Synthesis,Crystal Structure,and Optical Properties of (CH3NH3)2CoX4 (X = Cl,Br, I,Cl0.5Br0.5, Cl0.5I0.5, Br0.5I0.5)

The reaction of methylammonium halides and cobalt halides yielded the organic‐inorganic hybrid compounds of general formula (CH₃NH₃)₂CoX₄. By varying the different halides, we were able to synthesize the whole row from Cl to I as well as some mixed halides compounds and to determinate the crystal structures. (CH₃NH₃)₂CoX₄ (X = Cl, Br, Cl_0.5Br_0.5, Br_0.5I_0.5) crystallize isotypic to (CH₃NH₃)₂HgCl₄ in space group P2₁/c with Z = 4 [X = Cl: a = 7.6483(9), b = 12.6885(18), c = 10.8752(12) Å, β = 96.639(9)°; X = Cl_0.5Br_0.5: a = 7.8271(9), b = 12.9543(9), c = 11.1007(11) Å, β = 96.320(8)°; X = Br: a = 7.9782(2), b = 13.1673(2), c = 11.2602(2) Å, β = 96.3260(10)° and X = Br_0.5I_0.5: a = 8.2435(12), b = 13.645(2), c = 11.5856(18) Å, β = 95.54(2)°]. The mixed halides show a statistic distribution in both cases. In (CH₃NH₃)₂CoCl₂I₂ an ordered variant is realized representing a new structure type [C2/m, Z = 4, a = 18.808(4), b = 7.3604(7), c = 10.4109(17) Å, β = 120.364(13)°]. (CH₃NH₃)₂CoI₄ crystallizes again isotypic to the respective mercury compound [(CH₃NH₃)₂HgCl₄] [Pbca, Z = 8, a = 10.9265(5), b = 12.1552(5), c = 20.9588(9) Å]. All structures are build up by inorganic tetrahedral [CoX₄]^2– anions and organic (CH₃NH₄)⁺ cations. Additionally the Raman spectra as well as the optical reflectance spectra are discussed.     

Lead-Free,Water-Stable A3Bi2I9 Perovskites: Crystal Growth and Blue-Emitting Quantum Dots [A=CH3NH3+, Cs+, and (Rb0.05Cs2.95)+]

Despite the great success in the increase in the power conversion efficiency of lead halide perovskite solar cells, the toxicity of lead and the unstable nature of the materials are still major concerns for their wider implementation at the industrial level. Herein, large-size single crystals (SCs) are developed in HI solution by using a temperature lowering method and nanocrystals (NCs) of A₃Bi₂I₉ perovskites [where A=CH₃NH₃⁺ (MA)⁺, Cs⁺, and (Rb_0.05Cs_2.95)⁺] are formed in ethanol (EtOH) and toluene (TOL). The stability of A₃Bi₂I₉ perovskite is investigated by immersing the SCs for 24 h and pellets for 12 h in water. Moreover, the A₃Bi₂I₉ perovskite NCs displays a promising photoluminescence quantum yield of 17.63 % and a long lifetime of 8.20 ns.     

Phase transitions in perovskite-like oxyfluorides (NH4)3WO3F3 and (NH4)3TiOF5

Calorimetric and X-ray measurements have been performed on ammonium oxyfluorides (NH₄)₃WO₃F₃ and (NH₄)₃TiOF₅ from 120 up to 300 K. Two and one structural phase transitions were found for the former and latter compounds, respectively. In accordance with the entropy parameters both compounds undergo phase transitions of order–disorder type.     

Isotype Strukturen einiger Hexaamminmetall(II)-halogenide von 3d-Metallen: [V(NH3)6]I2, [Cr(NH3)6]I2, [Mn(NH3)6]Cl2, [Fe(NH3)6]Cl2, [Fe(NH3)6]Br2, [Co(NH3)6]Br2 und [Ni(NH3)6]Cl2

