Crystal structure, specific heat, and 119Sn Mossbauer spectroscopy of CeRu4Sn6:: A ternary stannide with condensed, distorted RuSn6 octahedra

被引:43
作者
Pottgen, R
Hoffmann, RD
Sampathkumaran, EV
Das, I
Mosel, BD
Mullmann, R
机构
[1] Univ Munster, Inst Anorgan Chem, D-48149 Munster, Germany
[2] Tata Inst Fundamental Res, Bombay 400005, Maharashtra, India
[3] Univ Munster, Inst Phys Chem, D-48149 Munster, Germany
关键词
CeRu4Sn6; stannide; cerium intermetallics;
D O I
10.1006/jssc.1997.7565
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
CeRu4Sn6 was prepared from the elements by a reaction in an arc-melting furnace and subsequent annealing at 1123 K. It crystallizes with the tetragonal YRu4Sn6 type structure of space group I (4) over bar 2m: a=688.1(1), c=975.2(2) pm, V=0.4617(1) nm(3), wR2 = 0.0472, 554 F-2 values, and 19 variables. The cerium atoms in CeRu4Sn6 have coordination number 16 formed by 12 tin and 4 ruthenium atoms. These polyhedra are arranged in a tetragonal body-centered packing and are linked by common Sn1 atoms. The strongest bonding interactions are between ruthenium and tin atoms. The ruthenium atoms have 6 tin neighbors at distances from 256.9 to 276.8 pm in the form of a strongly distorted octahedron. Four of such octahedra are condensed via common edges and faces forming [Ru4Sn6] units. These groups are packed in a tetragonal body-centered arrangement. The cerium atoms occupy the space between the [Ru4Sn6] units. The [Ru4Sn6] substructure of CeRu4Sn6 is discussed in comparison with the structures of Ru2Sn3, LaRuSn3, and Ru3Sn15O14 which also contain condensed RuSn6 octahedra or trigonal prisms as characteristic structural motifs. Despite the two different tin sites the Sn-119 Mossbauer spectroscopic measurements show only one signal at delta=1.99 mm/s subjected to quadrupole splitting. Heat capacity measurements indicate that CeRu4Sn6 behaves like a heavy-fermion compound. (C) 1997 Academic Press.
引用
收藏
页码:326 / 331
页数:6
相关论文
共 38 条
[1]   LEAST-SQUARES ABSOLUTE-STRUCTURE REFINEMENT - PRACTICAL EXPERIENCE AND ANCILLARY CALCULATIONS [J].
BERNARDINELLI, G ;
FLACK, HD .
ACTA CRYSTALLOGRAPHICA SECTION A, 1985, 41 (SEP) :500-511
[2]   ANOMALOUS MAGNETIC-BEHAVIOR OF CERIUM IN CE2SN5 AND CE3SN7, 2 SUPERSTRUCTURES OF CESN3 [J].
BONNET, M ;
BOUCHERLE, JX ;
GIVORD, F ;
LAPIERRE, F ;
LEJAY, P ;
ODIN, J ;
MURANI, AP ;
SCHWEIZER, J ;
STUNAULT, A .
JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, 1994, 132 (1-3) :289-302
[3]   STRUCTURES OF CE2SN5 AND CE3SN7, 2 SUPERSTRUCTURES OF CESN3 [J].
BOUCHERLE, JX ;
GIVORD, F ;
LEJAY, P ;
SCHWEIZER, J ;
STUNAULT, A .
ACTA CRYSTALLOGRAPHICA SECTION B-STRUCTURAL SCIENCE, 1988, 44 :377-380
[5]   ELECTRICAL-RESISTANCE ANOMALIES IN A CE-RU-SN PHASE [J].
DAS, I ;
SAMPATHKUMARAN, EV .
PHYSICAL REVIEW B, 1992, 46 (07) :4250-4252
[6]  
Donohue J., 1974, STRUCTURES ELEMENTS
[7]   CAGE STRUCTURES IN INTERMETALLIC COMPOUNDS - INFORMATION OF LARUSN3, CERUSN3, PRRUSN3 AND NDRUSN3 [J].
EISENMANN, B ;
SCHAFER, H .
JOURNAL OF THE LESS-COMMON METALS, 1986, 123 :89-94
[8]   ISOMORPHS OF THE SUPERCONDUCTING-MAGNETIC TERNARY STANNIDES [J].
ESPINOSA, GP ;
COOPER, AS ;
BARZ, H .
MATERIALS RESEARCH BULLETIN, 1982, 17 (08) :963-969
[9]   CRYSTAL-CHEMISTRY, GROWTH AND REENTRANT BEHAVIOR OF ADDITIONAL SUPERCONDUCTING-MAGNETIC STANNIDES [J].
ESPINOSA, GP ;
COOPER, AS ;
BARZ, H ;
REMEIKA, JP .
MATERIALS RESEARCH BULLETIN, 1980, 15 (11) :1635-1641