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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Published in | Chinese physics B Vol. 23; no. 12; pp. 127402 - 1-127402-5 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
01.12.2014
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Subjects | |
Online Access | Get full text |
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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. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 content type line 23 ObjectType-Feature-2 |
ISSN: | 1674-1056 1741-4199 |
DOI: | 10.1088/1674-1056/23/12/127402 |