001007495 001__ 1007495 001007495 005__ 20231027114405.0 001007495 0247_ $$2doi$$a10.1103/PhysRevResearch.5.013058 001007495 0247_ $$2Handle$$a2128/34465 001007495 0247_ $$2WOS$$aWOS:000926781700002 001007495 037__ $$aFZJ-2023-02085 001007495 082__ $$a530 001007495 1001_ $$0P:(DE-Juel1)194784$$aStekiel, Michal$$b0$$eCorresponding author$$ufzj 001007495 245__ $$aIncommensurate antiferromagnetic order in CePtAl 3 001007495 260__ $$aCollege Park, MD$$bAPS$$c2023 001007495 3367_ $$2DRIVER$$aarticle 001007495 3367_ $$2DataCite$$aOutput Types/Journal article 001007495 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1698057246_15069 001007495 3367_ $$2BibTeX$$aARTICLE 001007495 3367_ $$2ORCID$$aJOURNAL_ARTICLE 001007495 3367_ $$00$$2EndNote$$aJournal Article 001007495 520__ $$aWe report on a neutron diffraction study of single-crystal CePtAl3 complemented by measurements of the specific heat under applied magnetic field. Below TN ≈ 3 K, CePtAl3 develops incommensurate antiferromagneticorder with a single modulation vector k = (0.676 0 0). Residual magnetic scattering intensity above TN and a broadening of the specific heat anomaly at TN may be consistently described in terms of a Gaussiandistribution of transition temperatures with a standard deviation σ ≈ 0.5 K. The distribution of TN may be attributed to the observation of occupational and positional disorder between the Pt and Al sites consistent withstructural information inferred from neutron diffraction. 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