Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Simulating electron spin entanglement in a double quantum dot

Rodriguez-Moreno, A. D. Hernández de la Luz, Lilia Meza-Montes

Published Mar 23, 2011• 0 citations
OpenAlex

Related papers

Information driven double quantum-dot engine fueled by entanglement between electron spins

Martin Josefsson, Martin Leijnse

Bulletin of the American Physical Society•Mar 16, 2021•0 citations

Entanglement of two interacting electrons in a double quantum dot

Ping Zhang, Xiang‐Gui Li, Xian-Geng Zhao

arXiv:cond-mat/0210254•Physics Letters A•Feb 1, 2002•4 citations

Nonequilibrium electron spin polarization in a double quantum dot: Lande mechanism

Yuri A. Serebrennikov

In moderately strong magnetic fields, the difference in Land\'e $g$ factors in each of the dots of a two-electron double quantum dot (DQD) may induce oscillations between singlet and triplet states of an entangled pair and lead to a nonequilibrium electron spin polarization in the system. The calculated bipolar polarization reflects the strong spin correlation in the spatially separated pair of electrons that occupy almost degenerate states in a coupled DQD. We will show that this polarization may partially survive the rapid inhomogeneous decoherence caused by random nuclear magnetic fields.

arXiv:cond-mat/0508566•Physical Review B•Jul 20, 2006•3 citations

Double quantum dot turnstile as an electron spin entangler

Xuedong Hu, S. Das Sarma

We study the conditions for a double quantum dot system to work as a reliable electron spin entangler and the efficiency of a beam splitter as a detector for the resulting entangled electron pairs. In particular, we focus on the relative strengths of the tunneling matrix elements, the applied bias and gate voltage, the necessity of time-dependent input/output barriers, and the consequence of considering wave packet states for the electrons as they leave the double dot to enter the beam splitter. We show that a double quantum dot turnstile is, in principle, an efficient electron spin entangler or entanglement filter because of the exchange coupling between the dots and the tunable input/output potential barriers, provided certain conditions are satisfied in the experimental setup.

arXiv:cond-mat/0307024•Physical Review B•Mar 12, 2004•31 citations

Double Quantum Dot as a Filter for Spin Entanglement

Xuedong Hu, S. Das Sarma

APS•Mar 1, 2004•0 citations

Entanglement of two interacting electrons in a driven double quantum dot structure

John Boviatsis, Evangelos Voutsinas, Antonios Fountoulakis

Superlattices and Microstructures•Apr 25, 2007•12 citations
In moderately strong magnetic fields, the difference in Land\'e ggg factors in each of the dots of a two-electron double quantum dot (DQD) may induce oscillations between singlet and triplet states of an entangled pair and lead to a nonequilibrium electron spin polarization in the system. The calculated bipolar polarization reflects the strong spin correlation in the spatially separated pair of electrons that occupy almost degenerate states in a coupled DQD. We will show that this polarization may partially survive the rapid inhomogeneous decoherence caused by random nuclear magnetic fields.
We study the conditions for a double quantum dot system to work as a reliable electron spin entangler and the efficiency of a beam splitter as a detector for the resulting entangled electron pairs. In particular, we focus on the relative strengths of the tunneling matrix elements, the applied bias and gate voltage, the necessity of time-dependent input/output barriers, and the consequence of considering wave packet states for the electrons as they leave the double dot to enter the beam splitter. We show that a double quantum dot turnstile is, in principle, an efficient electron spin entangler or entanglement filter because of the exchange coupling between the dots and the tunable input/output potential barriers, provided certain conditions are satisfied in the experimental setup.