The Static Skin Effect in Bismuth. I

Masatsugu Suzuki; Sei ichi Tanuma

doi:10.1143/JPSJ.44.1539

The Static Skin Effect in Bismuth. I

Masatsugu Suzuki
, Sei ichi Tanuma

Physics

Binghamton University

The University of Tokyo

Research output: Contribution to journal › Article › peer-review

7 Scopus citations

Abstract

The transverse magneto-resistance of bismuth was measured at 1.5 K in magnetic fields up to 24 kOe. It became clear from the experimental results that the electric current is forced out towards one side surface of the sample in a certain configuration. The peculiar feature of this surface current is that the current path shifts to the opposite side surface with the reversal of the magnetic field but it remains unchanged with the reversal of DC current. The latter effect could not be understood in terms of ordinary static skin effect.

Original language	English
Pages (from-to)	1539-1546
Number of pages	8
Journal	Journal of the Physical Society of Japan
Volume	44
Issue number	5
DOIs	https://doi.org/10.1143/JPSJ.44.1539
State	Published - 1978

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10.1143/JPSJ.44.1539

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title = "The Static Skin Effect in Bismuth. I",

abstract = "The transverse magneto-resistance of bismuth was measured at 1.5 K in magnetic fields up to 24 kOe. It became clear from the experimental results that the electric current is forced out towards one side surface of the sample in a certain configuration. The peculiar feature of this surface current is that the current path shifts to the opposite side surface with the reversal of the magnetic field but it remains unchanged with the reversal of DC current. The latter effect could not be understood in terms of ordinary static skin effect.",

author = "Masatsugu Suzuki and Tanuma, \{Sei ichi\}",

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N2 - The transverse magneto-resistance of bismuth was measured at 1.5 K in magnetic fields up to 24 kOe. It became clear from the experimental results that the electric current is forced out towards one side surface of the sample in a certain configuration. The peculiar feature of this surface current is that the current path shifts to the opposite side surface with the reversal of the magnetic field but it remains unchanged with the reversal of DC current. The latter effect could not be understood in terms of ordinary static skin effect.

AB - The transverse magneto-resistance of bismuth was measured at 1.5 K in magnetic fields up to 24 kOe. It became clear from the experimental results that the electric current is forced out towards one side surface of the sample in a certain configuration. The peculiar feature of this surface current is that the current path shifts to the opposite side surface with the reversal of the magnetic field but it remains unchanged with the reversal of DC current. The latter effect could not be understood in terms of ordinary static skin effect.

UR - https://www.scopus.com/pages/publications/77952855274

U2 - 10.1143/JPSJ.44.1539

DO - 10.1143/JPSJ.44.1539

M3 - Article

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VL - 44

SP - 1539

EP - 1546

JO - Journal of the Physical Society of Japan

JF - Journal of the Physical Society of Japan

IS - 5

ER -

The Static Skin Effect in Bismuth. I

Abstract

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