Anisotropic magnetoresistance of CeNiSn

Y. Inada; T. Ishida; H. Azuma; D. Aoki; R. Settai; Y. Onuki; K. Kobayashi; T. Takabatake; G. Nakamoto; H. Fujii; K. Maezawa

doi:10.1016/S0921-4526(96)00804-6

Anisotropic magnetoresistance of CeNiSn

Y. Inada, T. Ishida, H. Azuma, D. Aoki, R. Settai, Y. Onuki, K. Kobayashi, T. Takabatake, G. Nakamoto, H. Fujii, K. Maezawa

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

5 Citations (Scopus)

Abstract

We have measured the magnetoresistance at high fields up to 15 T and at low temperatures down to 0.4 K for CeNiSn with the orthorhombic structure. The longitudinal magnetoresistance (J∥H) is small in magnitude for the magnetic field H∥b- and c-axis. On the other hand, the positive magnetoresistance is found to become dominant with the decrease of temperature for H∥b- and c-axis in the transverse configuration (J⊥H). For H∥a, the magnetoresistance is negative for any current direction. These experimental results have been discussed on the basis of the cyclotron motion of the compensated carriers with closed Fermi surfaces and the reduction of the anisotropic hybridization gap.

Original language	English
Pages (from-to)	690-694
Number of pages	5
Journal	Physica B: Condensed Matter
Volume	230-232
DOIs	https://doi.org/10.1016/S0921-4526(96)00804-6
Publication status	Published - Feb 1997
Externally published	Yes

Keywords

CeNiSn
Hybridization gap
Magnetoresistance

ASJC Scopus subject areas

Electronic, Optical and Magnetic Materials
Condensed Matter Physics
Electrical and Electronic Engineering

Access to Document

10.1016/S0921-4526(96)00804-6

Cite this

@article{9ef3ab5396634248b8a7634079c55ac0,

title = "Anisotropic magnetoresistance of CeNiSn",

abstract = "We have measured the magnetoresistance at high fields up to 15 T and at low temperatures down to 0.4 K for CeNiSn with the orthorhombic structure. The longitudinal magnetoresistance (J∥H) is small in magnitude for the magnetic field H∥b- and c-axis. On the other hand, the positive magnetoresistance is found to become dominant with the decrease of temperature for H∥b- and c-axis in the transverse configuration (J⊥H). For H∥a, the magnetoresistance is negative for any current direction. These experimental results have been discussed on the basis of the cyclotron motion of the compensated carriers with closed Fermi surfaces and the reduction of the anisotropic hybridization gap.",

keywords = "CeNiSn, Hybridization gap, Magnetoresistance",

author = "Y. Inada and T. Ishida and H. Azuma and D. Aoki and R. Settai and Y. Onuki and K. Kobayashi and T. Takabatake and G. Nakamoto and H. Fujii and K. Maezawa",

year = "1997",

month = feb,

doi = "10.1016/S0921-4526(96)00804-6",

language = "English",

volume = "230-232",

pages = "690--694",

journal = "Physica B: Condensed Matter",

issn = "0921-4526",

publisher = "Elsevier",

}

TY - JOUR

T1 - Anisotropic magnetoresistance of CeNiSn

AU - Inada, Y.

AU - Ishida, T.

AU - Azuma, H.

AU - Aoki, D.

AU - Settai, R.

AU - Onuki, Y.

AU - Kobayashi, K.

AU - Takabatake, T.

AU - Nakamoto, G.

AU - Fujii, H.

AU - Maezawa, K.

PY - 1997/2

Y1 - 1997/2

N2 - We have measured the magnetoresistance at high fields up to 15 T and at low temperatures down to 0.4 K for CeNiSn with the orthorhombic structure. The longitudinal magnetoresistance (J∥H) is small in magnitude for the magnetic field H∥b- and c-axis. On the other hand, the positive magnetoresistance is found to become dominant with the decrease of temperature for H∥b- and c-axis in the transverse configuration (J⊥H). For H∥a, the magnetoresistance is negative for any current direction. These experimental results have been discussed on the basis of the cyclotron motion of the compensated carriers with closed Fermi surfaces and the reduction of the anisotropic hybridization gap.

AB - We have measured the magnetoresistance at high fields up to 15 T and at low temperatures down to 0.4 K for CeNiSn with the orthorhombic structure. The longitudinal magnetoresistance (J∥H) is small in magnitude for the magnetic field H∥b- and c-axis. On the other hand, the positive magnetoresistance is found to become dominant with the decrease of temperature for H∥b- and c-axis in the transverse configuration (J⊥H). For H∥a, the magnetoresistance is negative for any current direction. These experimental results have been discussed on the basis of the cyclotron motion of the compensated carriers with closed Fermi surfaces and the reduction of the anisotropic hybridization gap.

KW - CeNiSn

KW - Hybridization gap

KW - Magnetoresistance

UR - http://www.scopus.com/inward/record.url?scp=0031072661&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=0031072661&partnerID=8YFLogxK

U2 - 10.1016/S0921-4526(96)00804-6

DO - 10.1016/S0921-4526(96)00804-6

M3 - Article

AN - SCOPUS:0031072661

SN - 0921-4526

VL - 230-232

SP - 690

EP - 694

JO - Physica B: Condensed Matter

JF - Physica B: Condensed Matter

ER -

Anisotropic magnetoresistance of CeNiSn

Abstract

Keywords

ASJC Scopus subject areas

Access to Document

Other files and links

Fingerprint

Cite this