing. Here, we propose and analyze an on-demand and tunable mechanism for converting single-electron pulses into holes through Andreev processes on a superconductor. We develop a Floquet-Nambu scattering formalism to demonstrate the dynamic conversion of charge pulses and the controllable generation of coherent electron-hole superpositions through interferometric magnetic flux control based on the chiral edge states of a quantum Hall sample. Our discussion covers optimal conditions in realistic scenarios, affirming the feasibility of our proposal with current technology.