48 research outputs found

    Magnetic and defect probes of the SmB6_6 surface state

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    The impact of non-magnetic and magnetic impurities on topological insulators is a central problem concerning their fundamental physics and possible novel spintronics and quantum computing applications. SmB6_6, predicted to be a topological Kondo insulator, is considered a benchmark material. Using a spin-polarized tip in scanning tunneling spectroscopy destroys the signature peak of the topological surface state, revealing its spin texture. Further, combining local STS with macroscopic transport measurements on SmB6_6 containing different substitutions enables us to investigate the effect of impurities. The surface states around impurities are locally suppressed with different length scales depending on their magnetic properties and, for sufficiently high impurity level, globally destroyed. Our study points directly to the topological nature of SmB6_6, and unveils, microscopically and macroscopically, how impurities -- magnetic or non-magnetic -- affect topological surface states

    Recent progress on superconductors with time-reversal symmetry breaking

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    Superconductivity and magnetism are antagonistic states of matter. The presence of spontaneous magnetic fields inside the superconducting state is, therefore, an intriguing phenomenon prompting extensive experimental and theoretical research. In this review, we discuss recent experimental discoveries of unconventional superconductors which spontaneously break time-reversal symmetry and theoretical efforts in understanding their properties. We discuss the main experimental probes and give an extensive account of theoretical approaches to understand the order parameter symmetries and the corresponding pairing mechanisms including the importance of multiple bands

    Synthesis and physical properties of Ce2_2Rh3+δ_{3+\delta}Sb4_4 single crystals

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    Millimeter-sized Ce2_2Rh3+δ_{3+\delta}Sb4_4 (δ1/8\delta\approx 1/8) single crystals were synthesized by a Bi-flux method and their physical properties were studied by a combination of electrical transport, magnetic and thermodynamic measurements. The resistivity anisotropy ρa,b/ρc2\rho_{a,b}/\rho_{c}\sim2, manifesting a quasi-one-dimensional electronic character. Magnetic susceptibility measurements confirm ab\mathbf{ab} as the magnetic easy plane. A long-range antiferromagnetic transition occurs at TN=1.4T_N=1.4 K, while clear short-range ordering can be detected well above TNT_N. The low ordering temperature is ascribed to the large Ce-Ce distance as well as the geometric frustration. Kondo scale is estimated to be about 2.4 K, comparable to the strength of magnetic exchange. Ce2_2Rh3+δ_{3+\delta}Sb4_4, therefore, represents a rare example of dense Kondo lattice whose Ruderman-Kittel-Kasuya-Yosida exchange and Kondo coupling are both weak but competing.Comment: 7 pages, 4 figures, 2 table

    Anisotropic c-f hybridization in the ferromagnetic quantum critical metal CeRh6_6Ge4_4

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    Heavy fermion compounds exhibiting a ferromagnetic quantum critical point have attracted considerable interest. Common to two known cases, i.e., CeRh6_6Ge4_4 and YbNi4_4P2_2, is that the 4f moments reside along chains with a large inter-chain distance, exhibiting strong magnetic anisotropy that was proposed to be vital for the ferromagnetic quantum criticality. Here we report an angle-resolved photoemission study on CeRh6Ge4, where we observe sharp momentum-dependent 4f bands and clear bending of the conduction bands near the Fermi level, indicating considerable hybridization between conduction and 4f electrons. The extracted hybridization strength is anisotropic in momentum space and is obviously stronger along the Ce chain direction. The hybridized 4f bands persist up to high temperatures, and the evolution of their intensity shows clear band dependence. Our results provide spectroscopic evidence for anisotropic hybridization between conduction and 4f electrons in CeRh6_6Ge4_4, which could be important for understanding the electronic origin of the ferromagnetic quantum criticality
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