Magneto-resistance and vortex phase diagram of BaNi sub(0.1)Fe sub(1.9)As sub(2) single crystal

The transition from vortex glass to a liquid phase is studied in BaNi sub(0.1)Fe sub(1.9)As sub(2) single crystal with T sub(c) = 19.4 K by magneto-resistance measurements. The resistivity curves are measured in magnetic fields in a range of 0 T-13 T for H || c and H[perpendicular]c. Good scalings f...

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Bibliographic Details
Published inChinese physics B Vol. 23; no. 12; pp. 127402 - 1-127402-5
Main Authors Lu, Jun-Chao, Yu, Yi, Pi, Li, Zhang, Yu-Heng
Format Journal Article
LanguageEnglish
Published 01.12.2014
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Summary:The transition from vortex glass to a liquid phase is studied in BaNi sub(0.1)Fe sub(1.9)As sub(2) single crystal with T sub(c) = 19.4 K by magneto-resistance measurements. The resistivity curves are measured in magnetic fields in a range of 0 T-13 T for H || c and H[perpendicular]c. Good scalings for all values of resistivity [rho](H,T) and the effective pinning potential U sub(0)(H,T) are obtained with the modified vortex glass theory by using the critical exponents s and H sub(0). Phase diagrams for H || c and H[perpendicular]c are determined based on the obtained vortex glass temperature T sub(g), the vortex dimensionality crossover temperature T*, and the upper critical magnetic field H sub(c2). Our results suggest that both below and above 5 T. single vortex pinning co-exists with collective creep, and collective creep is dominant. There is a narrower vortex liquid region for H[perpendicular]c than for H || c in the vortex phase diagram, which may originate from a stronger pinning force.
Bibliography:ObjectType-Article-1
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content type line 23
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ISSN:1674-1056
1741-4199
DOI:10.1088/1674-1056/23/12/127402