Scaffolds of magnetically active 3d metals in the valence electron controlled borides Ti9−xM2+xRu18B8 (M=Cr–Ni; x=0.5–1): Structutral, electronic and magnetic properties
Scaffolds of magnetically active 3d metals in the valence electron controlled borides Ti9−xM2+xRu18B8 (M=Cr–Ni; x=0.5–1): Structutral, electronic and magnetic properties
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价电子控制硼化物 Ti9−xM2+xRu18B8 (M=Cr–Ni; x=0.5–1) 中磁性活性 3d 金属的支架:结构、电子和磁性
DOI:
10.1016/j.jssc.2013.05.040
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发表时间:
2013
影响因子:
3.3
通讯作者:
B. Fokwa
中科院分区:
文献类型:
--
作者:
C. Goerens;Jakoah Brgoch;G. Miller;B. Fokwa
Polycrystalline samples of the boride series Ti9−xM2+xRu18B8(M=Cr, Co, Mn, Ni) including single crystals of Ti8Co3Ru18B8have been prepared by arc-melting the elements. The phases were characterized by powder X-ray diffraction (Rietveld refinement), single-crystal X-ray diffraction (for M=Co), and energy-dispersive X-ray (EDX) analysis. They are substitutional variants of the Zn11Rh18B8structure type, space groupP4/mbm(No. 127) and contain a “scaffold” structural unit (M-ladders interacting with M/Ti-chains) as well as isolated M/Ti-chains. According to DFT calculations, the Ru–X (X=B, Ti, Ti/M) bonding interactions are nearly constant throughout the series and responsible for the structural stability of these phases, whereas the M–M and Ru–M interactions vary significantly with varying valence electron count. Furthermore, density of states (DOS) analyses predict the phases with M=Mn and Ni to develop a total magnetic moment but not the M=Co phase. Susceptibility measurements confirm the Co phase to be paramagnetic and the Mn Phase orders ferrimagnetically below 120 K and thus develops a magnetic moment, as predicted.
影响因子:
15
作者:
Fang, Junfeng;Wallikewitz, Bodo H.;Huck, Wilhelm T. S.
通讯作者:
Huck, Wilhelm T. S.