Two superstructures of Ce3Rh4Ge4

2018 ◽  
Vol 233 (2) ◽  
pp. 81-95 ◽  
Author(s):  
Daniel Voßwinkel ◽  
Rolf-Dieter Hoffmann ◽  
Volodymyr Svitlyk ◽  
Wilfried Hermes ◽  
Magnus Greiwe ◽  
...  

AbstractTwo different samples of Ce3Rh4Ge4were synthesized from different starting compositions by melting of the elements in an arc-melting furnace followed by annealing sequences in a sealed tantalum ampoule in a muffle furnace. The structures of two different stacking variants were refined on the basis of temperature dependent single-crystal X-ray diffractometer data. At high temperature Ce3Rh4Ge4adopts the U3Ni4Si4type structure with strongly enhanced anisotropic displacement parameters for the Rh1 atoms. For the two different crystals, additional reflections start to appear at different temperatures. The first crystal showed additional reflections already at room temperature (stacking variant I) and the second one showed additional reflections emerging below 270 K (stacking variant II). Stacking variant I could be described with the (3+1)D superspace groupI2/m(α0γ)00;α=1/2a*,γ=1/2c*; (Z=2), 1252F2values, 48 variables, wR=0.0306 for the main and wR=0.0527 for 440 1storder satellite reflections, similar to Pr3Rh4Ge4. For stacking variant II the (3+1)D superspace group isImmm(α00)00s;α=1/2a*; (Z=2). The structure could be refined with 1261F2values, 53 variables and residuals ofwR=0.0331 for the main reflections andwR=0.1755 (R1obs=0.0788) for the 1storder satellite reflections, [a=406.2(1),b=423.7(1) andc=2497.1(1) pm]. The commensurate description could be transformed to a three-dimensional (3D) supercell with space groupPnmaandZ=4:a=812.5(1),b=423.7(1),c=2497.1(2) pm, 1261F2values, 69 variables andwR=0.0525. The relation of the U3Ni4Si4type structure, the (3+1)D modulated and the 3D supercells are discussed on the basis of group-subgroup schemes. Ab initio electronic structure calculations are in line with the diffraction experiments, revealing the lowest total energy for thePnmaphase.

2019 ◽  
Vol 74 (1) ◽  
pp. 15-25 ◽  
Author(s):  
Lukas Heletta ◽  
Samir F. Matar ◽  
Rainer Pöttgen

AbstractThe ZrNiAl-type (space groupP6̅2m) gallidesTIrGa (T=Zr, Nb, Hf, Ta), ZrNiGa and ScPdGa were obtained by arc-melting of the elements, followed by annealing in sealed silica tubes. The samples have been characterized through their Guinier powder patterns. The structures of ZrNiGa, NbIr1.08Ga0.92and TaIr1.10Ga0.90were refined from single-crystal X-ray diffractometer data. Refinements of the occupancy parameters indicate the formation of solid solutions for the niobium and the tantalum compound. Within the huge family of ZrNiAl-type phases, NbIr1.08Ga0.92and TaIr1.10Ga0.90have the smallestc/aratios; however, no structural distortions or superstructure formation have been observed. Electronic structure calculations were exemplarily carried out for NbIrGa, substantiating the dominance of the Ir–Ga and Nb–Ir bonding interactions. Temperature dependent magnetic susceptibility measurements of LT-ScPdGa, ZrIrGa, NbIrGa and HfIrGa have shown Pauli paramagnetism. ScPdGa is dimorphic with an orthorhombic TiNiSi-type high-temperature modification (arc-melting and quenching; space groupPnma) which transforms to the hexagonal ZrNiAl-type low-temperature modification upon annealing at 1023 K. Both structures were refined from single-crystal X-ray diffractometer data. HT-ScPdGa exclusively shows Pd–Ga bonding within the three-dimensional [PdGa] polyanionic network, while additional weak Pd–Pd and Ga–Ga interactions occur in LT-ScPdGa.


