Publications by authors named "Bobnar M"

The quaternary nitridochromate(IV) LiSr[CrN] crystallizes in a new structure type with the non-centrosymmetric space group 2 (no. 4) with = 5.5685(7) Å, = 5.

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The current development of soft shape-memory materials often results in materials that are typically limited to the synthesis of thin-walled specimens and usually rely on complex, low-yield manufacturing techniques to fabricate macro-sized, solid three-dimensional objects. However, such geometrical limitations and slow production rates can significantly hinder their practical implementation. In this work, we demonstrate a shape-memory composite material that can be effortlessly molded into arbitrary shapes or sizes.

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While a negative oxidation state occurs rarely for metals in general, this is commonly known for metal carbonyl anions, carbonyl metalates. Although CO and CN are isoelectronic, cyanidometalates usually do not exhibit metal centers with negative oxidation states. However, we report on the electron-rich tetrahedral tetracyanidoferrate(-II) anion [Fe(CN)], which was stabilized in (SrN)[Fe(CN)] (space group 3, = 702.

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Polymorphism is observed in the YRhGe series. The decrease of Y-content leads to the transformation of the primitive cubic YRhGe [ = 0.6, space group 3̄, = 8.

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The compound IrGa was synthesized by direct reaction of the elements. It is formed as a high-temperature phase in the Ir-Ga system. Single-crystal X-ray diffraction analysis confirms the tetragonal symmetry (space group 4 , No.

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Article Synopsis
  • YbCoGe is identified as the first material exhibiting a Remeika phase with a specific modulated crystal structure characterized by a 3 + 3 symmetry.
  • Increasing the proportion of Yb in YbCoGe eliminates satellite reflections and stabilizes a disordered primitive cubic structure.
  • This compound functions as a metal with hole-like charge carriers, where Yb ions exhibit a temperature-dependent intermediate valence state that fluctuates between +2.60 and +2.66 from 85 to 293 K, studied using various spectroscopy and measurement techniques.
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The metastable type-II clathrate Na Ge was obtained from Na Ge by applying a two-step procedure. At first, Na Ge was reacted at 70 °C with a solution of benzophenone in the ionic liquid (IL) 1,3-dibutyl-2-methylimidazolium-bis(trifluoromethylsulfonyl) azanide. The IL was inert towards Na Ge , but capable of dissolving the sodium salts formed in the redox reaction.

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Exceptionally electron-rich, nearly trigonal-planar tricyanidometalate anions [Fe(CN) ] and [Ru(CN) ] were stabilized in LiSr [Fe(CN) ] and AE [M(CN) ] (AE=Sr, Ba; M=Fe, Ru). They are the first examples of group 8 elements with the oxidation state of -IV. Microcrystalline powders were obtained by a solid-state route, single crystals from alkali metal flux.

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RbBSi forms under high-pressure, high-temperature conditions at = 8 GPa and = 1273 K. The new compound (space group 3̅, = 9.9583(1) Å) is the second example for a clathrate-I borosilicide.

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HfBIr crystallizes with a new type of structure: space group , = 5.6300(3) Å, = 11.2599(5) Å, and = 3.

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An efficient application of a material is only possible if we know its physical and chemical properties, which is frequently obstructed by the presence of micro- or macroscopic inclusions of secondary phases. While sometimes a sophisticated synthesis route can address this issue, often obtaining pure material is not possible. One example is TaGeIr, which has highly sample-dependent properties resulting from the presence of several impurity phases, which influence electronic transport in the material.

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The homogeneity range of ternary iron indium thiospinel at 873 K was investigated. A detailed study was focused on two distinct series (y=z): 1) a previously reported charge-balanced (In □ ) [In Fe ] S (A1-series; □ stands for vacancy; the abbreviations "tetr" and "oct" indicate atoms occupying tetrahedral 8a and octahedral 16d sites, respectively) and 2) a new charge-unbalanced (In □ ) [In Fe ] S (A2-series). Fe atoms were confirmed to exclusively occupy an octahedral position in both series.

