Magnetic behavior in a series of cerium ternary intermetallics: Ce 2 T 2 In T Ni, Cu, Rh, Pd, Pt, and Au D. Kaczorowski* W. Trzebiatowski Institute for Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937, 50-950 Wroclaw, Poland and Institut fu ¨r Physikalische Chemie, Universita ¨t Wien, Wa ¨hringerstraße 42, A-1090 Wien, Austria P. Rogl and K. Hiebl Institut fu ¨r Physikalische Chemie, Universita ¨t Wien, Wa ¨hringerstraße 42, A-1090 Wien, Austria Received 14 February 1996; revised manuscript received 2 May 1996 A group of ternary cerium compounds Ce 2 T 2 In T =Ni, Cu, Rh, Pd, Pt, and Auhas been synthesized. As found from single-crystal and powder x-ray-diffraction studies, all these phases crystallize in a primitive tetragonal structure of the Mo 2 FeB 2 type. Magnetic measurements magnetization, dc and ac susceptibility have revealed the physical properties of these intermetallics to be mainly governed by the 4 f - d hybridization. Depending on the filling of the transition metal d band the ground state in Ce 2 T 2 In changes from a nonmag- netic to a well localized magnetic regime. It was proved that Ce 2 Ni 2 In and Ce 2 Rh 2 In are intermediate-valence systems, Ce 2 Pt 2 In is a strongly temperature-dependent paramagnet, whereas Ce 2 Cu 2 In, Ce 2 Pd 2 In, and Ce 2 Au 2 In order magnetically at low temperatures. Measurements of the electrical resistivity have corroborated the intermediate-valence behavior in Ce 2 Ni 2 In and Ce 2 Rh 2 In. In turn, the resistivity of the remaining ternaries studied was found to be determined by an interplay of Kondo scattering and crystal-field effects. For Ce 2 Pt 2 In which behaves like a spin-fluctuating system due to strong Kondo-type interactions a nonmagnetic heavy- fermion ground state probably occurs. S0163-18299608134-9 I. INTRODUCTION Recently a series of ternary actinoid compounds with the composition An 2 T 2 M An =U, Np; T =3 d -, 4 d -, 5 d - transition metal; M =In, Sn, crystallizing in the tetragonal Mo 2 FeB 2 -type structure an ordered derivative of the U 3 Si 2 -type structure, has been discovered. 1–3 As a result of intensive experimental 2–8 and theoretical 9–12 studies of these materials it was established that their electronic properties are mainly determined by the hybridization of the 5 f states with the d states of transition elements. As for many other families of light actinoid intermetallics, the behavior in the An 2 T 2 M compounds was found to change gradually from a nonmagnetic to a magnetic ground state when moving from the left to the right of a transition-metal row. 7,13 Interest- ingly, most of the uranium 2:2:1 phases exhibit at low tem- peratures a strong enhancement in the electronic coefficient of the specific heat values up to 830 mJ/mole K 2 as ob- served for U 2 Pt 2 In 5 and this feature in conjunction with the characteristic magnetic and electrical properties of these compounds may support their classification as heavy- fermion systems. 5,9,10 In contrast to the extensively studied actinoid intermetal- lics with the 2:2:1 stoichiometry only very little is known up to date about the corresponding rare-earth-based materials. This fact has motivated us to start a systematic investigation of the Ce 2 T 2 In compounds. Our choice of cerium-based phases is due to a common tendency of this element to show anomalous physical behavior in its binary or ternary interme- tallics. Although already in 1990 the formation of Ce 2 Ni 2 In and Ce 2 Cu 2 In was described by Kalychak et al., 14 the mag- netic properties of these two compounds were not studied at that time. More recently Hulliger and Xue 15 synthesized the Ce 2 Pd 2 In indide and found that it is ferromagnetic below T c =4 K. This finding has subsequently been confirmed by Gordon et al. 16 who also reported on the nonmagnetic prop- erties of Ce 2 Ni 2 In. Already in the course of our present study two further publications by Hulliger appeared which ad- dressed the synthesis of Ce 2 Pt 2 In Ref. 17and Ce 2 Rh 2 In. 18 The first compound was briefly mentioned to be paramag- netic down to 1.5 K Ref. 17and for the latter a nonmag- netic ground state was claimed 18 due to the presence of Ce 4+ ions. In the present paper we give an extended survey of the physical behavior in the Ce 2 T 2 In intermetallics with T =Ni, Cu, Rh, Pd, Pt, and Au. We report here on the crystal struc- ture refinements from x-ray data and present the results of detailed magnetization, dc susceptibility, ac susceptibility, and electrical resistivity measurements performed on poly- crystalline samples of Ce 2 T 2 In. In the discussion we empha- size the role of interactions between the cerium 4 f electrons and the d electrons of neighboring transition-metal atoms in the magnetic moment formation in the compounds studied. II. EXPERIMENTAL DETAILS Polycrystalline samples of La 2 T 2 In and Ce 2 T 2 In were pre- pared by arc melting the appropriate amounts of the constitu- ent elements in a titanium gettered argon atmosphere. The buttons were turned over and remelted several times to en- sure a good homogeneity. Weight losses after meltings were always smaller than 0.5 mass%. No further heat treatment was given to the ingots except for Ce 2 T 2 In, T =Ni, Rh, Pd, which were subsequently wrapped with molybdenum foil, sealed in evacuated quartz tubes and annealed at 650 °C for two weeks. All the samples obtained as cast and annealed PHYSICAL REVIEW B 1 OCTOBER 1996-II VOLUME 54, NUMBER 14 54 0163-1829/96/5414/989112/$10.00 9891 © 1996 The American Physical Society