TY - JOUR
T1 - Normal and superconducting state properties of U6Fe at low temperatures and high magnetic fields
AU - Delong, L. E.
AU - Crabtree, G. W.
AU - Hall, L. N.
AU - Kierstead, H.
AU - Aoki, H.
AU - Dhar, S. K.
AU - Gschneidner, K. A.
AU - Junod, A.
PY - 1985/12/2
Y1 - 1985/12/2
N2 - High purity U6Fe polycrystals with a resistance ratio rrr=9 at T=4 K are found to exhibit a record onset temperature (T0 > 4.0 K) to superconductivity for U materials. Our measured values of the electronic coefficient of heat capacity γ*=(150±3) mJ/mol · K2, the mean Debye temperature Θ(T→0)=166 K and the normalized jump in heat capacity at Tc, Δ/γTc=2.3±0.1, are all in good agreement with previous work† † L.E Delong et al.Physics.Rev.Lett.51(1983)312., and suggest that U6Fe is a strong-coupled superconductor. Resistive upper critical field measurements on high purity samples revealed a pronounced S-shaped curvature of Hc2(T) and evidence for anisotropy, similar to effects seen in UPt3‡ † L.E Delong et al.Physics.Rev.Lett.51(1983)312., but not observed in lower purity U6Fe samples† † L.E Delong et al.Physics.Rev.Lett.51(1983)312.. We find Hc2(0) > 10T and transition widths ΔTc∝H 1 2 at moderate fields, followed by an abrupt increase in ΔTc for H>8T. Our Hc2 data cannot be explained by existing theoretical models. Preliminary heat capacity measurements in magnetic fields 0≤H≤10T suggest that γ* may decrease by ≈10% at H=10 T. These results and electrical resistivity data will be discussed in terms of a potential charge density wave instability in U6Fe at T{less-than or approximate}110 K.
AB - High purity U6Fe polycrystals with a resistance ratio rrr=9 at T=4 K are found to exhibit a record onset temperature (T0 > 4.0 K) to superconductivity for U materials. Our measured values of the electronic coefficient of heat capacity γ*=(150±3) mJ/mol · K2, the mean Debye temperature Θ(T→0)=166 K and the normalized jump in heat capacity at Tc, Δ/γTc=2.3±0.1, are all in good agreement with previous work† † L.E Delong et al.Physics.Rev.Lett.51(1983)312., and suggest that U6Fe is a strong-coupled superconductor. Resistive upper critical field measurements on high purity samples revealed a pronounced S-shaped curvature of Hc2(T) and evidence for anisotropy, similar to effects seen in UPt3‡ † L.E Delong et al.Physics.Rev.Lett.51(1983)312., but not observed in lower purity U6Fe samples† † L.E Delong et al.Physics.Rev.Lett.51(1983)312.. We find Hc2(0) > 10T and transition widths ΔTc∝H 1 2 at moderate fields, followed by an abrupt increase in ΔTc for H>8T. Our Hc2 data cannot be explained by existing theoretical models. Preliminary heat capacity measurements in magnetic fields 0≤H≤10T suggest that γ* may decrease by ≈10% at H=10 T. These results and electrical resistivity data will be discussed in terms of a potential charge density wave instability in U6Fe at T{less-than or approximate}110 K.
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U2 - 10.1016/0378-4363(85)90441-3
DO - 10.1016/0378-4363(85)90441-3
M3 - Article
AN - SCOPUS:0022228122
SN - 0378-4363
VL - 135
SP - 81
EP - 85
JO - Physica B: Physics of Condensed Matter & C: Atomic, Molecular and Plasma Physics, Optics
JF - Physica B: Physics of Condensed Matter & C: Atomic, Molecular and Plasma Physics, Optics
IS - 1-3
ER -