High magnetic field suppression of AFM in USb2_as presented
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This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore
National Laboratory under contract DE-AC52-07NA27344. Lawrence Livermore National Security, LLC
High-magnetic field suppression of
antiferromagnetism in USb2
Ryan L. Stillwell
Lawrence Livermore National Laboratory
Physical Phenomena at High Magnetic Fields VIII
Tallahassee, FL
January 7, 2016
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Outline
Why USb2?
Part One: Magnetostriction
—AFM suppression seen via fiber Bragg
dilatometer
Part Two: Magnetization
—AFM suppression confirmed via extraction
coil magnetometer
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Antiferromagnet below TN=202K
— High energy scales involved
Highly anisotropic, quasi-two
dimensional structure
U 5f-electrons are hybridized
Fermi surface reconstruction
going from paramagnetic to
antiferromagnetic phase
Introduction to USb2
D. Aoki et al., Phil. Mag. B, 80, 1517 (2000)
Paramagnetic
Antiferromagnetic
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D. Aoki et al., Phil. Mag. B, 80, 1517 (2000)
USb2 AFM unit cell is 2x the chemical unit cell
AFM unit cell
chemical unit cell
Paramagnetic
Antiferromagnetic
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Fiber Bragg dilatometer avoids eddy current
heating and enables measurements in pulsed fields
c-axis//H
1 mm a-b plane//H
Had to stack 6 crystals
a) b) c)
d)
R. Daou et al., RSI, 81, 033909 (2010)
M. Jaime et al., PNAS, 31, 12404 (2012)
A. Grockowiak, in preparation
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USb2 sample loading for extraction coil
magnetometry
Sample with c-axis coming out of the picture
Sample is ~50μm thick100μm
Compensated coils for
magnetization measurements
Sample outSample in
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Established first H-T phase diagram of USb2.
Magnetostriction and magnetization phase boundaries agree.
High-field, low-temperature magnetic state still unclear
(ie. PM or canted-AFM) due to field limitation.
Quantum oscillations to see Fermi surface above Hc?
Experiment on UBi2 to see possible Fermi surface effects.
Conclusions and Future Work