Double beryllium iodate dihydrates,M2Be(IO3)4·2H2O (M = K,NH4+, Rb): Preparation,X-ray powder diffraction and vibrational spectra

The solubilities in the three-component systems MIO₃–Be(IO₃)₂–H₂O (M = K, NH₄⁺, Rb, Cs) were studied at 25 °C by the method of isothermal decrease of supersaturation. It has been established that double salts, K₂Be(IO₃)₄·2H₂O, (NH₄)₂Be(IO₃)₄·2H₂O, and Rb₂Be(IO₃)₄·2H₂O, crystallize from the ternary solutions within wide concentration ranges. Both the X-ray powder diffraction and the spectroscopic studies (infrared and Raman) reveal that the title compounds are isostructural. They crystallize in the monoclinic space group P2/m with lattice parameters: K₂Be(IO₃)₄·2H₂O – a = 14.218(5) Å, b = 6.747(2) Å, c = 5.765(2) Å, β = 98.74(4)°, V = 546.6(2) Å³; (NH₄)₂Be(IO₃)₄·2H₂O – a = 14.414(4) Å, b = 6.838(2) Å, c = 5.947(2) Å, β = 99.52(4)°, V = 578.0(2) Å³; Rb₂Be(IO₃)₄·2H₂O – a = 14.423(4) Å, b = 6.867(2) Å, c = 5.743(3) Å, β = 98.15(3)°, V = 562.9(3) Å³.Infrared spectroscopic experiments show that comparatively strong hydrogen bonds are formed in the potassium and rubidium salts as deduced from the wavenumbers of ν_OD of matrix-isolated HDO molecules (isotopically dilute samples) owing to the strong Be–OH₂ interactions (synergetic effect). However, the IO₃⁻ ions in the ammonium compound are involved in hydrogen bonds with NH₄⁺ ions additionally to those with water molecules and as a result of these intermolecular interactions the proton acceptor strength of the iodate ions decreases (anti-cooperative effect), thus leading to the formation of weaker hydrogen bonds in this compound (bonds of moderate strength) as compared to those formed in the potassium and rubidium ones. The normal vibrations of other entities (IO₃⁻ ions and BeO₄ tetrahedra (skeleton vibrations)) are also discussed.     

Crystal structure,electronic structure and electrical conductivity of the antimony selenide BaLaSb2Se6

BaLaSb₂S₆ and BaLaSb₂Se₆ were prepared by heating the elements in the stoichiometric ratio under exclusion of air at 850 °C. Both chalcogenides adopt the KThSb₆Se₆ structure type, crystallizing in the space group P2₁/c (Z = 4) with a = 4.324(3) Å, b = 14.7057(16) Å, c = 15.910(2) Å, β = 92.741(3)°, Z = 4 for the sulfide and a = 4.4173(3) Å, b = 15.333(1) Å, c = 16.816(1) Å, β = 92.545(2)°, Z = 4 for the selenide. The structure of BaLaSb₂Se₆ is composed of ribbons of distorted SbSe₆ octahedra and Se₂^2? pairs. Electronic structure calculations show that the selenide is a semiconductor, in accord with the electrical conductivity measurement.     

Non-centrosymmetric sodium borate: Crystal growth,characterization and properties on Na2B4O12H10

In this study, both solvent evaporation and hydrothermal methods were employed to grow hydrated sodium borate crystals using NaOH and H₃BO₃ as reagents, and transparent and colorless single-crystals were successfully obtained with sizes up to 12 × 6 × 6 mm³ and 6 × 5 × 4 mm³, respectively. The structure is determined by single-crystal X-ray diffraction techniques. The title compound crystallizes in the trigonal space group R32, with a = 11.1042(16) Å, b = 11.1042(16) Å, c = 21.131(4) Å, Z = 9 and R₁ = 0.0322, wR₂ = 0.0840. Infrared and transmission spectra are presented for the reported material. The powder second-harmonic generation (SHG) intensity measured by the Kurtz-Perry method indicates that the SHG effect of Na₂B₄O₁₂H₁₀ is about one-third times that of KH₂PO₄ (KDP).     

