Hq Luo

Quasiparticle heat transport in single-crystalline Ba(1-x)KxFe(2)As(2):Evidence for a k-dependent superconducting gap without nodes

The thermal conductivity

Fermi surface dichotomy of the superconducting gap and pseudogap in underdoped pnictides

\ensuremath{\kappa}

Transmission electron microscopy study of one-dimensional incommensurate structural modulation in superconducting oxides Bi2+xSr2−xCuO6+δ (0.10≤x≤0.40)

of the iron-arsenide superconductor

Measurements of the fluctuation-induced in-plane magnetoconductivity at high reduced temperatures and magnetic fields in the iron arsenide BaFe2−xNixAs2

{\text{Ba}}_{1\ensuremath{-}x}{\text{K}}_{x}{\text{Fe}}_{2}{\text{As}}_{2}({T}_{c}\ensuremath{\simeq}30\text{ }\text{K})

Observation of anisotropic diamagnetism above the superconducting transition in iron pnictide Ba 1 − x K x Fe 2 As 2 single crystals due to thermodynamic fluctuations

was measured in single crystals at temperatures down to

Evolution of Fermi surface and normal-state gap in the chemically substituted cuprates Bi2Sr2-xBixCuO6+delta

T\ensuremath{\simeq}50\text{ }\text{mK}(\ensuremath{\simeq}{T}_{c}/600)

Direct measurement of the temperature dependence of the magnetic penetration depth in Ba(Fe1−xNix)2As2 superconductors

and in magnetic fields up to

Doping evolution of the optical scattering rate and effective mass of Bi2Sr2-xLaxCuO6

H=15\text{ }\text{T}(\ensuremath{\simeq}{H}_{c2}/4)

Critical and Gaussian conductivity fluctuations in a BaFe1.9Ni0.1As2 superconductor

. A negligible residual linear term in

Anisotropic structure of the order parameter in Fese 0.45 Te 0.55 revealed by angle-resolved specific heat

\ensuremath{\kappa}/T