Ba6(MN4)N2–x (M = MoVI/TaV), a Subvalent Nitridometalate with Perovskite‐like Crystal Structure

The subvalent nitridometalate Ba₆[(Mo_1–xTa_x)N₄]N_0.86 was prepared from mixtures of Mo powder with Ba, Na, and Ba₂N at 600 °C in Ta ampoules. It crystallizes in space group Cmcm with a = 11.672(3), b = 10.177(2) and c = 10.8729(19) Å. Its crystal structure exhibits an orthorhombically distorted Perovskite topology with [Ba₆N] building units forming the ReO₃‐type lattice via common vertices, and the nitridometalate anions occupying half of the available distorted cuboctahedral interstices. [MN₄] anions show statistically mixed occupancy of M by Mo^VI and Ta^V. They show no notable deviation from nitridometalate anions in known ionic nitridomolybdates and ‐tantalates, and the metrics of the [Ba₆N] octahedra correspond to those found in similar subvalent compounds. The nitrogen atom position centering the [Ba₆N] octahedra is underoccupied. Band structure calculations corroborate the subvalent character of the compound and the two individual anionic structural building units.     

A New Sodium Borate: Na[B6O8(OH)3]·6H2O·H3BO3

The structure of [B₆H₉NaO₁₄, H₃BO₃, 6H₂O] was determined by single‐crystal X‐ray diffraction and further analyzed by FTIR spectroscopy and differential thermal/thermogravimetric analysis. The asymmetric unit contains Na–O polyhedra (distorted octahedron), [B₆O₈(OH)₃]^– fundamental building blocks, one free water molecule and one free H₃BO₃ molecule. In the hexaborate anion, three B₃O₃ rings are linked by a common oxygen atom with five trigonal and one tetrahedral boron atoms. The hexaborate group is also linked to the oxygenated environment of the sodium atom by three other six‐membered rings, each of which involve two boron atoms, three oxygen atoms, and sodium as the joint atom.     

La3B6O13(OH): The First Acentric High-Pressure Borate Displaying Edge-Sharing BO4 Tetrahedra

La₃B₆O₁₃(OH) was obtained by a high-pressure/high-temperature experiment at 6 GPa and 1673 K. The compound crystallizes in the space group P2₁ (no. 4) with the lattice parameters a=4.785(2), b=12.880(4), c=7.433(3) Å, and β=90.36(10)°, and is built up of corner- as well as edge-sharing BO₄ tetrahedra. It represents the first acentric high-pressure borate containing these B₂O₆ entities. The compound develops borate layers of „sechser“-rings with the La³⁺ cations positioned between the layers. Single-crystal and powder X-ray diffraction, vibrational and MAS NMR spectroscopy, second-harmonic generation (SHG) and thermoanalytical measurements, as well as computational methods were used to affirm the proposed structure and the B₂O₆ entities.     

Ba2Cd(B3O6)2: A Congruent‐Melting Compound with Isolated B3O6 Units

The single crystals of Ba₂Cd(B₃O₆)₂ were grown by the spontaneous crystallization method for the first time. They crystallize in the centrosymmetric trigonal space group R$\bar{3}$ with a = 7.143(3) Å, c = 17.405(16) Å, and Z = 3. The structure is characterized by isolated B₃O₆ units, and the Ba²⁺ and Cd²⁺ cations connect with B₃O₆ rings to form three dimensional structure. The TG/DSC and XRD results reveal that Ba₂Cd(B₃O₆)₂ melts congruently. First‐principles electronic structure calculation performed with the density functional theory (DFT) method shows that the calculated bandgaps are 4.66 eV, which is in good agreement with the UV/Vis/NIR experimental value 4.59 eV. The calculation shows that the Ba₂Cd(B₃O₆)₂ crystal has a large birefringence (Δn = 0.0875–0.0569 from 270 nm to 2600 nm), which demonstrates that Ba₂Cd(B₃O₆)₂ is a potential birefringence crystal.     

