TY - JOUR
T1 - Quantum critical metamagnetism of Sr3Ru2O7 under hydrostatic pressure
AU - Wu, W.
AU - McCollam, A.
AU - Grigera, S. A.
AU - Perry, R. S.
AU - MacKenzie, A. P.
AU - Julian, S. R.
PY - 2011/1/25
Y1 - 2011/1/25
N2 - Using ac susceptibility, we have determined the pressure dependence of the metamagnetic critical endpoint temperature T⊃* for a field applied in the ab plane in the itinerant metamagnet Sr3Ru2O 7. We find that T⊃* falls monotonically to zero as pressure increases, producing a quantum critical endpoint (QCEP) at P c~13.6±0.2kbar. New features are observed near the QCEP-the slope of T⊃* versus pressure changes at ~12.8 kbar, and weak subsidiary maxima appear on either side of the main susceptibility peak at pressures near Pc-indicating that some new physics comes into play near the QCEP. Clear signatures of a nematic phase, however, that were seen in field-angle tuning of T⊃* are not observed. As T⊃* is suppressed by pressure, the metamagnetic peak in the susceptibility remains sharp as a function of an applied magnetic field. As a function of temperature, however, the peak becomes broad with only a very weak maximum, suggesting that, near the QCEP, the uniform magnetization density is not the order parameter for the metamagnetic transition.
AB - Using ac susceptibility, we have determined the pressure dependence of the metamagnetic critical endpoint temperature T⊃* for a field applied in the ab plane in the itinerant metamagnet Sr3Ru2O 7. We find that T⊃* falls monotonically to zero as pressure increases, producing a quantum critical endpoint (QCEP) at P c~13.6±0.2kbar. New features are observed near the QCEP-the slope of T⊃* versus pressure changes at ~12.8 kbar, and weak subsidiary maxima appear on either side of the main susceptibility peak at pressures near Pc-indicating that some new physics comes into play near the QCEP. Clear signatures of a nematic phase, however, that were seen in field-angle tuning of T⊃* are not observed. As T⊃* is suppressed by pressure, the metamagnetic peak in the susceptibility remains sharp as a function of an applied magnetic field. As a function of temperature, however, the peak becomes broad with only a very weak maximum, suggesting that, near the QCEP, the uniform magnetization density is not the order parameter for the metamagnetic transition.
UR - https://www.scopus.com/pages/publications/79551640641
U2 - 10.1103/PhysRevB.83.045106
DO - 10.1103/PhysRevB.83.045106
M3 - Article
AN - SCOPUS:79551640641
SN - 1098-0121
VL - 83
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 4
M1 - 045106
ER -