Kristallzucht und Strukturverfeinerung von Quecksilber(II)‐amidchlorid – HgClNH2

Crystal Growth and Refinement of the Crystal Structure of Mercury(II) Amide Chloride – HgClNH₂ Single crystals were prepared by recrystallization of HgClNH₂ from aqueous NH₃/NH₄⁺ solution at 160 °C. They were used for a single‐crystal X‐ray structure redetermination. The previously reported [W. N. Lipscomb, Acta. Crystallogr. 1951 , 4, 266.] structural topology determined on basis of X‐ray powder diffraction data is now confirmed. However, a higher symmetry is found: Space group type Pmma (instead of Pmm2), a = 6.709(1) Å, b = 4.351(1) Å, c = 5.154(1) Å, Z = 2. The crystal structure contains zig‐zag‐chains [Hg(NH₂)_2/2]⁺. Four Cl atoms complete the coordination sphere of Hg to a distorted octahedron. These share common faces and edges in layers [HgCl_4/4(NH₂)_2/2]. These layers are connected via hydrogen bonds N–H…Cl.     

Die Kristallstruktur von BiNi: eine komplexe Ausdünnungsvariante des InNi2-Typs

The Crystal Structure of BiNi: a Complex Superstructure of the InNi₂ Structure Type Chemical transport reactions using bromine or iodine yielded crystals of BiNi with a largely ordered distribution of nickel atoms on octahedral and trigonal bipyramidal interstices within the hexagonal packing of bismuth atoms. The observed superstructure of the NiAs or InNi₂ structure types is described in the monoclinic space group F 1 2/m 1 (No. 12) with lattice parameters a = 1412.4(1), b = 816.21(6), c = 2142.9(2) pm, and β = 90°. The pseudo-orthorhombic cell facilitates twinning along [100]. Some crystals show an additional threefold twinning along [001]. The phase width of BiNi ranges from the nickel poor to the nickel rich region. In the vicinity of the stoichiometric composition BiNi, this has only an effect on the occupation of a single nickel position in the crystal structure.     

Thermodynamic Phase Transition Through Crystal‐to‐Crystal Process of Photochromic 1,2‐Bis(5‐phenyl‐2‐propyl‐3‐thienyl)perfluorocyclopentene

A photochromic diarylethene, 1,2‐bis(5‐phenyl‐2‐propyl‐3‐thienyl)perfluorocyclopentene ( 1a ), was found to have two polymorphic crystal forms, α‐ and β‐crystals. From X‐ray crystallographic analysis, the space groups of α‐ and β‐crystals were determined to be P2₁/c and C2/c, respectively. The difference between two crystal forms is ascribed to the orientation of two of four molecules in the unit cell. The thermodynamic phase transition from α‐ to β‐forms occurred via a crystal‐to‐crystal process, as confirmed by differential scanning calorimetry measurements, optical microscopic observations in the reflection mode and under crossed Nicols, and powder X‐ray diffraction measurements. The movement of the molecules in the crystal was evaluated by analyzing the change of face indices before and after the phase transition.     

Die trikline Kristallstruktur von Ag2Bi2S3Cl2: Pseudosymmetrie und Zwillingsbildung

Ruby‐red crystals of Ag₂Bi₂S₃Cl₂ were synthesized from AgCl and Bi₂S₃ by cooling a melt from 770 K to room temperature. X‐ray diffraction on powders and single‐crystals revealed a triclinic crystal structure with special lattice constants (P &1macr; (No. 2), a = 1085.0(2), b = 717.2(1), c = 1137.6(1) pm, α = 89.80(1)?, β = 74.80(1)?, γ = 87.81(1)?). In the structure [Bi^IIIS₃Cl₄] polyhedra form 2[BiS_3/2Cl_4/4]^‐ double‐layers by sharing common faces and edges. The silver(I) cations between the layers are coordinated either octahedrally by sulfide ions or tetrahedrally by sulfide and chloride ions. The deviations from the monoclinic space group P 1 2₁/c 1 are small and induce twinning along [010]. Further pseudosymmetry is based on the stacking of layer packages with the symmetry of the layer group P (2/c) 2₁/c 2/b.     

