TY - JOUR
T1 - Hall coefficient and Hc2 in underdoped LaFeAsO 0.95F0.05
AU - Kohama, Y.
AU - Kamihara, Y.
AU - Riggs, S.
AU - Balakirev, F. F.
AU - Atake, T.
AU - Jaime, M.
AU - Hirano, M.
AU - Hosono, H.
N1 - Copyright:
Copyright 2011 Elsevier B.V., All rights reserved.
PY - 2008/11/1
Y1 - 2008/11/1
N2 - The electrical resistivity and Hall coefficient of LaFeAsO 0.95F0.05 polycrystalline samples were measured in pulsed magnetic fields up to μ0H=60 T from room temperature to 1.5 K. The resistance of the normal state shows a negative temperature coefficient (dρ/ dT<0) below 70 K for this composition, indicating insulating ground state in underdoped LaFeAsO system in contrast to heavily doped compound. The charge carrier density obtained from Hall effect can be described as constant plus a thermally activated term with an energy gap ΔE=630 K. The upper critical field, Hc2, estimated from resistivity measurements, exceeds 75 T with zero-field Tc=26.3 K, suggesting an unconventional nature for superconductivity.
AB - The electrical resistivity and Hall coefficient of LaFeAsO 0.95F0.05 polycrystalline samples were measured in pulsed magnetic fields up to μ0H=60 T from room temperature to 1.5 K. The resistance of the normal state shows a negative temperature coefficient (dρ/ dT<0) below 70 K for this composition, indicating insulating ground state in underdoped LaFeAsO system in contrast to heavily doped compound. The charge carrier density obtained from Hall effect can be described as constant plus a thermally activated term with an energy gap ΔE=630 K. The upper critical field, Hc2, estimated from resistivity measurements, exceeds 75 T with zero-field Tc=26.3 K, suggesting an unconventional nature for superconductivity.
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U2 - 10.1209/0295-5075/84/37005
DO - 10.1209/0295-5075/84/37005
M3 - Article
AN - SCOPUS:79051470823
SN - 0295-5075
VL - 84
JO - EPL
JF - EPL
IS - 3
M1 - 37005
ER -