Low field magnetic relaxation of superconducting C60Rb3

L. M. Wang; H. C. Yang; J. H. Hwang; C. Y. Mou; H. E. Horng

doi:10.1016/0921-4526(94)91533-4

Low field magnetic relaxation of superconducting C₆₀Rb₃

L. M. Wang, H. C. Yang, J. H. Hwang, C. Y. Mou, H. E. Horng

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

Abstract

The relaxation of magnetization M in superconducting C₆₀Rb₃ have been measured at different temperature ranges in low magnetic fields below T_c to explore the flux pinning. The measurements were performed with a superconducting quantum interference magnetometer. The applied magnetic field was 300 G - 600 G and the measured time at each temperature was 1 × 10⁴ sec. M versus 1nt shows a linear behavior for t ≥ 3600 sec. The data were analyzed in the framework of the flux pinning model of Anderson-Kim. The analyses give the activation energy of U(5K) ≈ 20 mev, and the critical current density based on J_c(T) ∝ [dM/dlnt] × [U/kT] shows J_c ∝ (1-t)^m, with the exponent m ≈ 2.0. The results are discussed.

Original language	English
Pages (from-to)	2067-2068
Number of pages	2
Journal	Physica B: Condensed Matter
Volume	194-196
Issue number	PART 2
DOIs	https://doi.org/10.1016/0921-4526(94)91533-4
Publication status	Published - Feb 2 1994
Externally published	Yes

ASJC Scopus subject areas

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

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10.1016/0921-4526(94)91533-4

Cite this

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title = "Low field magnetic relaxation of superconducting C60Rb3",

abstract = "The relaxation of magnetization M in superconducting C60Rb3 have been measured at different temperature ranges in low magnetic fields below Tc to explore the flux pinning. The measurements were performed with a superconducting quantum interference magnetometer. The applied magnetic field was 300 G - 600 G and the measured time at each temperature was 1 × 104 sec. M versus 1nt shows a linear behavior for t ≥ 3600 sec. The data were analyzed in the framework of the flux pinning model of Anderson-Kim. The analyses give the activation energy of U(5K) ≈ 20 mev, and the critical current density based on Jc(T) ∝ [dM/dlnt] × [U/kT] shows Jc ∝ (1-t)m, with the exponent m ≈ 2.0. The results are discussed.",

author = "Wang, {L. M.} and Yang, {H. C.} and Hwang, {J. H.} and Mou, {C. Y.} and Horng, {H. E.}",

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T1 - Low field magnetic relaxation of superconducting C60Rb3

AU - Wang, L. M.

AU - Yang, H. C.

AU - Hwang, J. H.

AU - Mou, C. Y.

AU - Horng, H. E.

PY - 1994/2/2

Y1 - 1994/2/2

N2 - The relaxation of magnetization M in superconducting C60Rb3 have been measured at different temperature ranges in low magnetic fields below Tc to explore the flux pinning. The measurements were performed with a superconducting quantum interference magnetometer. The applied magnetic field was 300 G - 600 G and the measured time at each temperature was 1 × 104 sec. M versus 1nt shows a linear behavior for t ≥ 3600 sec. The data were analyzed in the framework of the flux pinning model of Anderson-Kim. The analyses give the activation energy of U(5K) ≈ 20 mev, and the critical current density based on Jc(T) ∝ [dM/dlnt] × [U/kT] shows Jc ∝ (1-t)m, with the exponent m ≈ 2.0. The results are discussed.

AB - The relaxation of magnetization M in superconducting C60Rb3 have been measured at different temperature ranges in low magnetic fields below Tc to explore the flux pinning. The measurements were performed with a superconducting quantum interference magnetometer. The applied magnetic field was 300 G - 600 G and the measured time at each temperature was 1 × 104 sec. M versus 1nt shows a linear behavior for t ≥ 3600 sec. The data were analyzed in the framework of the flux pinning model of Anderson-Kim. The analyses give the activation energy of U(5K) ≈ 20 mev, and the critical current density based on Jc(T) ∝ [dM/dlnt] × [U/kT] shows Jc ∝ (1-t)m, with the exponent m ≈ 2.0. The results are discussed.

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Low field magnetic relaxation of superconducting C₆₀Rb₃

Abstract

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