Crystal structure and transport properties of Pd5HgSe

The Pd₅HgSe compound was synthesised by heating of stoichiometric mixture of elements at 400 °C by means of the evacuated silica glass tube technique. Its crystal structure was refined by Rietveld method from powder X-ray diffraction data. Pd₅HgSe adopts tetragonal symmetry, space group P4/mmm, unit cell parameters a = 4.0128(2) Å, c = 7.0378(6) Å, V = 113.33(2) Å³, Z = 1. The crystal structure of Pd₅HgSe is composed of alternating slabs of the AuCu₃-type cuboctahedra [HgPd₁₂] and the PtHg₂-type rectangular prisms [SePd₈]. The title compound crystallizes in the Pd₅TlAs structure type. The electric resistivity as well as the Seebeck coefficient measurements suggests semimetallic behaviour.     

New iodate materials as potential laser matrices. Preparation and characterisation of α-M(IO3)3 (M = Y,Dy) and β-M(IO3)3 (M = Y,Ce, Pr,Nd, Eu,Gd, Tb,Dy, Ho,Er). Structural evolution as a function of the Ln3+ cationic radius

Anhydrous yttrium iodate presents polymorphism; two crystalline phases are obtained under hydrothermal conditions. α-Y(IO₃)₃ crystallises in the monoclinic space-group P2₁/c with a three-dimensional structure, whereas β-Y(IO₃)₃ crystallises in the monoclinic space-group P2₁/n with a two-dimensional structure. The lattice parameters are a = 7.038(1) Å, b = 8.466(1) Å, c = 13.317(1) Å, β = 99.65(1)°, V = 782.3(2) Å³, Z = 4 for α-Y(IO₃)₃ and a = 8.685(1) Å, b = 5.964(1) Å, c = 14.958(1) Å, β = 96.99(2)°, V = 769.0(2) Å³, Z = 4 for β-Y(IO₃)₃. The α-form is isostructural with α-Dy(IO₃)₃ studied in this work and α-Ln(IO₃)₃ (Ln = Ce, Pr, Nd, Sm, Eu, Gd, Tb, Ho, Er, Tm, Yb, and Lu) already studied. The β-form is isostructural with β-Ln(IO₃)₃ (Ln = Ce, Pr, Nd, Eu, Gd, Tb, Dy, Ho and Er) studied in this work. The structural evolutions as a function of the Ln³⁺ cationic radius are studied. α-Y(IO₃)₃ and β-Y(IO₃)₃ present good thermal stability since they decompose at 600 °C. They are transparent up to 11.5 μm and they have good optical damage thresholds on powder.     

Solvothermal synthesis and structural characterization of a three-dimensional metal–organic polymer [NaZn(1,2,4-BTC)] (1,2,4-BTC=1,2,4-benzenetricarboxylate)

A new three-dimensional metal–organic polymer, [NaZn(1,2,4-BTC)] (where 1,2,4-BTC=1,2,4-benzenetricarboxylate), has been prepared under solvothermal conditions and characterized by single crystal X-ray diffraction. The compound crystallizes in the monoclinic space group P2₁/c, with cell parameters: a=9.7706(4) Å, b=12.3549(5) Å, c=6.8897(3) Å, β=91.640(2)°, V=831.35(6) Å³ and Z=4. In the three-dimensional structure of the compound, each Zn atom is five-coordinated in distorted trigonal bipyramidal geometry, while the sixfold coordination of Na corresponds to a slightly distorted triangular prism. The organic ligand, 1,2,4-BTC, shows a novel and unprecedented coordination mode: 11 bonds to 10 metals with each carboxylate function exhibiting different linkages. It remains stable when desolvated and when heated up to 410 °C.     