Abstandsvergleich M–H/M–D aus Röntgen‐ und Neutronenbeugungsdaten am Beispiel von Na3Rh(H/D)6

Comparison of the Distances M–H/M–D from X‐Ray and Powder Neutron Scattering Data on the Example of Na₃Rh(H/D)₆ Mixtures of NaNH₂, NaN₃ and Rh heated to 600 °C in autoclaves for salt melts show no indication of formation of ternary nitrides, but unexpectedly single crystals of a ternary hydride, Na₃RhH₆, were obtained. These crystals were isolated by washing the reaction product with liquid ammonia at room temperature. During this procedure metallic sodium – formed by decomposition of both the amide and the azide at elevated temperatures – is removed. X‐ray diffraction measurements on single crystals of Na₃RhH₆ allowed to even refine the displacement parameters of the hydrogen atoms and to compare the obtained results with data from powder neutron scattering of Na₃RhD₆ published by Bronger, Gehlen and Auffermann [1]. Only little differences are found between the lattice parameters, atomic positions and, noteworthy, the resulting distances Rh–H and Rh–D, respectively.     

A Water Sensitive Hydrate: The Bis‐Catena Complex Salt [Mn(H2O)6][BiI4]2·2H2O

Bright red crystals of [Mn(H₂O)₆][BiI₄]₂ · 2H₂O are obtained from a solution of MnI₂, BiI₃, and I₂ in absolute ethanol, which is exposed to humid air. Reversible dehydratization sets in at about 50 °C. Added water decomposes the hydrate by irreversible precipitation of BiOI. The optical bandgap is about 1.9(1) eV. X‐ray diffraction on a single‐crystal revealed a monoclinic lattice (space group P2₁/c) with a = 760.39(4) pm, b = 1315.6(1) pm, c = 1398.37(7) pm, and β = 97.438(4)°. In the crystal structure zigzag chains of edge‐sharing [BiI_2/1I_4/2]^– octahedra and linear strings of H₂O‐bridged [Mn(H₂O)₆]²⁺ octahedra run parallel [100].     

Structure of the Cu(II) chloride complex with 4-amino-l,2,4-triazole Cu(C2H4N4)Cl2

The coordination compounds of copper(II) chloride and bromide with 1,2,4-triazole (L¹) and 4-amino1,2,4-triazole (L²), CuL¹Hal₂ and CuL²Hal₂, possess interesting magnetic properties [1, 2]. For example, at very low temperatures CuL¹Cl₂ and CuL¹Br₂ are ferromagnets [2](T _c ≈ 3.3 and 6.5 K, respectively). To explain the magnetic behavior of copper(II) halide complexes with the above nitrogen heterocycles it is generally assumed that the complexes are polynuclear chain compounds in which the copper atoms are bridged by two halogen ions and bridging bidentate heterocycle molecules (coordination of N1 and N2 atoms). This hypothesis is made on the basis of the X-ray diffraction analysis of CuL¹Cl₂ [3]. It is interesting to perform an X-ray diffraction study of CuL²Cl₂ and CuL2Br2; this is important for obtaining reliable magnetostructural correlations for this group of compounds. In this study, we investigated single crystals of the complexes; this demanded choosing special conditions of synthesis, which differ from the conditions suggested for the synthesis of polycrystals in [1]. In this communication we report on the results of synthesis and X-ray diffraction analysis of the single crystals of the coordination compound CuL²Cl₂. Translated fromZhurnal Strukturnoi Khimii, Vol. 38, No. 1, pp. 207–212, January–February, 1997.     

Using Crystal Optics to Demonstrate Single‐Layer Localization of a Solid‐State Chain Reaction

Upon warming to 225 K, single crystals of 11‐bromoundecanoyl peroxide (BrUP), in which radicals have been created by photolysis at lower temperature, undergo partial decomposition by a radical chain reaction ca. 40 cycles long. FTIR allowed monitoring two chain products: CO₂ and an α‐lactone that decomposes further at 260 K. When initiation is confined to alternate molecular layers by polarized photoselection, the chain reaction reduces the crystal symmetry from tetragonal to monoclinic. Desymmetrization is easily observed by optical microscopy, although it is difficult to detect by X‐ray diffraction. Accurate monitoring of birefringence using a Sénarmont 1/4‐wave plate, and comparison with FTIR kinetics, proves that the chain reaction occurs within single molecular layers 2 nm thick.     

