TY - JOUR
T1 - Pressure-temperature phase diagram of the heavy-electron superconductor URu2 Si2
AU - Amitsuka, H.
AU - Matsuda, K.
AU - Kawasaki, I.
AU - Tenya, K.
AU - Yokoyama, M.
AU - Sekine, C.
AU - Tateiwa, N.
AU - Kobayashi, T. C.
AU - Kawarazaki, S.
AU - Yoshizawa, H.
N1 - Funding Information:
This work was supported, in part, by the Grant-in-Aids for the 21st Century COE “Topological Science and Technology” and for “Evolution of New Quantum Phenomena Realized in the Filled Skutterudite Structure” (no. 18027001) from the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan.
PY - 2007/3
Y1 - 2007/3
N2 - The pressure-temperature phase diagram of the heavy-electron superconductor URu2 Si2 has been reinvestigated by AC-susceptibility and elastic neutron-scattering (NS) measurements performed on a small single-crystalline rod (2 mm in diameter, 6 mm in length) in a Cu-Be clamp-type high-pressure cell (P < 1.1 GPa). At ambient pressure, this sample shows the weakest antiferromagnetic (AF) Bragg reflections reported so far, corresponding to the volume-averaged staggered moment of μo ∼ 0.011 μB / U. Under applied pressure, the AF scattering intensity exhibits a sharp increase at P ∼ 0.7 GPa at low temperatures. The saturation value of the AF scattering intensity above 0.7 GPa corresponds to μo ∼ 0.41 μB / U, which is in good agreement with that (∼ 0.39 μB / U) observed above 1.5 GPa in our previous NS measurements. The superconductivity is dramatically suppressed by the evolution of AF phase, indicating that the superconducting state coexists only with the hidden order phase. The presence of parasitic ferro- and/or antiferromagnetic phases with transition temperatures T1{star, open} = 120 (5), T2{star, open} = 36 (3) and T3{star, open} = 16.5 (5) K and their relationship to the low-T ordered phases are also discussed.
AB - The pressure-temperature phase diagram of the heavy-electron superconductor URu2 Si2 has been reinvestigated by AC-susceptibility and elastic neutron-scattering (NS) measurements performed on a small single-crystalline rod (2 mm in diameter, 6 mm in length) in a Cu-Be clamp-type high-pressure cell (P < 1.1 GPa). At ambient pressure, this sample shows the weakest antiferromagnetic (AF) Bragg reflections reported so far, corresponding to the volume-averaged staggered moment of μo ∼ 0.011 μB / U. Under applied pressure, the AF scattering intensity exhibits a sharp increase at P ∼ 0.7 GPa at low temperatures. The saturation value of the AF scattering intensity above 0.7 GPa corresponds to μo ∼ 0.41 μB / U, which is in good agreement with that (∼ 0.39 μB / U) observed above 1.5 GPa in our previous NS measurements. The superconductivity is dramatically suppressed by the evolution of AF phase, indicating that the superconducting state coexists only with the hidden order phase. The presence of parasitic ferro- and/or antiferromagnetic phases with transition temperatures T1{star, open} = 120 (5), T2{star, open} = 36 (3) and T3{star, open} = 16.5 (5) K and their relationship to the low-T ordered phases are also discussed.
KW - Antiferromagnetism
KW - Hidden order
KW - Hydrostatic pressure
KW - Superconductivity
KW - URu Si
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U2 - 10.1016/j.jmmm.2006.10.008
DO - 10.1016/j.jmmm.2006.10.008
M3 - Article
AN - SCOPUS:33847291939
SN - 0304-8853
VL - 310
SP - 214
EP - 220
JO - Journal of Magnetism and Magnetic Materials
JF - Journal of Magnetism and Magnetic Materials
IS - 2 SUPPL. PART 1
ER -