Microwave surface impedance in overdoped Tl2Ba2CuO6+δ

Koichi Izawa; Akinori Shibata; Hidekazu Takahashi; Yuji Matsuda; Masashi Hasegawa; Noriko Chikumoto; C. J. Van Der Beek; Marcin Konczykowski

doi:10.1016/S0921-4526(99)02263-2

Microwave surface impedance in overdoped Tl₂Ba₂CuO_6+δ

Koichi Izawa
, Akinori Shibata
, Hidekazu Takahashi
, Yuji Matsuda
, Masashi Hasegawa
, Noriko Chikumoto
, C. J. Van Der Beek
, Marcin Konczykowski

École Polytechnique

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

Abstract

The microwave surface impedance Z_s = R_s + iX_S and transmittivity T′_H of overdoped Tl₂Ba₂CuO_6+δ have been measured in a magnetic field up to 7 T in order to clarify the unusual temperature dependence of the DC resistivetransition field H* From the result of T′_H, columnar defects enhance H*, indicating that H* is the melting point of vortices instead of the mean field H_c2. The field dependence of R_s is found to be unusual as compared with that expected from the result of the DC resistivity.

Original language	English
Pages (from-to)	945-946
Number of pages	2
Journal	Physica B: Physics of Condensed Matter
Volume	284-288
Issue number	PART I
DOIs	https://doi.org/10.1016/S0921-4526(99)02263-2
Publication status	Published - 1 Jan 2000

Keywords

Microwave surface impedance
Transmittivity
Upper critical field

Access to Document

10.1016/S0921-4526(99)02263-2

Cite this

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title = "Microwave surface impedance in overdoped Tl2Ba2CuO6+δ",

abstract = "The microwave surface impedance Zs = Rs + iXS and transmittivity T′H of overdoped Tl2Ba2CuO6+δ have been measured in a magnetic field up to 7 T in order to clarify the unusual temperature dependence of the DC resistivetransition field H* From the result of T′H, columnar defects enhance H*, indicating that H* is the melting point of vortices instead of the mean field Hc2. The field dependence of Rs is found to be unusual as compared with that expected from the result of the DC resistivity.",

keywords = "Microwave surface impedance, Transmittivity, Upper critical field",

author = "Koichi Izawa and Akinori Shibata and Hidekazu Takahashi and Yuji Matsuda and Masashi Hasegawa and Noriko Chikumoto and \{Van Der Beek\}, \{C. J.\} and Marcin Konczykowski",

year = "2000",

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doi = "10.1016/S0921-4526(99)02263-2",

language = "English",

volume = "284-288",

pages = "945--946",

journal = "Physica B: Physics of Condensed Matter",

issn = "0921-4526",

number = "PART I",

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TY - JOUR

T1 - Microwave surface impedance in overdoped Tl2Ba2CuO6+δ

AU - Izawa, Koichi

AU - Shibata, Akinori

AU - Takahashi, Hidekazu

AU - Matsuda, Yuji

AU - Hasegawa, Masashi

AU - Chikumoto, Noriko

AU - Van Der Beek, C. J.

AU - Konczykowski, Marcin

PY - 2000/1/1

Y1 - 2000/1/1

N2 - The microwave surface impedance Zs = Rs + iXS and transmittivity T′H of overdoped Tl2Ba2CuO6+δ have been measured in a magnetic field up to 7 T in order to clarify the unusual temperature dependence of the DC resistivetransition field H* From the result of T′H, columnar defects enhance H*, indicating that H* is the melting point of vortices instead of the mean field Hc2. The field dependence of Rs is found to be unusual as compared with that expected from the result of the DC resistivity.

AB - The microwave surface impedance Zs = Rs + iXS and transmittivity T′H of overdoped Tl2Ba2CuO6+δ have been measured in a magnetic field up to 7 T in order to clarify the unusual temperature dependence of the DC resistivetransition field H* From the result of T′H, columnar defects enhance H*, indicating that H* is the melting point of vortices instead of the mean field Hc2. The field dependence of Rs is found to be unusual as compared with that expected from the result of the DC resistivity.

KW - Microwave surface impedance

KW - Transmittivity

KW - Upper critical field

U2 - 10.1016/S0921-4526(99)02263-2

DO - 10.1016/S0921-4526(99)02263-2

M3 - Article

AN - SCOPUS:0033699823

SN - 0921-4526

VL - 284-288

SP - 945

EP - 946

JO - Physica B: Physics of Condensed Matter

JF - Physica B: Physics of Condensed Matter

IS - PART I