Two coordination polymers of manganese(II) isophthalate and their preparation,structures, and magnetic properties

Two manganese coordination polymers, [Mn₂(ip)₂(dmf)]·dmf (1) and [Mn₄(ip)₄(dmf)₆]·2dmf (2) (ip=isophthalate; dmf=N,N-dimethylformamide), have been synthesized and characterized. X-ray crystal structural data reveal that compound 1 crystallizes in triclinic space group P?1, a=9.716(3) Å, b=12.193(3) Å, c=12.576(3) Å, α=62.19(2)°, β=66.423(17)°, γ=72.72(2)°, Z=2, while compound 2 crystallizes in monoclinic space group Cc, a=19.80(3) Å, b=20.20(2) Å, c=18.01(3) Å, β=108.40(4)°, Z=4. Variable-temperature magnetic susceptibilities of compounds 1 and 2 exhibit overall weak antiferromagnetic coupling between the adjacent Mn(II) ions.     

Synthesis,growth, and characterization of a new NLO material 3-(2,3-dimethoxyphenyl)-1-(pyridin-2-yl)prop-2-en-1-one

3-(2,3-Dimethoxyphenyl)-1-(pyridin-2-yl)prop-2-en-1-one (DMPP) a potential second harmonic generating (SHG) has been synthesized and grown as a single crystal by the slow evaporation technique at ambient temperature. The structure determination of the grown crystal was done by single crystal X-ray diffraction study. DMPP crystallizes with orthorhombic system with cell parameters a = 20.3106(8) Å, b = 4.9574(2) Å, c = 13.4863(5) Å, α = 90°, β = 90°, γ = 90° and space group Pca2₁. The crystals were characterized by FT-IR, thermal analysis, UV–vis–NIR spectroscopy and SHG measurements. Various functional groups present in DMPP were ascertained by FTIR analysis. DMPP is thermally stable up to 80 °C and optically transparent in the visible region. The crystal exhibits SHG efficiency comparable to that of KDP.     

Crystal structure of a new lithium indium borate Li3InB2O6

Single crystals of synthetic Li₃InB₂O₆ were obtained by heating a mixture of Li₂CO₃, In₂O₃ and B₂O₃; its formula was determined by the resolution of the structure from X-ray diffraction data. The compound is monoclinic, space group P2₁/n; the unit cell parameters are a=5.168(5) Å, b=8.899(9) Å, c=10.099(10) Å, β=91.112(17)°; Z=4. The crystal structure was solved from 669 reflections until R=0.0249; it exhibits a three-dimensional framework of vertex-sharing InO₅ trigonal bipyramids and BO₃ triangles, which isolates Li ions in channels. This structure is characterized by unusual oxygenated environments of In cations and of one of the three Li cations, which are forming more or less regular trigonal bipyramids. This compound melts incongruently at 827 °C; the powder may be obtained by annealing at 750 °C a mixture of Li₂CO₃, In₂O₃ and B₂O₃.     

Single crystal growth and structural characterization of ternary transition-metal uranium oxides: MnUO4, FeUO4, and NiU2O6

Single crystals of MnUO₄, FeUO₄, and NiU₂O₆ were grown for the first time. The use of chloride fluxes facilitated the crystal growth. MnUO₄, a hexavalent uranium compound, crystallizes in the orthorhombic space group, Imma, with a = 6.6421(19) Å, b = 6.978(2) Å, and c = 6.748(2) Å, and exhibits typical uranyl, UO₂²⁺, coordination. FeUO₄ and NiU₂O₆ contain pentavalent uranium and are structurally related, exhibiting three-dimensional connectivity. FeUO₄ crystallizes in the orthorhombic space group, Pbcn, with a = 4.8844(2) Å, b = 11.9328(5) Å, c = 5.1070(2) Å. NiU₂O₆ crystallizes in the trigonal space group, P321, with a = 9.0148(3) Å, c = 5.0144(3) Å.     

