TY - JOUR
T1 - Phase diagram and thermal expansion measurements on the system URu2-xFexSi2
AU - Ran, Sheng
AU - Wolowiec, Christian T.
AU - Jeon, Inho
AU - Pouse, Naveen
AU - Kanchanavatee, Noravee
AU - White, Benjamin D.
AU - Huang, Kevin
AU - Martien, Dinesh
AU - DaPron, Tyler
AU - Snow, David
AU - Williamsen, Mark
AU - Spagna, Stefano
AU - Riseborough, Peter S.
AU - Maple, M. Brian
N1 - Publisher Copyright:
© 2016, National Academy of Sciences. All rights reserved.
PY - 2016/11/22
Y1 - 2016/11/22
N2 - Thermal expansion, electrical resistivity, magnetization, and specific heat measurements were performed on URu2-xFexSi2 single crystals for various values of Fe concentration x in both the hidden-order (HO) and large-moment antiferromagnetic (LMAFM) regions of the phase diagram. Our results show that the paramagnetic (PM) to HO and LMAFM phase transitions are manifested differently in the thermal expansion coefficient. The uniaxial pressure derivatives of the HO/LMAFM transition temperature T0 change dramatically when crossing from the HO to the LMAFM phase. The energy gap also changes consistently when crossing the phase boundary. In addition, for Fe concentrations at xc ≈ 0.1, we observe two features in the thermal expansion upon cooling, one that appears to be associated with the transition from the PM to the HO phase and another one at lower temperature that may be due to the transition from the HO to the LMAFM phase.
AB - Thermal expansion, electrical resistivity, magnetization, and specific heat measurements were performed on URu2-xFexSi2 single crystals for various values of Fe concentration x in both the hidden-order (HO) and large-moment antiferromagnetic (LMAFM) regions of the phase diagram. Our results show that the paramagnetic (PM) to HO and LMAFM phase transitions are manifested differently in the thermal expansion coefficient. The uniaxial pressure derivatives of the HO/LMAFM transition temperature T0 change dramatically when crossing from the HO to the LMAFM phase. The energy gap also changes consistently when crossing the phase boundary. In addition, for Fe concentrations at xc ≈ 0.1, we observe two features in the thermal expansion upon cooling, one that appears to be associated with the transition from the PM to the HO phase and another one at lower temperature that may be due to the transition from the HO to the LMAFM phase.
KW - Hidden order
KW - Thermal expansion
KW - URuSi
UR - https://www.scopus.com/pages/publications/84996598726
U2 - 10.1073/pnas.1616542113
DO - 10.1073/pnas.1616542113
M3 - Article
AN - SCOPUS:84996598726
SN - 0027-8424
VL - 113
SP - 13348
EP - 13353
JO - Proceedings of the National Academy of Sciences of the United States of America
JF - Proceedings of the National Academy of Sciences of the United States of America
IS - 47
ER -