Journal of the Physical Society of Japan · 2005 · 11 citations · 16 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsElectronic MaterialsMagnetic MaterialsMagnetic Properties Of SolidsMagnetic SusceptibilityMagnetism In SolidsPhase TransitionsSemiconducting MaterialsStrongly Correlated Electron SystemsActivationElectrical ResistivityHall ConductivityHall EffectMagnetic Phase TransitionsSpecific Heat CapacitySuperconducting Gap
Magnetic, transport and specific-heat measurements of Ce 1- x La x RhAs ( x ≤0.1) have been performed. The host compound CeRhAs undergoes successive phase transitions with formation of superlattices at T 1 =360, T 2 =235, and T 3 =165 K, respectively. The transitions at T 1 and T 3 are associated with the formation of a wide gap of E g1 / k B =2200 K and a narrow one of E g2 / k B =310 K, respectively. All anomalies at T 1 , which are a jump in the specific heat C , a drop in the magnetic susceptibility χ and the activation-type behavior in the Hall coefficient, remain until x is increased up to 0.10, at which T 1 is depressed to 297 K. These observations indicate that both the phase transition at T 1 and the gap of E g1 remain up to x =0.10. Anomalies in C and χ at T 2 and T 3 , on the other hand, vanish at a small concentration x =0.01. The semiconducting behavior in both the electrical resistivity and thermopower below T 3 also disappears at x =0.02. These facts corroborate that the narrow gap of E g2 is quenched when the phase transition at T 3 disappears. The distinct effects on the phase transitions in Ce 1- x La x RhAs and CeRhAs 1- y Sb y indicate that coherent hybridization between Rh 4 d and As 4 p states is important for the formation of E g1 below T 1 .
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Ce- and Yb-based Kondo semiconductors
T. Takabatake, F. Iga, Takashi Yoshino et al. · Journal of Magnetism and Magnetic Materials · 1998 · 161 citations