Coexistence of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2
arXiv:1407.3711 · doi:10.1103/PhysRevB.91.014508
Abstract
Through the combination of X-ray diffraction, electrical transport, magnetic susceptibility, and the heat capacity measurements, we studied the effect of Ce doping in the newly discovered SrFBiS system. It is found that SrCeFBiS undergoes a second-order transition below $7.5 K, followed by a superconducting transition with the critical temperature Tc=2.8 K. Our transport, specific heat and DC-magnetization results suggest the presence of bulk ferromagneticcorrelation of Ce ion below 7.5 K that coexist with superconductivity when the temperature is further lowered below 2.8 K.
6 pages, 5 figures
References in corpus (10)
- Pressure induced superconductivity in CaFeAs
- Superconductivity Appears in the Vicinity of an Insulating-Like Behavior in CeOFBiS
- Superconductivity induced by phosphorus doping and its coexistence with ferromagnetism in EuFe(AsP)
- Superconductivity of F-substituted LnOBiS2 (Ln = La, Ce, Pr, Nd, Yb) compounds
- Ferroelectric Soft Phonons, Charge Density Wave Instability and Strong Electron-Phonon Coupling in BiS2-Layered Superconductors
- Superconductivity induced by La doping in Sr1-xLaxFBiS2 system
- CeRuPO: A rare example of a Ferromagnetic Kondo lattice
- CeFePO: A Heavy Fermion Metal with Ferromagnetic Correlations
- RPA Analysis of a Two-orbital Model for the BiS2-based Superconductors
- The crystalline electric field as a probe for long range antiferromagnetic order and superconductivity in CeFeAsOF
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- Bulk Superconductivity Induced by Se Substitution in BiCh2-Based Layered Compounds Eu0.5Ce0.5FBiS2-xSex
- Mn-doping induced ferromagnetism and enhanced superconductivity in Bi_4-x Mn_x O_4 S_3 (0.075 < = x < = 0.15)