Abstract
The compound CeIr3B2 crystallizes in a monoclinic unit cell (space group C2/m) with a structure related to that of hexagonal CeCo3B2 [1]. Cerium has been shown to be in a mixed valent states in this compound [2]. On the other hand CeRh3B2 has the hexagonal CeCo3B2 type structure (space group P6/mmm) and orders ferromagnetically with TC=115K, and a small magnetic moment of 0.42 μB/fu. The magnetism in CeRh3B2 [3] is very puzzeling. To understand the origin of magnetism in CeRh3B2, many mixed alloys have been studied, such as (Ce1−xLax)Rh3B2 [4], CeRh3−xMxB2 (M= Ru,Os and Ir) [5−8] and CeRh3B2_xSix [9]. In this structure, hybridization of the Ce-4f electrons with neighbouring atoms is believed to play an important role [10]. Since Rh and Ir are isoelectronic and Ce-Ce distances are nearly the same in CeT3B2 (T = Rh and Ir), the absence of magnetic ordering in CeIr3B2 is rather surprising. We report on the structure and the magnetic behaviour of CeIr3B2−xSix alloys. We find that initial replacement of Si by B causes magnetic ordering to appear in this system.
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© 1987 Plenum Press, New York
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Umarji, A.M., Malik, S.K. (1987). Structure and Magnetic Properties of CeIr3B2−xSix System. In: Gupta, L.C., Malik, S.K. (eds) Theoretical and Experimental Aspects of Valence Fluctuations and Heavy Fermions. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-0947-5_70
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DOI: https://doi.org/10.1007/978-1-4613-0947-5_70
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