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Anomalous magnetoresistance by breaking ice rule in Bi2Ir2O7/Dy2Ti2O7 heterostructure

delete2023-03-14
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OA
AI
H
Han Zhang
C
Chengkun Xing
K
Kyle Noordhoek
Z
Zhaoyu Liu
T
Tianhao Zhao
L
Lukáš Horák
Q
Qing Huang
L
Lin Hao
J
Junyi Yang
S
Shashi Pandey
E
Elbio Dagotto
Z
Zhigang Jiang
J
Jiun‐Haw Chu
Y
Yan Xin
E
Eun Sang Choi
H
Haidong Zhou *
刘健 cover
刘健 (Jian Liu)
DOI:10.1038/s41467-023-36886-2delete
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Abstract

Abstract

En 中文
While geometrically frustrated quantum magnets host rich exotic spin states with potentials for revolutionary quantum technologies, most of them are necessarily good insulators which are difficult to be integrated with modern electrical circuit. The grand challenge is to electrically detect the emergent fluctuations and excitations by introducing charge carriers that interact with the localized spins without destroying their collective spin states. Here, we show that, by designing a Bi2Ir2O7/Dy2Ti2O7 heterostructure, the breaking of the spin-ice rule in insulating Dy2Ti2O7 leads to a charge response in the conducting Bi2Ir2O7 measured as anomalous magnetoresistance during the field-induced Kagome ice-to-saturated ice transition. The magnetoresistive anomaly also captures the characteristic angular and temperature dependence of this ice-rule-breaking transition, which has been understood as magnetic monopole condensation. These results demonstrate a novel heteroepitaxial approach for electronically probing the transition between exotic insulating spin states, laying out a blueprint for the metallization of frustrated quantum magnets. Spin ice compounds are typically insulating and introducing carriers can destroy the spin ice state, making integration into electronic devices problematic. Here the authors report a transport response to an ice-rule-breaking transition in a heterostructure of a pyrochlore spin ice and a nonmagnetic metal.
Keywords:
MAGNETIC MONOPOLE
SPIN ICE
DYNAMICS
STATE
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Nature Communications
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15.7
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Georgia Institute of Technology
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University of Washington
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University of Tennessee System
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