Magnetoresistance of under high magnetic fields parallel to the conducting plane

E. Ohmichi, Y. Maeno, S. Nagai, Zhiqiang Mao, M. Tanatar, T. Ishiguro

Research output: Contribution to journalArticle

16 Citations (Scopus)

Abstract

The interplane resistivity (Formula presented) and in-plane resistivity (Formula presented) of the layered superconductor (Formula presented) were studied at 50 mK under magnetic fields B up to 33 T applied parallel to the conducting plane. The superconductivity recurrence predicted theoretically was not observed for either (Formula presented) or (Formula presented) in magnetic fields up to 33 T. In the normal-state transverse magnetoresistance of (Formula presented) a pronounced anisotropy was found within the conducting plane. A sharp resistance peak with an apex in the direction of the parallel field and a superlinear field dependence at the peak were observed with a magnetic field in the  direction, while this peak was absent with a magnetic field parallel to the  direction. The results are discussed in terms of the in-plane anisotropy of the interplane transfer energy (Formula presented) For (Formula presented) the longitudinal magnetoresistance with the current both in the  and  directions increased notably, which is incompatible with semiclassical behavior.

Original language English (US) 7101-7107 7 Physical Review B - Condensed Matter and Materials Physics 61 10 https://doi.org/10.1103/PhysRevB.61.7101 Published - Jan 1 2000

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Magnetoresistance
Magnetic fields
conduction
magnetic fields
Anisotropy
Superconductivity
Energy transfer
Superconducting materials
anisotropy
electrical resistivity
Direction compound
apexes
superconductivity
energy transfer

All Science Journal Classification (ASJC) codes

• Electronic, Optical and Magnetic Materials
• Condensed Matter Physics

Cite this

Ohmichi, E. ; Maeno, Y. ; Nagai, S. ; Mao, Zhiqiang ; Tanatar, M. ; Ishiguro, T. / Magnetoresistance of under high magnetic fields parallel to the conducting plane. In: Physical Review B - Condensed Matter and Materials Physics. 2000 ; Vol. 61, No. 10. pp. 7101-7107.
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abstract = "The interplane resistivity (Formula presented) and in-plane resistivity (Formula presented) of the layered superconductor (Formula presented) were studied at 50 mK under magnetic fields B up to 33 T applied parallel to the conducting plane. The superconductivity recurrence predicted theoretically was not observed for either (Formula presented) or (Formula presented) in magnetic fields up to 33 T. In the normal-state transverse magnetoresistance of (Formula presented) a pronounced anisotropy was found within the conducting plane. A sharp resistance peak with an apex in the direction of the parallel field and a superlinear field dependence at the peak were observed with a magnetic field in the  direction, while this peak was absent with a magnetic field parallel to the  direction. The results are discussed in terms of the in-plane anisotropy of the interplane transfer energy (Formula presented) For (Formula presented) the longitudinal magnetoresistance with the current both in the  and  directions increased notably, which is incompatible with semiclassical behavior.",
author = "E. Ohmichi and Y. Maeno and S. Nagai and Zhiqiang Mao and M. Tanatar and T. Ishiguro",
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Magnetoresistance of under high magnetic fields parallel to the conducting plane. / Ohmichi, E.; Maeno, Y.; Nagai, S.; Mao, Zhiqiang; Tanatar, M.; Ishiguro, T.

In: Physical Review B - Condensed Matter and Materials Physics, Vol. 61, No. 10, 01.01.2000, p. 7101-7107.

Research output: Contribution to journalArticle

TY - JOUR

T1 - Magnetoresistance of under high magnetic fields parallel to the conducting plane

AU - Ohmichi, E.

AU - Maeno, Y.

AU - Nagai, S.

AU - Mao, Zhiqiang

AU - Tanatar, M.

AU - Ishiguro, T.

PY - 2000/1/1

Y1 - 2000/1/1

N2 - The interplane resistivity (Formula presented) and in-plane resistivity (Formula presented) of the layered superconductor (Formula presented) were studied at 50 mK under magnetic fields B up to 33 T applied parallel to the conducting plane. The superconductivity recurrence predicted theoretically was not observed for either (Formula presented) or (Formula presented) in magnetic fields up to 33 T. In the normal-state transverse magnetoresistance of (Formula presented) a pronounced anisotropy was found within the conducting plane. A sharp resistance peak with an apex in the direction of the parallel field and a superlinear field dependence at the peak were observed with a magnetic field in the  direction, while this peak was absent with a magnetic field parallel to the  direction. The results are discussed in terms of the in-plane anisotropy of the interplane transfer energy (Formula presented) For (Formula presented) the longitudinal magnetoresistance with the current both in the  and  directions increased notably, which is incompatible with semiclassical behavior.

AB - The interplane resistivity (Formula presented) and in-plane resistivity (Formula presented) of the layered superconductor (Formula presented) were studied at 50 mK under magnetic fields B up to 33 T applied parallel to the conducting plane. The superconductivity recurrence predicted theoretically was not observed for either (Formula presented) or (Formula presented) in magnetic fields up to 33 T. In the normal-state transverse magnetoresistance of (Formula presented) a pronounced anisotropy was found within the conducting plane. A sharp resistance peak with an apex in the direction of the parallel field and a superlinear field dependence at the peak were observed with a magnetic field in the  direction, while this peak was absent with a magnetic field parallel to the  direction. The results are discussed in terms of the in-plane anisotropy of the interplane transfer energy (Formula presented) For (Formula presented) the longitudinal magnetoresistance with the current both in the  and  directions increased notably, which is incompatible with semiclassical behavior.

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