Die Kristallstruktur von [BeCl2(15‐Krone‐5)]

Crystal Structure of [BeCl₂(15‐Crown‐5)] Single crystals of [BeCl₂(15‐crown‐5)] ( 1 ) were obtained from dichloromethane solutions of BeCl₂ in the presence of the equivalent amount of 15‐crown‐5 and characterized by IR spectroscopy and X‐ray diffraction. Space group P2₁/c, Z = 4, lattice dimensions at 100 K: a = 1036.2(1), b = 1071.1(1), c = 1360.1(1) pm, β = 109.86(1)°, R₁ = 0.0225. The structure determination shows no disorder, all hydrogen positions were refined isotropically. The results are in contrast to the previously reported crystal structure determination in the space group P2₁nb. The beryllium atom of 1 forms a BeO₂C₂ five‐membered heterocycle with terminal chlorine atoms to give a distorted tetrahedral coordination with distances Be–O 166.5(2), 169.9(2) pm, and Be–Cl 195.8(2), 197.8(2) pm. The structural results are in good agreement with DFT calculations on B3LYP/6‐311+G** level.     

X‐Ray and Electron Diffraction Study of Poly(p‐dioxanone)

Summary: Solution‐grown lamellar crystals of poly(p‐dioxanone) (PPDX) have been crystallized isothermally from butane‐1,4‐diol at 100 °C. The crystal structure of PPDX has been determined by interpretation of X‐ray fiber diagrams of PPDX fibers and electron diffraction diagrams of lozenge‐shaped chain‐folder lamellar crystals. The unit cell of PPDX is orthorhombic with space group P2₁2₁2₁ and parameters: a = 0.970 nm, b = 0.742 nm, and c (chain axis) = 0.682 nm. There are two chains per unit cell, which exist in an antiparallel arrangement.

Transmission electron micrograph of PPDX chain‐folded lamellar crystals obtained by isothermal crystallization and its electron diffraction diagram.     

A combined crystallographic,thermal, Raman and computational study on polymorphism and phase transition in 1‐(4‐hexyloxy‐3‐hydroxyphenyl)ethanone

The crystal structure of the triclinic polymorph of 1‐(4‐hexyloxy‐3‐hydroxyphenyl)ethanone, C₁₄H₂₀O₃, differs markedly from that of the orthorhombic polymorph [Manzano et al. (2015). Acta Cryst. C 71 , 1022–1027]. The two molecular structures are alike with respect to their bond lengths and angles, but differ in their spatial arrangement. This gives rise to quite different packing schemes, even if built up by similar chains having the hydroxy–ethanone O—H…O hydrogen‐bond synthon in common. Both phases were found to be related by a first‐order thermally driven phase transformation at 338–340 K, which is discussed in detail. The relative stabilities of both polymorphs are explained on the basis of both the noncovalent interactions operating in each structure and quantum chemical calculations. The polymorphic phase transition has also been studied experimentally by means of differential scanning calorimetry (DSC) experiments, conducted on individual single crystals, Raman spectroscopy and controlled heating under a microscope of individual single crystals, which were further characterized by powder and single‐crystal X‐ray diffraction.     

The perchlorotriphenylmethyl (PTM) radical

In spite of the considerable understanding and development of perchlorotriphenylmethyl (PTM) radical derivatives, the preparation of crystals of the pure unsubstituted PTM radical, C₁₉Cl₁₅, suitable for single‐crystal X‐ray diffraction has remained a challenge since its discovery, and only two studies dealing with the crystal structure of the unsubstituted PTM radical have been published. In one study, the radical forms clathrates with aromatic solvents [Veciana, Carilla, Miravitlles & Molins (1987). J. Chem. Soc. Chem. Commun. pp. 812–814], and in the other the structure was determined ab initio from powder X‐ray diffraction data [Rius, Miravitlles, Molins, Crespo & Veciana (1990). Mol. Cryst. Liq. Cryst. 187 , 155–163]. We report here the preparation of PTM crystals for single‐crystal X‐ray diffraction and their resolution. The structure, which shows monoclinic symmetry (C2/c), revealed a nonsymmetric molecular propeller conformation (D₃ symmetry) caused by the steric strain between the ortho‐Cl atoms, which protect the central C atom (sp²‐hybridization and major spin density) and give high chemical and thermal persistence to the PTM. The supramolecular structure of PTM shows short Cl...Cl intermolecular interactions and can be described in terms of layers formed by rows of molecules positioned in a head‐to‐tail manner along the c axis.     