The Structures of some Hexaammine Metal(II) Halides of 3 d Metals: [V(NH₃)₆]I₂, [Cr(NH₃)₆]I₂, [Mn(NH₃)₆]Cl₂, [Fe(NH₃)₆]Cl₂, [Fe(NH₃)₆]Br₂, [Co(NH₃)₆]Br₂ and [Ni(NH₃)₆]Cl₂ Crystals of yellow [V(NH₃)₆]I₂ and green [Cr(NH₃)₆]I₂ were obtained by the reaction of VI₂ and CrI₂ with liquid ammonia at room temperature. Colourless crystals of [Mn(NH₃)₆]Cl₂ were obtained from Mn and NH₄Cl in supercritical ammonia. Colourless transparent crystals of [Fe(NH₃)₆]Cl₂ and [Fe(NH₃)₆]Br₂ were obtained by the reaction of FeCl₂ and FeBr₂ with supercritical ammonia at 400°C. Under the same conditions orange crystals of [Co(NH₃)₆]Br₂ were obtained from [Co₂(NH₂)₃(NH₃)₆]Br₃. Purple crystals of [Ni(NH₃)₆]Cl₂ were obtained by the reaction of NiCl₂ · 6H₂O and NH₄Cl with aqueous NH₃ solution. The structures of the isotypic compounds (Fm3 m, Z = 4) were determined from single crystal diffractometer data (see “Inhaltsübersicht”). All compounds crystallize in the K₂[PtCl₆] structure type. In these compounds the metal ions have high-spin configuration. The orientation of the dynamically disordered hydrogen atoms of the ammonia ligands is discussed.     

Untersuchungen an Polyhalogeniden III. Tetrammin-kupfer(II)-tetraiodid, [Cu(NH3)4I2 · I2], und Tetrammin-kupfer(II)-hexaiodid, [Cu(NH3)4I3]I3

Studies on Polyhalides. III. Crystal Structures of [Cu(NH₃)₄I₂ · I₂] and [Cu(NH₃)₄I₃]I₃ Tetramminecopper(II)tetraiodide [Cu(NH₃)₄I₂ · I₂] (I) crystallizes monoclinically in the space group C2/m with a = 1 185.9 pm, b = 892.8 pm, c = 656.8 pm, β = 111.10° and Z = 2 formula units. Tetramminecopper(II)hexaiodide [Cu(NH₃)₄I₃]I₃ (II) crystallizes orthorhombically in the space group Pnnm with a = 874.9 pm, b = 1 089.8 pm, c = 885.3 pm, and Z = 2 formula units. A special feature of these structures are coordinated polyiodide ions I₄^2? (I) or I₃^? (II). In both compounds four coplanar nitrogen atoms and two axial iodine atoms form a quasi-octahedral coordination around copper with the usual (4+2)-tetragonal distortion. The copper ions are connected by linear, centrosymmetric polyiodide ions I₄^2? (I) or I₃^? (II). Therefore infinite planar zigzag chains of units [Cu(NH₃)₄I₄] (I) or [Cu(NH₃)₄I₃]⁺(II) are resulting. The counterion I₃^? (II) is intercalated between these chains.     

Synthese und Kristallstruktur von (NH4)3Cu4Ho2Br13. Weitere Bromide vom Typ (NH4)3Cu4M2Br13 (M = Dy?Lu,Y) und Rb3Cu4Ho2Br13

Synthesis and Crystal Structure of (NH₄)₃Cu₄Ho₂Br₁₃. Further Bromides of the (NH₄)₃Cu₄M₂Br₁₃ Type (M = Dy? Lu, Y) and on Rb₃Cu₄Ho₂Br₁₃ Single crystals of (NH₄)₃Cu₄Ho₂Br₁₃ were obtained for the first time from the reaction of CuBr with HoBr₃ which was contaminated with NH₄Br: cubic, space group Pn3 , Z = 2, a = 1101.71(5) pm. The crystal structure may be considered as a variant of the fluorite type according to [(HoBr₆)₄][(NH₄)₆(Cu₄Br)₂] ? Ca₄F₈. Pure products can be prepared from the binary halides in glass ampoules at 350°C. The bromides (NH₄)₃Cu₄M₂Br₁₃ (M = Dy? Lu, Y) and Rb₃Cu₄Ho₂Br₁₃ are isotypic with (NH₄)₃Cu₄Ho₂Br₁₃.     