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The clathrate I superconductor Sr Si is obtained under high-pressure high-temperature conditions, at 5 GPa and temperatures in the range of 1273 to 1373 K. At ambient pressure, the compound decomposes upon heating at T=796(5) K into Si and SrSi . The crystal structure of the clathrate is isotypic to that of Na Si .

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The silicon-rich cage compound MgSi was obtained by high-pressure high-temperature synthesis. Initial crystal structure determination by electron diffraction tomography provided the basis for phase analyses in the process of synthesis optimization, finally facilitating the growth of single crystals suitable for X-ray diffraction experiments. The crystal structure of MgSi (space group Cmme, Pearson notation oS24, a=4.

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Synthetic bulk and natural pyrite from the hydrothermal mine in Schönbrunn (Saxony, Germany) are confirmed to be stoichiometric FeS2 compounds and stable (for thermoelectric applications) up to ∼600 K by combined thermal, chemical, spectroscopic and X-ray diffraction analyses. Natural pyrite with a small amount (<0.6 wt%) of well-defined transition metal carbonates revealed characteristics of a nondegenerate semiconductor and is suitable as a model system for the investigation of thermoelectric performance.

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The iron manganese nitride FeMnN was obtained by high-pressure-high-temperature synthesis from -FeN and elemental Mn at 15(2) GPa and 1573(200) K. The phase crystallizes isostructural to binary -FeN. In comparison to the corresponding binary iron nitride, the microhardness of -FeMnN is reduced to 6.

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Article Synopsis
  • BaSi₃ is synthesized under high pressures (12-15 GPa) and temperatures (800-1050 K) for one to five hours, then rapidly cooled.
  • It has a unique distorted structure resembling CaGe₃ and belongs to the space group 4¯ (no. 121).
  • At normal conditions (570 K), it decomposes exothermically into BaSi₂ and silicon-rich phases, exhibiting metallic properties through resistivity and magnetic susceptibility analysis.
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LuGe was obtained under high-pressure and high-temperature conditions at pressures between 8(1) and 14(2) GPa and at temperatures in the range from 1100(150) to 1500(150) K. The high-pressure phase is isotypic to DyGe and decomposes at ambient pressure and T = 690 K mainly into ( cF8)Ge and LuGe. Chemical bonding analysis of LuGe reveals two-center electron-deficient Ge-Ge bonds, multicenter polar Lu-Ge interactions, and lone pairs on germanium.

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The influence of Al incorporation on the heavy fermion superconductor UBe was investigated to explain the sample dependence of physical properties. Clear evidence for incorporated Al in flux-grown UBe single crystals is presented by results from X-ray diffraction, nuclear magnetic resonance and X-ray spectroscopy. The increase of the lattice parameter and the concomitant change of the superconducting properties are caused by substitution of Be in the compound by 1-2 at.

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Two new calcium nitridomanganates, Ca [Mn N ] (P3, a=11.81341(3) Å, c=5.58975(2) Å, Z=1) and Ca [Mn N ] (P3‾ , a=39.

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Materials with the crystal structure of γ-brass type (CuZn type) are typical representatives of intermetallic compounds. From the electronic point of view, they are often interpreted using the valence electron concentration approach of Hume-Rothery, developed previously for transition metals. The γ-brass-type phases of the main-group elements are rather rare.

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The superconducting properties of [Formula: see text]MoS [[Formula: see text]] Chevrel phase [[Formula: see text] K] are studied on a sample compacted by spark plasma sintering. Both lower ([Formula: see text] mT) and the upper [[Formula: see text] T] critical magnetic fields are obtained from magnetization and electrical resistivity measurements for the first time. The analysis of the low-temperature electronic specific heat indicates [Formula: see text]MoS to be a two band superconductor with the energy gaps [Formula: see text] meV (95%) and [Formula: see text] meV (5%).

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Hybrid organometallic systems offer a wide range of functionalities, including magnetoelectric (ME) interactions. However, the ability to design on-demand ME coupling remains challenging despite a variety of host-guest configurations and ME phases coexistence possibilities. Here, we report the effect of metal-ion substitution on the magnetic and electric properties in the paramagnetic ferroelectric NH(CH)Al Cr (SO) × 6HO.

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