Low-Temperature Specific Heat ofYBa2Cu3O7−

Evidence of nodal superconductivity inNa0.35CoO2·1.3H2Yang1, Lin2, Sun3 et al. 2005Phys. Rev. B637530View full textAdd to dashboardCite

“…This allows one to reliably analyze in field data. dependence is a manifestation of nodal line order parameter and has been observed in HTSC's [13][14][15][16] and Sr 2 RuO 4 [25,26]. The dashed line is a fit of data for H≤0.5T to [14,32] and H c2 //c=4 T is taken from Fig.…”

Depression of Quasiparticle Density of States at Zero Energy inLa1.9Sr0.1Cu1−Chang1, Lin2, Yang3 2000Phys. Rev. Lett.

“…There are now at least two questions remaining controversial. One is the extended quasiparticle states and quasiparticle transport in the mixed state [1][2][3], which has been intensively studied by the methods like the thermal conductivity [4,5] and specific heat [6][7][8][9]. The other is the quasiparticle density of states in the presence of impurities or disorders.…”

Effect of controlled disorder on quasiparticle thermal transport inBi2Sr2CaCuNakamae1, Behnia2, Balicas3 et al. 2001Phys. Rev. B4312601View full textAdd to dashboardCite

“…Subsequently, Chiao et al [4] found a quantitative agreement between this gap structure as deduced from thermal conductivity and the one directly observed by ARPES studies [8] in optimally-doped Bi2212. On the other hand, data on electronic specific heat [9][10][11] and penetration depth [12,13] are limited to T >2K and probe excitations within a higher energy interval where the density of states is a linear function of energy. The temperature dependence of electronic specific heat in Y123 is in agreement with theoretical expectations for the gap structure near the nodes [4,11].…”