Completely Amine-Free Open-Atmospheric Synthesis of High-Quality Cesium Lead Bromide (CsPbBr3) Perovskite Nanocrystals

Cesium lead halide perovskite nanocrystals (NCs) CsPbX₃ (X=Cl, Br, and I) have been prominent materials in the last few years due to their high photoluminescence quantum yield (PLQY) for light-emitting diodes and other significant applications in photovoltaics and optoelectronics. In colloidal CsPbX₃ synthesis, the most commonly used ligands are oleic acid and oleylamine. The latter plays an important role in surface passivation but may also be responsible for poor colloidal stability as a result of facile proton exchange leading to the formation of labile oleylammonium halide, which pulls halide ions out of the NC surface. Herein, a facile, efficient, completely amine-free synthesis of cesium lead bromide perovskite nanocrystals using hydrobromic acid as halide source and tri-n-octylphosphane as ligand under open-atmospheric conditions is demonstrated. Hydrobromic acid serves as labile source of bromide ion, and thus this three-precursor approach (separate precursors for Cs, Pb, Br) gives more control than a conventional single-source precursor for Pb and Br (PbBr₂). The use of HBr paved the way to eliminate oleylamine, and thus the formation of labile oleylammonium halide can be completely excluded. Various Cs:Pb:Br molar ratios were studied and optimum conditions for making very stable CsPbBr₃ NCs with high PLQY were found. These completely amine-free CsPbBr₃ perovskite NCs synthesized under bromine-rich conditions exhibit good stability and durability for more than three months in the form of colloidal solutions and films, respectively. Furthermore, stable tunable emission across a wide spectral range through anion exchange was demonstrated. More importantly, this work reports open-atmosphere-stable CsPbBr₃ NCs films exhibiting strong PL, which can be further used for optoelectronic device applications.     

Kristallstruktur von (NH4)3SnF7: Ein Doppelsalz gemäß (NH4)3[SnF6]F und kein (NH4)4SnF8

Crystal Structure of (NH₄)₃SnF₇: A Double Salt According to (NH₄)₃[SnF₆]F and not (NH₄)₄SnF₈ (NH₄)₃SnF₇ is obtained as colourless single crystals from the reaction of NH₄HF₂ with tin powder at 300°C. The crystal structure (cubic, Pm3m, Z = 1, a = 602.5(1) pm at 293 K; a = 598.0(1) pm at 100 K) contains [SnF₆]^2? octahedra and lonesome F^? ions surrounded by NH₄⁺ cations only; it may be considered as a derivative of the Cu₃Au-type of structure according to Cu₃[Au]□ ?(NH₄)₃[SnF₆]F. The F^? ions of the [SnF₆]^2? octahedra with their Sn⁴⁺ centre in the origin of the unit cell at m3m are disordered in different ways at 293 and 100 K, respectively.     

NIR triggered NaYF4:Yb3+,Tm3+@NaYF4/CsPb(Br1-x/Ix)3 composite for up-converted white-light emission and dual-model anti-counterfeiting applications

Assembling nanomaterials from two classes with exceptional control at the nanoscale can lead to new nanohybrids with novel properties. Here, we report the tunable up-conversion luminescence properties of CsPb(Br_1-x/I_x)₃ perovskite nanocrystals (PeNCs) sensitized by NaYF₄:Yb,Tm@NaYF₄ up-conversion nanoparticles (UCNPs) at 980 nm excitation. The up-conversion luminescence of NaYF₄:Yb³⁺,Tm³⁺@NaYF₄/CsPb(Br_1-x/I_x)₃ composite demonstrates that the radiative photon reabsorption process is accountable for the UC energy transfer from excited levels of Tm³⁺-based UCNPs to PeNCs. The long-lived Tm³⁺ states feed PeNCs carriers with intrinsic lifetimes extending from nanoseconds to microseconds. By varying the UCNPs/PeNCs concentration ratio, the NaYF₄:Yb³⁺,Tm³⁺@NaYF₄/CsPb(Br_0.55I_0.45)₃ composite generates UC white light emission. The near-infrared excited white light-emitting devices are more compatible with human tissues than blue light-excited ones. Therefore, the prototype of UC white light-emitting diode is developed by coupling the UCNPs/PeNCs composite coated glass plate onto a commercial 940 nm-light-emitting diode chip. To overcome the counterfeiting risk that arises in the case of a single fluorescence mode, we developed a simple dual-model strategy based on manipulation of UC and down-conversion luminescence in anti-counterfeiting under 980 nm and 365 nm excitation, which makes it difficult to encrypt the information. In addition, the UCNPs/PeNCs composite exhibited better photostability under near-infrared illumination, retaining 85% of initial photoluminescence intensity, solving the problem of photo-instability.     