Hydrothermal Synthesis and X‐ray Crystal Structure of Four Inorganic‐Organic Hybrid Compounds in Vanadium /Copper Iodate Family

Four inorganic‐organic hybrid compounds with the formulae (1,10‐phen)(VO₂)(IO₃) ( 1 ), (2,2′‐bipy)(VO₂)(IO₃) ( 2 ), [Cu₃(2,2′‐bipy)₃Cl₃(IO₃)₂]·I_1.5 ( 3 ), and [Cu(2,2′‐bipy)(H₂O)(IO₃)₂]· (H₂O)₂ ( 4 ) are hydrothermally synthesized at 120 °C for 6 d and characterized by single‐crystal X‐ray diffraction. The use of two different bidentate organodiamine ligands 1,10‐phen and 2,2′‐bipy in the V/I/O system gives rise to compounds 1 and 2 , which crystallize in a monoclinic system with the space group C2/c, a = 17.8131(6) Å, b = 15.0470(7) Å, c = 12.9902(4) Å, β = 133.095(2)°, V = 2542.49(17) ų for 1 and space group P2₁/c, a = 13.3095(5) Å, b = 15.0993(8) Å, c = 13.0454(4) Å, β = 116.971(2)°, V = 2335.88(17) ų for 2 . The use of the bidentate organodiamine ligand 2,2′‐bipy in the Cu/I/O system gives rise to the variety in the structure of products 3 and 4 , which crystallize in a triclinic system with the same space group . a = 8.5143(2) Å, b = 10.4908(3) Å, c = 22.8420(6) Å, α = 93.769(10)°, β = 91.723(10)°, γ = 112.111(10)°, V = 1882.83(9) ų for 3 and a = 6.731(6) Å, b = 10.110(4) Å, c = 12.899(6) Å, α = 106.00(5)°, β = 95.45(4)°, γ = 107.69(6)°, V = 788.4(9) ų for 4 . The solid‐state structures of the compounds 1 and 2 have chains with repeat units of alternative corner sharing of [VO₄N₂] octahedra and [IO₃] pyramids. Compound 3 is a chain containing [IO₃] pyramids and [VO₄N] square pyramids and compound 4 consists of Cu(2,2′‐bipy)²⁺ linked by one water molecule and two [IO₃] pyramids. The thermal stabilities of the compounds are investigated.     

Two new barium borate bromides: Ba2BO3Br and Ba3BO3Br3

Two new barium borate bromide crystals, Ba₂BO₃Br and Ba₃BO₃Br₃, have been obtained by spontaneous crystallization. Ba₂BO₃Br crystallizes in P−3m1 space group, with cell parameters of a = 5.5157(10) Å, c = 11.019(4) Å, and Z = 2, its structure is build up by alternately stacking along c-axis of [Ba₂(BO₃)₂]²⁻ layers and bromide [Ba₂Br₂]²⁺ layers. The solved structure is analog to Ba₂(BO₃)_1−x(CO₃)_xCl_1+x except the interstitial halogen atoms at (0, 0, 1/2) is missing and accordingly the partly CO₃ substitution for BO₃ has not been observed. Ba₃BO₃Br₃ crystallizes in a new structure type with P−1 space group and cell parameters of a = 9.280(4) Å, b = 9.349(7) Å, c = 13.025(9) Å, α = 92.71(3)°, β = 98.29(3)°, γ = 116.200(18)° and Z = 4. The basic structural unit in Ba₃BO₃Br₃ is the clusters composed of 4 BO₃ groups and 12 Ba atoms, which in turn are linked by eight Ba–O bonds with other four clusters to form sheets extend in the (001) plane.     

