TY - JOUR
T1 - Zooming on the quantum critical point in Nd-LSCO
AU - Cyr-Choinire, Olivier
AU - Daou, R.
AU - Chang, J.
AU - Laliberté, Francis
AU - Doiron-Leyraud, Nicolas
AU - Leboeuf, David
AU - Jo, Y. J.
AU - Balicas, L.
AU - Yan, J. Q.
AU - Cheng, J. G.
AU - Zhou, J. S.
AU - Goodenough, J. B.
AU - Taillefer, Louis
PY - 2010/12
Y1 - 2010/12
N2 - Recent studies of the high-Tc superconductor La 1.6-xNd0.4SrxCuO4 (Nd-LSCO) have found a linear-T in-plane resistivity ρab and a logarithmic temperature dependence of the thermopower S/T at a hole doping p=0.24 and a Fermi-surface reconstruction just below p=0.24 [1,2]. These are typical signatures of a quantum critical point (QCP). Here we report data on the c-axis resistivity ρc(T) of Nd-LSCO measured as a function of temperature near this QCP, in a magnetic field large enough to entirely suppress superconductivity. Like ρab,ρc shows an upturn at low temperature, a signature of Fermi surface reconstruction caused by stripe order. Tracking the height of the upturn as it decreases with doping enables us to pin down the precise location of the QCP where stripe order ends, at p=0.235±0.005. We propose that the temperature Tρ below which the upturn begins marks the onset of the pseudogap phase, found to be roughly twice as high as the stripe-ordering temperature in this material.
AB - Recent studies of the high-Tc superconductor La 1.6-xNd0.4SrxCuO4 (Nd-LSCO) have found a linear-T in-plane resistivity ρab and a logarithmic temperature dependence of the thermopower S/T at a hole doping p=0.24 and a Fermi-surface reconstruction just below p=0.24 [1,2]. These are typical signatures of a quantum critical point (QCP). Here we report data on the c-axis resistivity ρc(T) of Nd-LSCO measured as a function of temperature near this QCP, in a magnetic field large enough to entirely suppress superconductivity. Like ρab,ρc shows an upturn at low temperature, a signature of Fermi surface reconstruction caused by stripe order. Tracking the height of the upturn as it decreases with doping enables us to pin down the precise location of the QCP where stripe order ends, at p=0.235±0.005. We propose that the temperature Tρ below which the upturn begins marks the onset of the pseudogap phase, found to be roughly twice as high as the stripe-ordering temperature in this material.
KW - C-Axis electrical resistivity
KW - La-based cuprates
KW - Nd-LSCO
KW - Quantum critical point
KW - Superconductivity
UR - http://www.scopus.com/inward/record.url?scp=78649696979&partnerID=8YFLogxK
U2 - 10.1016/j.physc.2009.11.073
DO - 10.1016/j.physc.2009.11.073
M3 - Article
AN - SCOPUS:78649696979
SN - 0921-4534
VL - 470
SP - S12-S13
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - SUPPL.1
ER -