Tunneling picture of interlayer magnetotransport in multilayer systems

Toshihito Osada; Masahiko Kuraguchi; Kaya Kobayashi; Eiji Ohmichi

doi:10.1016/S1386-9477(02)00965-7

Tunneling picture of interlayer magnetotransport in multilayer systems

Toshihito Osada, Masahiko Kuraguchi, Kaya Kobayashi, Eiji Ohmichi

Research output: Contribution to journal › Conference article › peer-review

13 Citations (Scopus)

Abstract

Interlayer magnetotransport of multilayer systems has been generally studied. In multilayer systems with weak interlayer coupling, interlayer conduction is mainly dominated by single tunneling process between neighboring layers. The selection rule and probability of single interlayer tunneling are controlled by orientation and strength of magnetic fields. This tunneling model gives the most general explanation of most of the magnetoresistance angular effects observed in Q2D or Q1D layered conductors. The existence of the Fermi surface is not necessary for appearance of them. This model can also be applied to the modified angular effects under strong electric fields.

Original language	English
Pages (from-to)	200-201
Number of pages	2
Journal	Physica E: Low-Dimensional Systems and Nanostructures
Volume	18
Issue number	1-3
DOIs	https://doi.org/10.1016/S1386-9477(02)00965-7
Publication status	Published - May 1 2003
Externally published	Yes
Event	23rd International Conference on Low Temperature Physics - Hiroshima, Japan Duration: Aug 20 2002 → Aug 27 2002

Keywords

Angular-dependent magnetoresistance oscillations
Incoherent transport
Interlayer tunneling
Low-dimensional conductor

ASJC Scopus subject areas

Electronic, Optical and Magnetic Materials
Atomic and Molecular Physics, and Optics
Condensed Matter Physics

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10.1016/S1386-9477(02)00965-7

Cite this

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title = "Tunneling picture of interlayer magnetotransport in multilayer systems",

abstract = "Interlayer magnetotransport of multilayer systems has been generally studied. In multilayer systems with weak interlayer coupling, interlayer conduction is mainly dominated by single tunneling process between neighboring layers. The selection rule and probability of single interlayer tunneling are controlled by orientation and strength of magnetic fields. This tunneling model gives the most general explanation of most of the magnetoresistance angular effects observed in Q2D or Q1D layered conductors. The existence of the Fermi surface is not necessary for appearance of them. This model can also be applied to the modified angular effects under strong electric fields.",

keywords = "Angular-dependent magnetoresistance oscillations, Incoherent transport, Interlayer tunneling, Low-dimensional conductor",

author = "Toshihito Osada and Masahiko Kuraguchi and Kaya Kobayashi and Eiji Ohmichi",

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doi = "10.1016/S1386-9477(02)00965-7",

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pages = "200--201",

journal = "Physica E: Low-Dimensional Systems and Nanostructures",

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note = "23rd International Conference on Low Temperature Physics ; Conference date: 20-08-2002 Through 27-08-2002",

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TY - JOUR

T1 - Tunneling picture of interlayer magnetotransport in multilayer systems

AU - Osada, Toshihito

AU - Kuraguchi, Masahiko

AU - Kobayashi, Kaya

AU - Ohmichi, Eiji

PY - 2003/5/1

Y1 - 2003/5/1

N2 - Interlayer magnetotransport of multilayer systems has been generally studied. In multilayer systems with weak interlayer coupling, interlayer conduction is mainly dominated by single tunneling process between neighboring layers. The selection rule and probability of single interlayer tunneling are controlled by orientation and strength of magnetic fields. This tunneling model gives the most general explanation of most of the magnetoresistance angular effects observed in Q2D or Q1D layered conductors. The existence of the Fermi surface is not necessary for appearance of them. This model can also be applied to the modified angular effects under strong electric fields.

AB - Interlayer magnetotransport of multilayer systems has been generally studied. In multilayer systems with weak interlayer coupling, interlayer conduction is mainly dominated by single tunneling process between neighboring layers. The selection rule and probability of single interlayer tunneling are controlled by orientation and strength of magnetic fields. This tunneling model gives the most general explanation of most of the magnetoresistance angular effects observed in Q2D or Q1D layered conductors. The existence of the Fermi surface is not necessary for appearance of them. This model can also be applied to the modified angular effects under strong electric fields.

KW - Angular-dependent magnetoresistance oscillations

KW - Incoherent transport

KW - Interlayer tunneling

KW - Low-dimensional conductor

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DO - 10.1016/S1386-9477(02)00965-7

M3 - Conference article

AN - SCOPUS:0038518537

SN - 1386-9477

VL - 18

SP - 200

EP - 201

JO - Physica E: Low-Dimensional Systems and Nanostructures

JF - Physica E: Low-Dimensional Systems and Nanostructures

IS - 1-3

T2 - 23rd International Conference on Low Temperature Physics

Y2 - 20 August 2002 through 27 August 2002

ER -

Tunneling picture of interlayer magnetotransport in multilayer systems

Abstract

Keywords

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