Author(s):  
Oliver Niehaus ◽  
Rolf-Dieter Hoffmann ◽  
Bernard Chevalier ◽  
Rainer Pöttgen

AbstractCeCoGa was synthesized by melting of the elements in an arc-melting furnace as well as in a sealed niobium tube in an induction furnace. A further annealing step improves the purity and crystallinity of the samples significantly. Its structure was refined on the basis of single-crystal X-ray diffractometer data at different temperatures. Already at room temperature CeCoGa crystallizes in a superstructure of the HT-CeCoAl type. This superstructure can be described in the (3+1)D superspace group


2011 ◽  
Vol 66 (12) ◽  
pp. 1241-1247
Author(s):  
Patrick R.N. Misse ◽  
Richard Dronskowski ◽  
Boniface P. T. Fokwa

Powder samples and single crystals of the boride phases MxRh7−xB3 (M = Cr,Mn, Ni; x ≤ 1) have been synthesized from the elements using an arc-melting furnace under purified argon atmosphere in a water-cooled copper crucible. The new phases were characterized from single-crystal and powder X-ray diffraction, as well as semi-quantitative EDX measurements. The obtained phases crystallize in the hexagonal Th7Fe3 structure type (space group P63mc, no. 186, Z = 2). In all cases (M = Cr, Mn, Ni), M is found to preferentially mix with rhodium at only one (6c) of the three available rhodium positions. Pauli paramagnetism was observed in CrxRh7−xB3 (x < 1), whereas both Pauli and temperature-dependent paramagnetisms were found in NiRh6B3.


2018 ◽  
Vol 73 (12) ◽  
pp. 1015-1021 ◽  
Author(s):  
Lukas Heletta ◽  
Rainer Pöttgen

AbstractThe plumbides RE2Rh2Pb (RE = La–Nd, Sm, Gd, Tb) were synthesized in sealed niobium ampoules by induction melting of the pure elements or directly via arc-melting. The characterization of the samples by X-ray powder diffraction confirmed their Mo2B2Fe-type structure (space group P4/mbm) at room temperature. The Sm2Rh1.924Pb structure was refined from single-crystal X-ray diffractometer data: a=760.02(5), c=378.20(3) pm, wR=0.0387, 292 F2 values, 13 variables. The rhodium site shows small defects. The RE2Rh2Pb plumbides are simple 1:1 intergrowth structures of AlB2 and CsCl related slabs of compositions RERh2 and REPb. The Rh2 dumbbell in the SmRh2 slab of Sm2Rh2Pb shows a Rh–Rh distance of 281 pm. Temperature-dependent magnetic susceptibility measurements of La2Rh2Pb, Pr2Rh2Pb and Nd2Rh2Pb showed that the rhodium atoms carry no localized magnetic moments. La2Rh2Pb exhibits Pauli-paramagnetic behavior induced by the conduction electrons. The ground state of the praseodymium compound is ferromagnetic below TC=3.3 K while the neodymium compound shows a transition to an antiferromagnetic state at TN=6.1 K and a metamagnetic transition at a critical field of ca. 1000 Oe.


2002 ◽  
Vol 57 (7) ◽  
pp. 798-802 ◽  
Author(s):  
Vasyl’ I Zaremba ◽  
Vitaliy P Dubenskiy ◽  
Rainer Pöttgena

The ternary indides LnRhIn2 (Ln = La, Ce, Pr, Nd, Sm) were synthesized by arc-melting of the elements under an argon atmosphere and subsequent annealing at 870 K. The samples have been investigated by X-ray diffraction on powders and single crystals: MgCuAl2 type, Cmcm, a = 448.2(1), b = 1025.7(1), c = 795.1(1) pm, wR2 = 0.0372, 228 F2 values, 16 variables for LaRhIn2, a = 446.0(1), b = 1017.3(2), c = 792.7(1) pm for CeRhIn2, a = 444.03(6), b = 1013.1(1), c = 792.5(1) pm for PrRhIn2, a = 442.49(5), b = 1012.7(1), c = 789.3(1) pm for NdRhIn2, and a = 438.1(1), b = 1009.3(1), c = 788.3(1) pm, wR2= 0.0414, 304 F2 values, 16 variables for SmRhIn2. Geometrical motifs of these structures are tricapped trigonal prisms around the rhodium atoms. The shortest interatomic distances were observed for the Rh-In contacts: 280-282 pm for LaRhIn2 and 276-279 pm for SmRhIn2. Together, the rhodium and indium atoms build a three-dimensional [RhIn2] polyanion in which the lanthanoid atoms fill distorted pentagonal channels. According to one short La-Rh (282 pm) and Sm-Rh (284 pm) distance one can assume strong bonding of the lanthanoid atoms to the polyanion.