The three‐dimensional intermolecular network formed via water molecules in trans‐bis(nitrito‐κN)tetrakis(pyridine‐κN)ruthenium(II) dihydrate

The molecular geometry of the tetragonal crystal structure of the title compound, [Ru(NO₂)₂(C₅H₅N)₄]·2H₂O, differs from that previously determined by powder diffraction [Schaniel et al. (2010). Phys. Chem. Chem. Phys. 12 , 6171–6178]. In the [Ru(NO₂)(C₅H₅N)₄] molecule, the Ru atom lies at the intersection of three twofold axes (Wyckoff position 8b). It is coordinated by four N atoms of the pyridine rings, as well as by two N atoms of N‐nitrite groups. The last two N atoms are located on a twofold axis (Wyckoff position 16f). The O atoms of the water molecules are situated on a twofold axis (Wyckoff position 16e). Short intermolecular contacts are observed in the crystal structure, viz. N—O...OW and N—O...H—OW contacts between nitrite and water, and weak C—H...OW hydrogen bonds between pyridine and water. Thus, the intercalated water molecules act as bridges connecting the trans‐[Ru(NO₂)₂(py)₄] molecules into a three‐dimensional network.     

The crystal structure of [1.1.1]propellane at 138 K

The molecular structure of [1.1.1]propellane has been determined from single-crystal X-ray diffraction measurements at 138 K. The crystals of this reactive compound were grown from the melt at ca. 263 K. The space group is C2, and the asymmetric unit contains four molecules. All have large thermal motion and two show orientational disorder as well. Because of these problems, the atomic positions cannot be determined with high accuracy. Within the experimental limits, the two ordered molecules have D_3h symmetry, with corrected lengths of central and side bonds of ca. 1.60 Å and 1.53 Å, respectively. At lower temperature, the crystals undergo a phase transition. The transition temperature, in the range of 100 to 132 K, varied from one crystal sample to another. All crystals obtained of the low-temperature phase were twinned, and its space group could not be established.     

[WNCl3 · 0,5 HN3]4; Kristallstruktur und IR-Spektrum

[WNCl₃ · 0.5 HN₃]₄: Crystal Structure and I.R. Spectrum [WNCl₃ · 0.5 HN₃]₄ is formed from tungsten hexachloride and iodine azide in dichloro methane solution yielding dark red and needleshaped crystals. The crystal structure was determined by aid of X-ray diffraction data. The compound crystallises in the triclinic space group P1 with one formula unit per unit cell (R = 0.08, 2 811 independent reflexions). The four metal atoms are arranged in a square, the edges being formed by almost linear W?N? W bridge bonds of alternating length (168 and 210 pm). Two opposite tungsten atoms are coordinated by theαN atom of a HN₃ molecule and by three terminal chloro ligands. The other tungsten atoms achieve coordination number 6 by two terminal and two bridging Cl atoms, linking the tetrameric units to bands along [010]. The i.r. spectrum is reported and assigned.     

Synthese und Kristallstrukturen von 1,1,3,3‐Tetramethylimidazolinium‐dichlorid und 1,1,4‐Trimethylpiperazinium‐chlorid

Synthesis and Crystal Structures of 1,1,3,3‐Tetramethylimidazolinium Dichloride and 1,1,4‐Trimethylpiperazinium Chloride Single crystals of 1,1,3,3‐tetramethylimidazolinium dichloride ( 1 ) and 1,1,4‐trimethylpiperazinium chloride ( 2 ) were obtained by reaction of CH₂Cl₂ with tetramethylethylenediamine (TMEDA) and NNN′N″N″‐pentamethyldiethylenetriamine (PMDETA), respectively. Both compounds are characterized by single crystal X‐ray diffraction and by IR spectroscopy. 1: [C₇H₁₈N₂]Cl₂, space group P2₁/c, Z = 4, lattice dimensions at 193(2) K: a = 821.97(11), b = 1130.38(8), c = 1143.08(13) pm, β = 100.348(15)°, R₁ = 0.0271. The C₇N₂ heterocyclic ring has envelope conformation like other salts with this dication. 2: [C₇H₁₇N₂]Cl, space group P2₁2₁2₁, Z = 4, lattice dimensions at 100(2) K: a = 1030.37(8), b = 1036.55(6), c = 831.39(4) pm, R₁ = 0.0180. Although the heterocyclic mono‐cation is without site symmetry in the crystal, its molecular symmetry is close to C_s, forming chair conformation of the C₄N₂ six‐membered ring.     

