Evolution of magnetism and superconductivity in CeCu2(Si1−xGex)2
O. Trovarelli, M. Weiden, R. Müller-Reisener, M. Gómez-Berisso, P. Gegenwart, M. Deppe, C. Geibel, J. G. Sereni, F. Steglich
DOI 10.1103/PhysRevB.56.678 · Physical Review B
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Abstract
We have determined the magnetic phase diagram of CeCu2(Si1−xGex)2 using specific heat, susceptibility, and resistivity measurements and additional thermal expansion and muon spin resonance experiments. The system evolves continuously from the heavy-fermion state at x=0 to an antiferromagnetically (AF) ordered state at x=1, though the magnetic structure undergoes significant modifications. The results strongly suggest that the AF ordering emerges from the A phase of pure CeCu2Si2. The phase diagram can be divided into three regions: Low Ge content (x<~0.2) leads to an enhancement of the A phase of pure CeCu2Si2 and to a moderate decrease of the Kondo temperature. Despite this increase of the magnetic character, we could observe superconductivity up to x=0.1. At large Ge content (x>0.5) the behavior resembles that of pure CeCu2Ge2. The intermediate region is characterized by the appearance of a second magnetic transition below TN, which seems to be of first-order type. The appearance of this transition leads to a well-defined critical point at x=0.3 and suggests the possibility of another critical point at x≃0.5.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| CeCu2Si2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.7 | Pressure unresolved | unknown |
| CeCu2Ge2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | 7 GPa | unknown |
| CeCu2(Si1-xGex)2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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