PM3 semiempirical study and its comparison with X-ray crystal structure of 2-methyl-4-(4-methoxyphenylazo)phenol

The crystal and molecular structure of 2-methyl-4-(4-methoxyphenylazo)phenol have been determined by X-ray single crystal diffraction technique. The compound crystallizes in the monoclinic space group P2₁/c with a=9.7763(8) Å, b=11.3966(8) Å, c=11.9531(8) Å and β=108.752(6)°. In addition to the molecular geometry from X-ray experiment, its optimized molecular structure has been obtained with the aid of PM3 semiempirical quantum mechanical method, and then the corresponding geometric parameters were compared with those of X-ray crystallography. To determine conformational flexibility and crystal packing effects on the molecules, molecular energy profile of the title compound was obtained with respect to two selected degrees of torsional freedom, which were varied from ?180° to +180° in steps of 10°. Crystal structure of the title compound is a fibroid structure constructed by C–H···O and O–H···N type intermolecular hydrogen bonds. The most favorable conformer of the title compound has been determined by the crystal packing effects and there is no steric hindrance during rotation around the selected torsion angles.     

Intercalation of KCl into layered neptunyl and plutonyl iodates

The hydrothermal reaction of Np(IV) or Pu(IV) with KIO₄ and CsCl at 180°C for 1 day results in the formation of NpO₂(IO₃)₂·0.5KCl·3.25H₂O (1) or PuO₂(IO₃)₂·0.5KCl·2.5H₂O (2). The neutral layers in compounds 1 and 2 are isostructural with NpO₂(IO₃)₂·H₂O and PuO₂(IO₃)₂·H₂O, respectively. The Np and Pu centers are found in distorted pentagonal bipyramidal [AnO₇] environments that are formed from the ligation of NpO₂²⁺ or PuO₂²⁺ cations by iodate anions. There are two crystallographically unique pyramidal iodate anions in 1 and 2. One of these anions utilizes all three oxygen atoms to simultaneously bridge three neptunyl or plutonyl units. The second anion only bridges two actinyl units and has a terminal oxo atom. The bridging of the actinyl cations by iodate anions creates neutral _∞²[AnO₂(IO₃)₃] (An=Np, Pu) sheets that are separated by K⁺ cations, Cl⁻ anions, and water molecules. Crystallographic data (203 K, MoKα, λ=0.71073): 1, monoclinic, space group C2/c,a=21.537(5) Å, b=11.670(3) Å, c=7.315(2) Å, β=93.033(4)°, Z=4, R(F)=5.43% for 136 parameters with 1309 reflections with I>2σ(I); 2, monoclinic, space group C2/c, a=21.570(4) Å, b=11.656(2) Å, c=7.348(2) Å, β=94.00(3), Z=4, R(F)=4.92% for 148 parameters with 1317 reflections with I>2σ(I).     

Bi2(IO3)(IO6): First combination of [IO3]− and [IO6]5− anions in three-dimensional framework

A new bismuth (III) iodate periodate, Bi₂(IO₃)(IO₆) was obtained from hydrothermal reactions using Bi(NO₃)₃·5H₂O, and H₅IO₆ as starting materials. Bi₂(IO₃)(IO₆) crystallizes in the monoclinic space group P2₁/c (No. 14) with lattice parameters ɑ = 8.1119(6), b = 5.4746(4), c = 16.357(1) Å, β = 99.187(2)°, V = 717.07(9) ų, Z = 4. The structure of Bi₂(IO₃)(IO₆) features a three-dimensional framework which is a combination of [Bi(1)O₅] tetragonal pyramids, [Bi(2)O₈] bicapped trigonal prisms and [IO₃]⁻ and [IO₆]⁵⁻ anions. Thermal analysis shows that the compound is thermally stable up to about 350 °C. The solid state UV-vis-NIR diffuse reflectance spectrum indicates that Bi₂(IO₃)(IO₆) is a semiconductor with a band gap of 2.76 eV.     