Mixed‐chalcogenide double‐butterfly complex [{(CO)6Fe2SSe}2{μ‐­C(H)—C(H)}]

Bubbling acetyl­ene gas slowly through a methanol solution of [(CO)₆Fe₂{μ‐SSe}] containing sodium acetate for 48 h at room temperature yields the double‐butterfly complex μ‐[ethane‐1,1,2,2‐tetra(selenido/sulfido)]bis[hexacarbonyldiiron(Fe—Fe)], [Fe₄(C₂H₂S₂Se₂)(CO)₁₂]. The molecular structure was established by single‐crystal X‐ray diffraction techniques. The structure consists of two Fe₂SSe butterfly units linked to each other through a bridging HC—CH group. The mol­ecule has twofold symmetry and the two Fe atoms have distorted octahedral geometries.     

Investigations on Preparation,Crystal Structure and Thermal Stability of Bis(O-ethylcarbonodithiolato-S,S′)(1,10-phenanthroline-N~1,N~(10))cobalt(II) Complex:[Co(Et-XA)_2·phen]·H_2O (XA=xanthate)

IntroductionTheincreasingcommercialvalueoftransitionmetalcomplexesofxanthateshasarousedconsiderableinterestintheirchemistry .Whiletheiranalyticalapplicationsarewellknown ,1theyarenowfindingextensiveuseinvulcan izationofrubber ,frothfloatationprocessforconcentrationofsulphideores ,asantioxidants ,lubricants ,2 ,3andhavebeenfoundtopossessfungicidalandinsecticidalactivi ties .4 Recently ,molecularrecognitionbetweenhostandguestmolecules ,inclusionphenomenaandnoncovalentmolecularinteractionarefunda…     

Bildung,Kristallstruktur und absolute Konfiguration von (−)-N-(Chloromethyl)galanthaminium-chlorid

Formation, X-Ray Crystal Structure, and Absolute Configuration of (?)-N-(Chloromethyl)galanthaminium Chloride The acetylcholinesterase inhibitor galanthamine ( 1 ), main alkaloid of several Narcissus species, readily forms a quaternary ammonium salt by reaction with the solvent CH₂Cl₂. The structure and absolute configuration of (?)-N-(chloromethyl)galanthaminium chloride ( 2 ) were determined by X-ray diffraction (R = 0.075 for 2775 observed independent reflexions) and NMR spectroscopy. The tetragonal crystals (space group P4₃) contain two crystallographically independent cations which do not differ significantly from one another. The CH₂Cl group is attached to the quaternary N-atom in stereospecific (R)-configuration. In the crystal, the configurational position of the Me group at the N-atom of 2 differs from that of the crystalline free base 1 . Hydrogen bonding is observed from the OH group at C(3) of 2 to the Cl^? anion or to the Cl-atom of an adjacent cation.     

Zur oxidativen Addition von 1-Halogenalk-1-inen – Synthese und Struktur von Phenylalkinylpalladium-Komplexen

On the Oxidative Addition of 1-Halogenalk-1-ynes – Synthesis and Structure of Phenylalkynylpalladium Complexes [Pd(PPh₃)₄] ( 2 ) reacts with IC≡CPh and ClC≡CPh in the sense of an oxidative addition to give trans-[Pd(C≡CPh)X(PPh₃)₂] (X = I: 3 a , X = Cl: 3 b ). As side products trans-[PdX₂(PPh₃)₂] (X = I: 4 a , X = Cl: 4 b ; < 10%) and PhC≡C–C≡CPh ( 5 ; X = I: ca 30%, X = Cl: < 4%) are formed. 3 a and 3 b were characterized by NMR (¹H, ¹³C, ³¹P) and IR spectroscopies as well as by X-ray single-crystal structure analyses. In the crystals of 3 a and 3 b isolated molecules were found. The Pd–C≡C–Ph unit is linear in 3 a and approximately linear in 3 b [Pd–C≡C 174.2(6)°, C≡C–C 179,0(7)°].