Sr3(BS3)2 und Sr3(B3S6)2: Zwei neue nicht‐oxidische Chalkogenoborate mit trigonal‐planar koordiniertem Bor

Sr₃(BS₃)₂ and Sr₃(B₃S₆)₂: Two Novel Non‐oxidic Chalcogenoborates with Boron in a Trigonal‐Planar Coordination The thioborates Sr₃(BS₃)₂ and Sr₃(B₃S₆)₂ were prepared from strontium sulfide, amorphous boron and sulfur in solid state reactions at a temperature of 1123 K. In a systematic study on the structural cation influence on this type of ternary compounds, the crystal structures were determined by single crystal X‐ray diffraction. Sr₃(BS₃)₂ crystallizes in the monoclinic spacegroup C2/c (No. 15) with a = 10.187(4) Å, b = 6.610(2) Å, c = 15.411(7) Å, β = 102.24(3)° and Z = 4. The crystal structure of Sr₃(B₃S₆)₂ is trigonal, spacegroup R3¯ (Nr. 148), with a = 8.605(1) Å, c = 21.542(4) Å and Z = 3. Sr₃(BS₃)₂ contains isolated [BS₃]^3— anions with boron in a trigonal‐planar coordination. The strontium cations are found between the layers of orthothioborate anions. Sr₃(B₃S₆)₂ consists of cyclic [B₃S₆]^3— anions and strontium cations, respectively.     

Silver Vanadyl(IV) ortho‐Pyrophosphate: Synthesis,Crystal Structure,and Characterization of the (V≡O)2+ Group

Ag₆(V^IVO)₂(PO₄)₂(P₂O₇) was obtained by reaction of Ag₃PO₄ and (VO)₂P₂O₇ (sealed ampoule, 550 °C, 3 d). The crystal structure of the new mixed ortho‐pyrophosphate was determined from X‐ray single‐crystal data [Pnma, Z = 4, a = 12.759(3) Å, b = 17.340(4) Å, c = 6.418(1) Å, R₁ = 0.071, wR₂ = 0.184 for 3174 unique reflections with F_o > 4σ(F_o), 141 variables]. Ag⁺ ions are located in between layers [(V^IVO)₂(PO₄)₂(P₂O₇)]^6–. Equilibrium relations of the new phosphate to neighboring phases were determined. The electronic structure of the (V^IV≡O)²⁺ group was investigated by polarized electronic absorption spectroscopy (ν̃_1a = 9450 cm^–1, ν̃_1b = 9950 cm^–1, ν̃₂ = 14750 cm^–1), EPR spectroscopy [X‐ and Q‐band, powder and single crystal, orthorhombic crystal g‐tensor with g₁ = 1.9445(3), g₂ = 1.9521(3), g₃ = 1.9695(3)], and magnetic measurements (powder, μ_exp/μ_B = 1.71, Θ_p = –1.7 K).     

Metallsalze des Benzol‐1, 2‐di(sulfonyl)amins. 9 [1, 2] Der Bariumkomplex [Ba{C6H4(SO2)2N}2(H2O)22: Ein säulenförmiges Koordinationspolymer mit lamellarer Kristallpackung

Metal Salts of Benzene‐1, 2‐di(sulfonyl)amine. 9. The Barium Complex [[Ba{C₆H₄(SO₂)₂N}₂(H₂O)2₂]: A Columnar Coordination Polymer with Lamellar Crystal Packing The title complex, obtained by treating ortho‐benzenedi‐sulfonimide with Ba(OH)₂ in aqueous solution, has been characterized by low‐temperature X‐ray diffraction (monoclinic, space group C2/c, Z = 4, Ba²⁺ on a crystallographic twofold axis). The cation attains a tenfold coordination by accepting bonds from two water molecules, four κ¹O‐bonding anions and two (O, N)‐chelating anions. The cation‐anion interactions create columnar strands parallel to the z axis, from which protrude twin stacks of benzo rings in the directions ±x, and water molecules and non‐coordinating sulfonyl oxygen atoms in the directions ±y. Adjacent strands related by translation parallel to y are associated via O(W)—H···O=S hydrogen bonds to form lamellar sandwich layers. The contiguous benzo rings of adjacent layers are markedly interlocked.     