Hydrothermal synthesis, structure and thermal property of a 2-dimensional network: sodium sulfate [Ni(H2O)6(NaSO4)2]

The title compound of [Ni(H₂O)₆(NaSO₄)₂] has been synthesized under hydrothermal conditions and characterized by single crystal X-ray diffraction. The compound crystallizes in space group P2₁/c of the monoclinic system in a cell at 293.2 K of a=6.1820(12) Å, b=12.316(3) Å, c=9.0890(18) Å, β=106.03(3)°, and V=665.1(2) Å³. In the title compound, each SO₄ tetrahedron coordinates with three Na(I) ions and each Na(I) connects to three SO₄ tetrahedrons. Such a coordinate model makes up a two-dimensional network having two different kinds of rings and, in the bigger rings, the [Ni(H₂O)₆]²⁺ ions are located. In the solid state, some hydrogen bonds connect the title compound to form three-dimensional networks, stabilizing the crystal structure. Thermogravimetric analysis shows that there are three steps of weight loss from the beginning of 110 °C and the residue may be the mixtures of NiO₂ and Na₂O.     

Ca2CoNbO6: A new monoclinically distorted double perovskite

The new Ca₂CoNbO₆ double perovskites has been synthesized by solid-state reaction and its crystal structure has been refined using X-ray powder diffraction data. Rietveld fit to the diffraction data shows that the compound is monoclinically distorted and adopts space group P21/n. The cell parameters are: a = 5.4797(1) Å, b = 5.6051(1) Å, c = 7.8119(2) Å, β = 89.96(1)°. The Co and Nb are found to be distributed over the six coordinated octahedral sites in rock salt arrangement. However, nearly identical ionic radii of Co and Nb lead to severe degree of anti-site disorder (31%). The refined Co–O and Nb–O bond lengths are 1.9788(2) Å and 2.0642(2) Å respectively.     

Synthesis and structure of a new compound (NH4)3[{Ta2(NH)3Cl6}Cl], with a novel imido-bridged chain: 1∞[Ta2(NH)3Cl6]2−

A new imido-bridged tantalum compound, (NH₄)₃[{Ta₂(NH)₃Cl₆}Cl], was synthesized from the mixture of TaCl₅, NaNH₂ and NH₄Cl (excess) in a vacuum sealed silica tube at 350–400 °C. Single crystal X-ray diffraction results for the title compound detailed in the orthorhombic space group Cmcm (No. 63); Z=4, a=10.1601(6) Å; b=19.8834(13) Å; and c=7.4362(4) Å. The structure consists of imido-bridged one-dimensional chains with composition [Ta₂(NH)₃Cl₆]²⁻ and running along c. These chains are separated by ammonium and chloride ions. In the present study, NH₄Cl was used to facilitate relatively smooth reaction between TaCl₅ and NaNH₂, which otherwise leads to an exothermic, self-propagating reaction.     

Crystal structure of single crystals of nonlinear optical l-histidinium trichloroacetate

Single crystals of a new histidinium salt: l-histidinium trichloroacetate {abbreviated as LHTCA; [(C₃N₂H₄) CH₂CH (NH₃) (CO₂)]⁺ CCl₃COO⁻} were grown by slow evaporation of an aqueous solution at room temperature. The compound crystallizes in a non-centrosymmetric space group P2₁ of monoclinic system with cell parameters a = 5.4505(18) Å, b = 25.769(8) Å, c = 9.210(2) Å and β = 99.98(2)° with Z = 4. The structure has been refined to an R-value of 0.05 for 2539 observed reflections using three-dimensional X-ray diffraction data. The vibrational structure of the compound confirms the presence of various functional groups in the molecule. The UV–Vis–NIR spectrum shows a good transparency in the whole of the region from ultraviolet to near IR. The Kurtz–Perry powder SHG measurement confirms the frequency doubling of the crystal and its powder SHG efficiency was measured as d_eff = 0.33 d_eff (KDP).