Scandium iridium boride Sc3Ir5B2 and the quaternary derivatives Sc2MIr5B2 with M = Be, Al, Si, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Ga, or Ge:: Preparation, crystal structure, and physical properties

被引:44
作者
Nagelschmitz, EA [1 ]
Jung, W [1 ]
机构
[1] Univ Cologne, Inst Anorgan Chem, D-50939 Cologne, Germany
关键词
D O I
10.1021/cm9802898
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The new compounds Sc3Ir5B2 and Sc2MIr5B2 with M = Be, Al, Si, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Ga, or Ge were prepared by are-melting appropriate compressed mixtures of the elemental components in an argon atmosphere. They crystallize tetragonally with Z = 2 in the space group P4/mbm with lattice constants a = 952.6(1) pm and c = 304.8(1) pm for Sc3Ir5B2 and ranging from a = 927.0(1) pm and c = 296.8(1) pm (Sc2BeIr5B2) to a = 932.9(1) pm and c = 310.3(1) pm (Sc2TiIr5B2) for the quaternary compounds. According to powder diagrams, all compounds are isotypic. Structure determinations based on single-crystal X-ray data were performed for Sc2SiIr5B2, Sc2VIr5B2, and Sc2FeIr5B2. Sc3Ir5B2 crystallizes with the Ti3Co5B2-type compounds, while the quaternary compounds form an ordered substitutional variant of this structure. The M atoms are arranged in rows along [001] with M-M distances of similar to 300 pm in the rows and similar to 660 pm between the rows. For the compounds with M = Mn, Fe, or Co, this results in highly anisotropic magnetic properties. Susceptibility measurements with a Faraday balance in the range 7-770 K suggest ferromagnetic coupling in the rows at low temperatures. Between the rows, the coupling was antiferromagnetic for Sc2FeIr5B2 (T-N approximate to 190 K) and ferromagnetic for Sc2MnIr5B2 (T-C approximate to 115 K, mu(s) approximate to 1.2 mu(B)) and for Sc2CoIr5B2 (T-C approximate to 135 K, mu(s) approximate to 1.2 mu(B)). The temperature dependence of the resistivity was measured for the compounds with M = Si, Mn, Fe, and Co.
引用
收藏
页码:3189 / 3195
页数:7
相关论文
共 11 条
[1]  
BELOV KP, 1965, MAGNETIC TRANSITION, P34
[2]  
HALL SR, 1989, XTAL 3 2
[3]   QUATERNARY MAGNESIUM IRIDIUM BORIDES MG2XIR5B2 WITH X = BE, AL, SI, P, TI, V, CR, MN, FE, CO, NI, CU, ZN, GA, GE, AS - A SUBSTITUTION VARIANT OF THE TI3CO5B2 TYPE OF STRUCTURE [J].
JUNG, W ;
SCHIFFER, J .
ZEITSCHRIFT FUR ANORGANISCHE UND ALLGEMEINE CHEMIE, 1990, 581 (02) :135-140
[4]   A THEORY OF METALLIC FERROMAGNETISM AND ANTIFERROMAGNETISM ON ZENERS MODEL [J].
KASUYA, T .
PROGRESS OF THEORETICAL PHYSICS, 1956, 16 (01) :45-57
[5]   DETAILED MAGNETIC BEHAVIOR OF NICKEL NEAR ITS CURIE POINT [J].
KOUVEL, JS ;
FISHER, ME .
PHYSICAL REVIEW, 1964, 136 (6A) :1626-+
[6]  
KUZMA YB, 1971, ZH STRUKT KHIM, V12, P458
[7]   ELECTRONS IN TRANSITION METALS [J].
MOTT, NF .
ADVANCES IN PHYSICS, 1964, 13 (51) :325-+
[8]  
NAGELSCHMITZ EA, UNPUB
[9]  
PAULING L, 1964, NATUR CHEMISCHEN BIN
[10]   INDIRECT EXCHANGE COUPLING OF NUCLEAR MAGNETIC MOMENTS BY CONDUCTION ELECTRONS [J].
RUDERMAN, MA ;
KITTEL, C .
PHYSICAL REVIEW, 1954, 96 (01) :99-102