Polysulfonylamine. CLVIII [1] Kristallstrukturen von Metall‐di(methansulfonyl)amiden. 9 [2] Erhöhung der Kristallsymmetrie durch Kokristallisation: Monoklines Na[(CH3SO2)2N]·H2O und tetragonales NaK[(CH3SO2)2N]2·2H2O

Polysulfonylamines. CLVIII. Crystal Structures of Metal Di(methanesulfonyl)amides. 9. Enhancing Crystal Symmetry by Co‐crystallization: Monoclinic Na[(CH₃SO₂)₂N]·H₂O and Tetragonal NaK[(CH₃SO₂)₂N]₂·2H₂O The three‐dimensional coordination polymers NaA·H₂O ( 1 ) and NaKA₂·2H₂O ( 2 ), derived from the strong NH acid (MeSO₂)₂NH = HA, have been characterized by single crystal X‐ray diffraction at —95 °C ( 1 : monoclinic, space group C2/c, Z′ = 2; 2 : tetragonal, P4₃2₁2, Z′ = 1). The results suggest that structures with Z′ > 1 are good candidates for co‐crystallization experiments. Both packings display layer substructures built up from the multidentately coordinating anions, the aquo ligands and two kinds of chemically and/or crystallographically distinct cations, whereas cations of a third type are intercalated between the layers. All anions have the extended standard conformation of this species; 1 contains two pseudo‐C₂ symmetric A^—, 2 one pseudo‐C₂ and two crystallographically C₂ symmetric A^—. Details for structure 1 : a) The layer‐forming Na(1) and Na(3) cations are distributed over three distinctly separated planes, Na(1) occupies general positions and has a non‐octahedral O₅N environment, Na(3) resides on inversion centres that generate an octahedral O₆ coordination; b) one independent A^— is oriented vertically, the other parallel to the layer plane; c) the intercalated Na(2) ions occupy twofold rotation axes within a single plane and possess a non‐octahedral O₆ environment. Details for structure 2 : a) The layer‐forming K(1) and K(2) cations occupy twofold rotation axes within a unique plane and have chemically identically O₆N₂ coordination polyhedra approximating to hexagonal bipyramids; b) all A^— are oriented vertically to the layer plane; c) the intercalated sodium ions reside on pseudo‐inversion centres, have an octahedral O₆ environment and are distributed over two closely adjacent planes. Owing to the enhanced packing efficiency of the bimetal complex, the vertical layer repeat‐distance is reduced from 1140 pm for 1 to 720 pm for 2 . Each structure exhibits an infinite cation‐water chain that propagates in the direction of the layer stacking and contains the three independent cations.     

Temperature‐Induced Intersite Charge Transfer Involving Cr ions in A‐Site‐Ordered Perovskites ACu3Cr4O12 (A=La and Y)

Changes in the valence state of transition‐metal ions in oxides drastically modify the chemical and physical properties of the compounds. Intersite charge transfer (ISCT), which involves simultaneous changes in the valence states of two valence‐variable transition‐metal cations at different crystallographic sites, further expands opportunities to show multifunctional properties. To explore new ISCT materials, we focus on A‐site‐ordered perovskite‐structure oxides with the chemical formula AA′₃B₄O₁₂, which contain different transition‐metal cations at the square‐planar A′ and octahedral B sites. We have obtained new A‐site‐ordered perovskites LaCu₃Cr₄O₁₂ and YCu₃Cr₄O₁₂ by synthesis under high‐pressure and high‐temperature conditions and found that they showed temperature‐induced ISCT between A′‐site Cu and B‐site Cr ions. The compounds are the first examples of those, in which Cr ions are involved in temperature‐induced ISCT. In contrast to the previously reported ISCT compounds, LaCu₃Cr₄O₁₂ and YCu₃Cr₄O₁₂ showed positive‐thermal‐expansion‐like volume changes at the ISCT transition.     

