The Charge Transport in Minimal Kitaev Chain

The quantum transport is investigated in minimal Kitaev chain coupled to normal metal leads. The exact formulas of the charge current I and the conductance G are exhibited using the nonequilibrium Greens function approach. For simplify, the cases of asymmetric and symmetric bias voltage, the charge current, and the conductance G are presented at zero temperature. For asymmetric bias, due to the crossed Andreev reflection, the current and conductance are asymmetric. However, there is not crossed Andreev reflection in the case of symmetrically applied bias voltage. The current and conductance are symmetric about bias voltage eV = 0. In both cases, as the system's parameters ε L , ε R , and t , Δ satisfy the relation ε L ε R = t 2 −Δ 2 , there are zero‐bias peaks, which is known as poor man's Majoranas. A zero magnitude of nonlocal conductance Δ G NL , along with a flip in the sign of Δ G NL , is observed. The gap of Δ G NL must close and reopen, signaling a topological phase transition.

Authors

Institutions

Publication Details

Journal
physica status solidi (b)
Published
2025-12-26
DOI
https://doi.org/10.1002/pssb.202500525
Primary Topic
Topological Materials and Phenomena
Type
article
Field-Weighted Citation Impact
0.00

Funders

Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

The Charge Transport in Minimal Kitaev Chain

Fa‐Li Chong, Nuo‐Wei Li, Wei‐Ke Zou
physica status solidi (b)
Topological Materials and Phenomena
article

The Charge Transport in Minimal Kitaev Chain

Fa‐Li Chong, Nuo‐Wei Li, Wei‐Ke Zou
article en

Abstract

The quantum transport is investigated in minimal Kitaev chain coupled to normal metal leads. The exact formulas of the charge current I and the conductance G are exhibited using the nonequilibrium Greens function approach. For simplify, the cases of asymmetric and symmetric bias voltage, the charge current, and the conductance G are presented at zero temperature. For asymmetric bias, due to the crossed Andreev reflection, the current and conductance are asymmetric. However, there is not crossed Andreev reflection in the case of symmetrically applied bias voltage. The current and conductance are symmetric about bias voltage eV = 0. In both cases, as the system's parameters ε L , ε R , and t , Δ satisfy the relation ε L ε R = t 2 −Δ 2 , there are zero‐bias peaks, which is known as poor man's Majoranas. A zero magnitude of nonlocal conductance Δ G NL , along with a flip in the sign of Δ G NL , is observed. The gap of Δ G NL must close and reopen, signaling a topological phase transition.

physica status solidi (b)Vol. 263(1)
Xuzhou University of Technology (CN)
Government of Jiangsu Province, Beijing Institute of Technology
Openalex Percentile: Top 31%
Topological Materials and Phenomena
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.