Ishida S, Nakajima M, Liang T, Kihou K, Lee C H, Iyo A, Eisaki H, Kakeshita T, Tomioka Y, Ito T, Uchida S
Department of Physics, University of Tokyo, Tokyo 113-0033, Japan and National Institute of Advanced Industrial Science and Technology, Tsukuba 305-8568, Japan and JST, Transformative Research-Project on Iron Pnictides, Tokyo 102-0075, Japan.
National Institute of Advanced Industrial Science and Technology, Tsukuba 305-8568, Japan and JST, Transformative Research-Project on Iron Pnictides, Tokyo 102-0075, Japan.
Phys Rev Lett. 2013 May 17;110(20):207001. doi: 10.1103/PhysRevLett.110.207001. Epub 2013 May 13.
We investigated the in-plane resistivity anisotropy for underdoped Ba(Fe(1-x)Co(x))(2)As(2) single crystals with improved quality. We demonstrate that the anisotropy in resistivity in the magnetostructural ordered phase arises from the anisotropy in the residual component which increases in proportion to the Co concentration x. This gives evidence that the anisotropy originates from the impurity scattering by Co atoms substituted for the Fe sites, rather than the so far proposed mechanisms such as the anisotropy of Fermi velocities of reconstructed Fermi surface pockets. As doping proceeds to the paramagnetic-tetragonal phase, a Co impurity transforms to a weak and isotropic scattering center.
我们研究了质量有所提高的欠掺杂Ba(Fe(1 - x)Co(x))(2)As(2)单晶的面内电阻率各向异性。我们证明,磁结构有序相中的电阻率各向异性源于残余分量的各向异性,该残余分量与Co浓度x成比例增加。这证明了各向异性源于取代Fe位点的Co原子的杂质散射,而非迄今所提出的机制,如重构费米面口袋的费米速度各向异性。随着掺杂进入顺磁四方相,Co杂质转变为弱且各向同性的散射中心。