UV nonlinear optical crystal Ba2[B6O9(OH)4] featuring unique chiral layers with a new B18O42 circle based on BO3 and BO4 units

A new noncentrosymmetric polyborate, Ba(2)[B(6)O(9)(OH)(4)], has been synthesized under a hydrothermal condition. The polyborate contains chiral layers constructed by two kinds of helical chains and also form new B(18)O(42) circles based on B(3)O(8) units [(3: Δ+2T)]. One kind of Ba atom locates in the cavity surrounded by the B(11)O(11) ring within the anion layer, and the other kind of Ba atom inserts between two adjacent layers. UV-vis diffuse reflectance spectroscopy demonstrates that the compound has a cutoff edge below 190 nm and has a large second-harmonic generation (SHG) effect, which is approximately 3 times that of KH(2)PO(4) (KDP) and is type-I phase matchable.     

Assembly of a New Cyano‐bridged 4f‐3d Dimer Sm(DMSO)4‐ (H2O)3Cr(CN)6 and Crystal Structure of [K3(18‐crown‐6)3‐(H2O)4]Cr(CN)6·3H2O

A new cyano‐bridged binuclear 4f‐3d complex Sm(DMSO)₄‐(H₂O)₃Cr(CN)₆ was synthesized and characterized by single crystal structure analysis. It crystallizes in monoclinic, space group P2₁ with a=0.9367(2) nm, b = 1.3917(3) nm, c = 1.1212(2) run, β = 99.88(3)° and Z = 2. In this binuclear complex, Sm atom is eight coordinated and linked to the Cr atom by a cyano bridge. The molecules packs to form 3D structure due to the hydrogen bonds among them. [K₃(18‐C‐6)₃(H₂O)₄]Cr(CN)₆·3H₂O (18‐C‐6 represents 18‐crown‐6‐ether) that was synthesized as a byproduct in the preparation of a Gd—Cr complex is also structurally characterized. Crystal data: triclinic, space group P‐l with a = 1.0496(7) nm, b= 1.1567(14) nm, c = 1.3530(13) nm, a = 94.15(9)°, β = 96.04(8)°, γ = 95.25(9)° and Z = l. [K₃(18‐C‐6)₃(H₂O)₄]‐Cr(CN)₆·3H₂O consists of ionic [K₃(18‐C‐6)₃(H₂O)₄]³⁺ and [Cr(CN)₆]^3‐ pairs, of which the [K₃(18‐C‐6)₃(H₂O)₄]³⁺ ion is a trinuclear duster connected by water, and K atoms are eight coordinated by eight oxygen atoms of one 18‐C‐6 and two water molecules.     

DFT study of 1‐D Li6Gd(BO3)3

Solid‐state calculations were performed with the program CASTEP to analyze some electronic structure features of the crystal compound Li₆Gd(BO₃)₃ (LIGDBO), which is known to be an efficient gamma radiation detector, in particular when doped with rare‐earth ions. The structure of this material displays a clear 1‐D preference, where chains of atoms are formed along one of the crystalline axes. These quasilinear chains are responsible for the energy transfer occurring in the system prior to the actual detection. To elucidate on some aspects of the former process, calculations based on a few cluster models were also carried out by means of the molecular program JAGUAR. One of our results corresponds to a theoretical absorption energy value close to that experimentally obtained. In our calculation, the absorption process seems to be associated with the formation of an excitonic magnon state. © 2003 Wiley Periodicals, Inc. Int J Quantum Chem, 2003     

Bariumstannat‐Pulver durch hydrothermale Synthese und durch Thermolyse von Bariumzinn(IV)‐glykolaten. Synthese und Struktur von [Ba(C2H6O2)4][Sn(C2H4O2)3] und [Ba(C2H6O2)2][Sn(C2H4O2)3]·CH3OH