2000 ◽  
Vol 55 (11) ◽  
pp. 1025-1030 ◽  
Author(s):  
Yaroslav V. Galadzhun ◽  
Vasyl' I. Zaremba ◽  
Holger Piotrowski ◽  
Peter Mayer ◽  
Rolf-Dieter Hoffmann ◽  
...  

The ternary indides ScPtln, TbPtln, and HoPtln were synthesized by reaction of the elements in an arc-melting furnace and subsequent annealing for four weeks. ScPtln and HoPtln are reported here for the first time. The three indides crystallize with the hexagonal ZrNiAl structure, a ternary ordered version of the Fe2P type, space group P6̄2m. Single crystal X-ray data yielded a = 754.6(1), c = 348.31(8) pm, wR2 = 0.0390, 177 F2 values for ScPtln, a = 759.3(1), c = 387.6(1) pm, wR2 = 0.0576, 183 F2 values for TbPtln, and a = 758.13(1), c = 381.62(1) pm, wR2 = 0.0530, 239 F2 values for HoPtln with 14 variable parameters for each refinement. Striking structural motifs of these intermetallics are short Pt-In distances (270 - 286 pm) within the three-dimensional [Ptln] polyanions which are composed of Pt(2)In6 trigonal prisms and trigonal planar P t(l)In3 units. The platinum-indium substructure of ScPtln is discussed in comparison with the various platinum-indium networks in the structures of Ptln2, Pt3In7, SrPtln, Sr2Pt3ln4, SrPtIn2, LaPtIn3, and PtIn7Fi3.


1997 ◽  
Vol 52 (1) ◽  
pp. 141-144 ◽  
Author(s):  
Rainer Pöttgen

Zr5CuSn3 was prepared from the elements in an arc-melting furnace and investigated by X-ray diffraction of powders as well as of single crystals. The crystal structure was refined from four-circle diffractometer data: P63/mcm, a = 860.04(7) pm, c = 586.80(5) pm, V = 0.3759(1) nm3, Z = 2, wR2 = 0.0402 for 371 F2 values and 15 variables. A refinement of the occupancy parameters re­vealed that the copper position is occupied to only 95.3(8)% in the crystal used for the X-ray investigation. Zr5CuSn3 crystallizes in the Hf5CuSn3 type structure, a filled variant of the Mn5Si3 type. The main features of the Zr5CuSn3 structure are condensed Zr6 octahedra that are centered by copper atoms


2011 ◽  
Vol 66 (8) ◽  
pp. 777-783
Author(s):  
Konrad Schäfer ◽  
Wilfried Hermes ◽  
Ute Ch. Rodewald ◽  
Rolf-Dieter Hoffmann ◽  
Rainer Pöttgen

The antimonides RE2Ir3Sb4 (RE = La, Ce, Pr, Nd) were synthesized by arc-melting of the elements and subsequent annealing or via high-frequency melting. The samples were characterized by X-ray powder diffraction, and the four structures were refined from single-crystal X-ray diffraction data: Pr2Ir3Sb4 type, Pnma, Z = 4, a = 1621.9(2), b = 458.60(8), c = 1099.8(1) pm, wR2 = 0.036, 1558 F2 values for La2Ir3Sb4, a = 1616.6(8), b = 456.5(2), c = 1094.8(5) pm, wR2 = 0.092, 1080 F2 values for Ce2Ir3Sb4, a = 1613.0(5), b = 454.9(2), c = 1094.1(5) pm, wR2 = 0.057, 1428 F2 values for Pr2Ir3Sb4, and a = 1609.8(6), b = 452.9(2), c = 1092.3(5) pm, wR2 = 0.052, 1472 F2 values for Nd2Ir3Sb4, with 56 parameters per refinement. The Sb1 atoms show enhanced displacement off the mirror planes at y = 1/4 and y = 3/4. A series of temperature-dependent structure refinements of Pr2Ir3Sb4 down to 90 K are indicative of static disorder. The iridium and antimony atoms build up covalently bonded three-dimensional [Ir3Sb4] networks with Ir-Sb distances ranging from 256 -269 pm (Nd2Ir3Sb4). The two crystallographically independent rare earth sites fill cavities of coordination numbers 17 (8 Ir + 9 Sb) and 15 (6 Ir + 9 Sb) within the [Ir3Sb4] polyanions. Temperature-dependent magnetic susceptibility measurements indicate a stable trivalent ground state for the cerium compound. No magnetic ordering was evident down to 3 K.


