Direct coupling-induced pseudoparity nonconservation scattering: bipolar spin diode and unipolar spin entanglement pairing

The zigzag graphene nanoribbon (ZR) is characterized by the distinct pseudoparity combined with valley-selection rule, which could feature exotic transport phenomena, especially in ZR-based superconducting spintronic devices. However, the ZR with superconductivity induced by proximity of a bulk supe...

Full description

Bibliographic Details
Main Authors: Mengyao Li, Ning Bu, Jingguo Hu, Yongchun Tao, Hao Fu, Jun Wang
Format: Article
Language:English
Published: IOP Publishing 2022-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/ac8f67
_version_ 1797748446985191424
author Mengyao Li
Ning Bu
Jingguo Hu
Yongchun Tao
Hao Fu
Jun Wang
author_facet Mengyao Li
Ning Bu
Jingguo Hu
Yongchun Tao
Hao Fu
Jun Wang
author_sort Mengyao Li
collection DOAJ
description The zigzag graphene nanoribbon (ZR) is characterized by the distinct pseudoparity combined with valley-selection rule, which could feature exotic transport phenomena, especially in ZR-based superconducting spintronic devices. However, the ZR with superconductivity induced by proximity of a bulk superconductor (SC) on it still keeps original band properties. Herein, we present a superconducting heterostructure with an SC directly coupling to two ZRs, which is characteristic of pseudoparity-mixing, resulting in pseudoparity nonconservation elastic cotunneling (EC) and crossed Andreev reflection (CAR) processes. It is shown that the mixing leads to the switch effect of the EC and CAR processes manipulated by the SC length, particularly the full spin polarization. In the context of only one magnetized ZR lead, a novel bipolar spin diode behavior on a scale of small SC length and unipolar spin entanglement pairing at some large SC lengths, are both exhibited on a large scale of forward and/or reverse bias voltages. More importantly, the spin-diode can be combined with the quantum spin Hall (QSH) insulator to provide smoking gun evidence for the helical spin texture of the (QSH) insulator, which is still lacking.
first_indexed 2024-03-12T16:04:53Z
format Article
id doaj.art-b80827eb1dd841d4a12301edc61c0978
institution Directory Open Access Journal
issn 1367-2630
language English
last_indexed 2024-03-12T16:04:53Z
publishDate 2022-01-01
publisher IOP Publishing
record_format Article
series New Journal of Physics
spelling doaj.art-b80827eb1dd841d4a12301edc61c09782023-08-09T14:25:02ZengIOP PublishingNew Journal of Physics1367-26302022-01-0124909302410.1088/1367-2630/ac8f67Direct coupling-induced pseudoparity nonconservation scattering: bipolar spin diode and unipolar spin entanglement pairingMengyao Li0https://orcid.org/0000-0001-6351-3098Ning Bu1Jingguo Hu2https://orcid.org/0000-0003-3829-5177Yongchun Tao3https://orcid.org/0000-0001-5539-3815Hao Fu4https://orcid.org/0000-0002-9897-2478Jun Wang5https://orcid.org/0000-0002-6278-0677Department of Physics, Nanjing Normal University , Nanjing 210023, People’s Republic of ChinaDepartment of Physics, Nanjing Normal University , Nanjing 210023, People’s Republic of ChinaDepartment of Physics, Yangzhou University , Yangzhou 225009, People’s Republic of ChinaDepartment of Physics, Nanjing Normal University , Nanjing 210023, People’s Republic of ChinaDepartment of Physics, Nanjing Normal University , Nanjing 210023, People’s Republic of China; School of Mathematical Sciences, Nanjing Normal University , Nanjing 210023, People’s Republic of ChinaDepartment of Physics, Southeast University , Nanjing 210096, People’s Republic of ChinaThe zigzag graphene nanoribbon (ZR) is characterized by the distinct pseudoparity combined with valley-selection rule, which could feature exotic transport phenomena, especially in ZR-based superconducting spintronic devices. However, the ZR with superconductivity induced by proximity of a bulk superconductor (SC) on it still keeps original band properties. Herein, we present a superconducting heterostructure with an SC directly coupling to two ZRs, which is characteristic of pseudoparity-mixing, resulting in pseudoparity nonconservation elastic cotunneling (EC) and crossed Andreev reflection (CAR) processes. It is shown that the mixing leads to the switch effect of the EC and CAR processes manipulated by the SC length, particularly the full spin polarization. In the context of only one magnetized ZR lead, a novel bipolar spin diode behavior on a scale of small SC length and unipolar spin entanglement pairing at some large SC lengths, are both exhibited on a large scale of forward and/or reverse bias voltages. More importantly, the spin-diode can be combined with the quantum spin Hall (QSH) insulator to provide smoking gun evidence for the helical spin texture of the (QSH) insulator, which is still lacking.https://doi.org/10.1088/1367-2630/ac8f67spin entanglement pairingzigzag graphene nanoribbonvalley-selection rulespin diodeAndreev reflection
spellingShingle Mengyao Li
Ning Bu
Jingguo Hu
Yongchun Tao
Hao Fu
Jun Wang
Direct coupling-induced pseudoparity nonconservation scattering: bipolar spin diode and unipolar spin entanglement pairing
New Journal of Physics
spin entanglement pairing
zigzag graphene nanoribbon
valley-selection rule
spin diode
Andreev reflection
title Direct coupling-induced pseudoparity nonconservation scattering: bipolar spin diode and unipolar spin entanglement pairing
title_full Direct coupling-induced pseudoparity nonconservation scattering: bipolar spin diode and unipolar spin entanglement pairing
title_fullStr Direct coupling-induced pseudoparity nonconservation scattering: bipolar spin diode and unipolar spin entanglement pairing
title_full_unstemmed Direct coupling-induced pseudoparity nonconservation scattering: bipolar spin diode and unipolar spin entanglement pairing
title_short Direct coupling-induced pseudoparity nonconservation scattering: bipolar spin diode and unipolar spin entanglement pairing
title_sort direct coupling induced pseudoparity nonconservation scattering bipolar spin diode and unipolar spin entanglement pairing
topic spin entanglement pairing
zigzag graphene nanoribbon
valley-selection rule
spin diode
Andreev reflection
url https://doi.org/10.1088/1367-2630/ac8f67
work_keys_str_mv AT mengyaoli directcouplinginducedpseudoparitynonconservationscatteringbipolarspindiodeandunipolarspinentanglementpairing
AT ningbu directcouplinginducedpseudoparitynonconservationscatteringbipolarspindiodeandunipolarspinentanglementpairing
AT jingguohu directcouplinginducedpseudoparitynonconservationscatteringbipolarspindiodeandunipolarspinentanglementpairing
AT yongchuntao directcouplinginducedpseudoparitynonconservationscatteringbipolarspindiodeandunipolarspinentanglementpairing
AT haofu directcouplinginducedpseudoparitynonconservationscatteringbipolarspindiodeandunipolarspinentanglementpairing
AT junwang directcouplinginducedpseudoparitynonconservationscatteringbipolarspindiodeandunipolarspinentanglementpairing