Barium Stannate Powders from Hydrothermal Synthesis and by Thermolysis of Barium‐Tin(IV)‐Glycolates. Synthesis and Structure of [Ba(C₂H₆O₂)₄][Sn(C₂H₄O₂)₃] and [Ba(C₂H₆O₂)₂][Sn(C₂H₄O₂)₃]·CH₃OH The hydrothermal reaction as well as the microwave assisted hydrothermal reaction of SnO₂·aq with barium hydroxide gives Ba[Sn(OH)₆] ( 1 ) as powder with bar like particles. Compound 1 of the same morphology can also be isolated from a hydrothermal reaction of [Ba(C₂H₆O₂)₄][Sn(C₂H₄O₂)₃] ( 3 ). The reaction of SnO₂·aq with Ba(OH)₂·8H₂O in ethylene glycol yields the glycolate [Ba(C₂H₆O₂)₄][Sn(C₂H₄O₂)₃] ( 3 ), which forms in methanol the solvate [Ba(C₂H₆O₂)₂][Sn(C₂H₄O₂)₃]·CH₃OH ( 4 ). Compounds 1 , 3 and 4 react at different temperatures to BaSnO₃ ( 2 ) consisting of powders with different morphologies; because of the grain size of the resulting powders compounds 3 and 4 are suitable as precursor for the fabrication of corresponding ceramics.     

A Dynamic Crystal‐to‐Amorphous Transformation Microporous ZnII Mixed Neutral‐ligand Metal‐organic Polymer {[Zn(bpp)2(μ‐4,4′‐bipy)(H2O)2](ClO4)2·H2O}n

A new rarely reported Zn^II mixed‐polypyridine coordination polymer with both rigid and flexible spacers, {[Zn(bpp)₂(μ‐4,4′‐bipy)(H₂O)₂](ClO₄)₂ · H₂O}_n ( 1 ), has been synthesized and characterized by elemental analysis, IR‐, ¹H NMR‐, ¹³C NMR spectroscopy and single‐crystal X‐ray diffraction. The thermal stability of compound 1 was studied by thermal gravimetric (TG) and differential thermal analyses (DTA). The single‐crystal X‐ray structure of 1 shows that the complex has been formed from a 1D polymer as a result of bridging by the 4,4′‐bipy ligands. Solution and solid‐state luminescent spectra of the compound 1 indicate intense fluorescent emissions at ca. 353.6 and 468.8 nm, respectively. Removal of the interstitial water guest molecules results in a loss of crystallinity, but exposure to water vapor reestablishes the original structure, thus constituting 1 as a third‐generation porous framework.     

Chromhexacyano‐Komplexe: Die Kristallstrukturen der Cyanoelpasolithe (NMe4)2ACr(CN)6 (A = K,Cs) und der kubischen Bariumverbindung Ba3[Cr(CN)6]2 · 20 H2O

Chromium Hexacyano Complexes: The Crystal Structures of the Cyano Elpasolites (NMe₄)₂ACr(CN)₆ (A = K, Cs) and of the Cubic Barium Compound Ba₃[Cr(CN)₆]₂ · 20 H₂O The crystal structures of the cyano elpasolites (NMe₄)₂KCr(CN)₆ (a = 1527.3(1), b = 888.1(1), c = 1539.0(1) pm, β = 109.92(1)°; C2/c, Z = 4) and (NMe₄)₂CsCr(CN)₆ (a = 1278.9(1) pm; Fm3m, Z = 4), as well as of the cubic compound Ba₃[Cr(CN)₆]₂ · 20 H₂O (a = 1631.0(1) pm; Im3m, Z = 4) were determined by X‐ray methods with single crystals. Reasons for the enlarged distances within the [Cr(CN)₆]^3–‐octahedron of the K compound (Cr–C: 209.3 pm) compared to the observations within both cubic complexes (206.1 resp. 206.9 pm) are discussed in context with the tolerance factors of cyano elpasolites. As is the case there concerning the cyano bridges Cr–CN–A towards the alkali ions the novel structure type of the barium compound, too, exhibits nearly linear bridging towards Ba. It contributes, however, only four N ligands to the ninefold [BaN₄O₅] coordination; part of the aqua ligands show disorder (Ba–N: 287.5, Ba–O: 281/293 pm).