2018
DOI: 10.1038/s41598-018-34991-7
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Magnetic field driven complex phase diagram of antiferromagnetic heavy-fermion superconductor Ce3PtIn11

Abstract: We present the results of our comprehensive investigation on the antiferromagnetic heavy-fermion superconductor Ce3PtIn11 carried out by means of electrical transport, heat capacity and ac magnetic susceptibility measurements, performed on single-crystalline specimens down to 50 mK in external magnetic fields up to 9 T. Our experimental results elucidate a complex magnetic field – temperature phase diagram which contains both first- and second-order field-induced magnetic transitions and highlights the emergen… Show more

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Cited by 25 publications
(36 citation statements)
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“…The detailed synthesis process and preliminary characterization data are reported elsewhere [28]. The sample contains a partial parasitic phase of CeIn 3 (less than 5%-10%) but has a fairly sharp superconducting transition at T c 0.33 K and two antiferromagnetic transitions at T N1 = 2.2 K and T N2 = 2.0 K, in agreement with the literature data [18,21]. For NQR measurements, the sample was fine powdered in order to reduce the heating-up effect at low temperatures and improve the NQR signal intensity.…”
Section: Methodssupporting
confidence: 83%
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“…The detailed synthesis process and preliminary characterization data are reported elsewhere [28]. The sample contains a partial parasitic phase of CeIn 3 (less than 5%-10%) but has a fairly sharp superconducting transition at T c 0.33 K and two antiferromagnetic transitions at T N1 = 2.2 K and T N2 = 2.0 K, in agreement with the literature data [18,21]. For NQR measurements, the sample was fine powdered in order to reduce the heating-up effect at low temperatures and improve the NQR signal intensity.…”
Section: Methodssupporting
confidence: 83%
“…Even in the antiferromagnetic state, they exhibit superconductivity below T c = 0.32 K (M = Pt) and 0.42 K (M = Pd) [19,20]. In each material, a further metamagnetic transition occurs in a high magnetic field [21,22]. This suggests that the coexistence of antiferromagnetism and superconductivity in the Ce 3 MIn 11 compounds is quite a unique phenomenon driven by the hybridization between f electrons of Ce ions and conduction electrons [23].…”
Section: Introductionmentioning
confidence: 98%
“…Although, one should notice that MR(H) follows a linear dependence without any dendency of a saturation at higher fields, which is quite unusual as regards heavy-fermion AFM systems. It is also worth to emphasize that similar behavior has previously been observed only in a few such systems, including Ce3TmIn11 (Tm= Pt and Pd) [30,31] and Ce2PdGa12 [37], yet its actual origin remains unclear.…”
Section: Resultssupporting
confidence: 62%
“…In this context it is noteworthy to mention Ce3TmIn11 (n=3, m=1 and Tm=Pt, Pd) in particular, as it turns out to be quite a unique example where superconductivity coexists with AFM ordered state with a pressure induced quantum criticality [23,24]. Moreover, a field-induced phase diagram of this system is very complex [30,31]. These unusual observations pave the way to look for new CeTmIn (Tm= Pt and Pd) based ternary compounds including hypotheticalCePtIn5 and CePdIn5.…”
Section: Introductionmentioning
confidence: 99%
“…Above situation may well explain the observed physical properties in the recently discovered HF material Ce 3 PtIn 11 [15][16][17]. The material belongs to the Ce n T m In 3n+2m class of layered materials to which also CeCoIn 5 , CeRhIn 5 and Ce 2 RhIn 8 belong.…”
Section: Introductionmentioning
confidence: 53%