2001 ◽  
Vol 56 (6) ◽  
pp. 463-468 ◽  
Author(s):  
Ratikanta Mishra ◽  
Rainer Pöttgen ◽  
Gunter Kotzyba

AbstractThe metal-rich intermetallic compounds NblrSi, NblrGe, and TalrSi were synthesized by arc-melting of the elements and subsequent annealing in glassy carbon crucibles in a high-frequency furnace. The three compounds were investigated by X-ray diffraction on powders and single crystals: TiNiSi type, Pnma, a = 641.27(3), b = 379.48(2), c = 727.70(3) pm, wR2 = 0.0773, 430 F2 values for NblrSi, a = 645.48(3), b = 389.21(2), c = 741.11(4) pm, wR2 = 0.0981, 297 F2 values for NblrGe, and a = 638.11(3), b = 378.69(2), c = 726.78(3) pm, wR2 = 0.0887, 290 F2 values for TalrSi with 20 variables for each refinement. The iridium and silicon (germanium) atoms form a three-dimensional network of puckered Ir3Si3 and Ir3Ge3 hexagons in which the niobium (tantalum) atoms fill larger cages. Magnetic susceptibility measurements on NblrSi and TalrSi indicate Pauli paramagnetism with room temperature susceptibilities of 0.30(5)·10-9 and 0.97(5)·10-9 m3/mol, respectively.


2016 ◽  
Vol 71 (5) ◽  
pp. 567-577 ◽  
Author(s):  
Birgit Gerke ◽  
Alexander Korthaus ◽  
Oliver Niehaus ◽  
Frank Haarmann ◽  
Rainer Pöttgen

AbstractThe gold-rich intermetallic compounds Sr2Au6Zn3, Eu2Au6Zn3, Sr2Au6Ga3, and Eu2Au6Ga3 were synthesized from the elements in sealed tantalum ampoules in induction or muffle furnaces. The europium compounds are reported for the first time and their structures were refined from single crystal X-ray diffractometer data: Sr2Au6Zn3 type, R3̅c, a = 837.7(1), c = 2184.5(4) pm, wR2 = 0.0293, 572 F2 values for Eu2Au6.04Zn2.96 and a = 838.1(2), c = 2191.7(5) pm, wR2 = 0.0443, 513 F2 values for Eu2Au6.07Ga2.93 with 20 variables per refinement. The structures consist of a three-dimensional gold network with a 6R stacking sequence, similar to the respective diamond polytype. The cavities of the network are filled in a ratio of 2:1 by strontium (europium) atoms and Ga3 (Zn3) triangles in an ordered manner. Sr2Au6Zn3 and Sr2Au6Ga3 are diamagnetic with room temperature susceptibilities of –3.5 × 10−4 emu mol–1. Temperature dependent susceptibility and 151Eu Mössbauer spectroscopic measurements show a stable divalent ground state for both europium compounds. Eu2Au6Zn3 and Eu2Au6Ga3 order antiferromagnetically below Néel temperatures of 16.3 and 12.1 K, respectively. Anisotropic electrical conductivity of Sr2Au6Ga3 is proven by an alignment of the crystallites in the magnetic field. Orientation-dependent 69;71Ga NMR experiments combined with quantum mechanical calculations (QM) give evidence for a highly anisotropic charge distribution of the Ga atoms.


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