Synthese und Kristallstruktur von [Cr(NH3)6][Cr(NH3)2F4][BF4]2

Synthesis and Crystal Structure of [Cr(NH₃)₆][Cr(NH₃)₂F₄][BF₄]₂ The action of ammonium fluoride on a mixture of boron and chromium in a sealed Monel ampoule at 300 °C yields single crystals of [Cr(NH₃)₆][Cr(NH₃)₂F₄][BF₄]₂. The crystal structure (tetragonal, P4/mbm, Z = 2, a = 1056.0(1), c = 781.7(1) pm; R₁ = 0.0414; wR₂ = 0.1087 for 411 reflections with I₀ > 2σ(I)) contains [Cr(NH₃)₆]³⁺ and [Cr(NH₃)₂F₄]^– octahedra and twice as many [BF₄]^– tetrahedra that are arranged in a quadrupled super‐structure of the CsCl‐type of structure.     

Crystal Structure of Ni(NH3)Cl2 and Ni(NH3)Br2

Ni(NH₃)Cl₂ and Ni(NH₃)Br₂ were prepared by the reaction of Ni(NH₃)₂X₂ with NiX₂ at 350 °C in a steel autoclave. The crystal structures were determined by X‐ray powder diffraction using synchrotron radiation and refined by Rietveld methods. Ni(NH₃)Cl₂ and Ni(NH₃)Br₂ are isotypic and crystallize in the space group I2/m with Z = 8 and for Ni(NH₃)Cl₂: a = 14.8976(3) Å, b = 3.56251(6) Å, c = 13.9229(3) Å, β = 106.301(1)°; Ni(NH₃)Br₂: a = 15.5764(1) Å, b = 3.74346(3) Å, c = 14.4224(1) Å, β = 105.894(1)°. The crystal structures are built up by two crystallographically distinct but chemically mostly equivalent polymeric octahedra double chains [NiX_3/3X_2/2(NH₃)] (X = Cl, Br) running along the short b‐axis. The octahedra NiX₅NH₃ share common edges therein. The crystal structures of the ammines Ni(NH₃)_mX₂ with m = 1, 2, 6 can be derived from that of the halides NiX₂ (X = Cl, Br) by successive fragmentation of its CdCl₂ like layers by NH₃.     

[Pd(NH3)4][Ir0.5Os0.5Cl6] Solid Solution: Synthesis and Properties

[Pd(NH₃)₄][Ir_0.5Os_0.5Cl₆] solid solution, isomorphic to [Pd(NH₃)₄][IrCl₆], is synthesized and studied by X-ray powder diffraction and elemental analyses, IR and Raman spectroscopies.     

Tailored Engineering of an Unusual (C4H9NH3)2(CH3NH3)2Pb3Br10 Two‐Dimensional Multilayered Perovskite Ferroelectric for a High‐Performance Photodetector

Two‐dimensional (2D) layered hybrid perovskites have shown great potential in optoelectronics, owing to their unique physical attributes. However, 2D hybrid perovskite ferroelectrics remain rare. The first hybrid ferroelectric with unusual 2D multilayered perovskite framework, (C₄H₉NH₃)₂(CH₃NH₃)₂Pb₃Br₁₀ ( 1 ), has been constructed by tailored alloying of the mixed organic cations into 3D prototype of CH₃NH₃PbBr₃. Ferroelectricity is created through molecular reorientation and synergic ordering of organic moieties, which are unprecedented for the known 2D multilayered hybrid perovskites. Single‐crystal photodetectors of 1 exhibit fascinating performances, including extremely low dark currents (ca. 10⁻¹² A), large on/off current ratios (ca. 2.5×10³), and very fast response rate (ca. 150 μs). These merits are superior to integrated detectors of other 2D perovskites, and compete with the most active CH₃NH₃PbI₃.     

Über den thermischen Abbau einiger Alkalimetall- und Ammoniumhalogenoaurate(III) und die Kristallstruktur der Zersetzungsprodukte Rb2Au2Br6, Rb3Au3Cl8 und Au(NH3)Cl3

Thermal Decomposition of Some Alkali Metal and Ammonium Halogenoaurates(III), and the Crystal Structure of the Decomposition Products, Rb₂Au₂Br₆, Rb₃Au₃Cl₈, and Au(NH₃)Cl₃ The thermal decomposition of the salts MAuX₄ and M₂Au₂I₆, with M = K, NH₄, Rb; and X = Cl, Br; has been investigated. With the exception of NH₄AuCl₄ and KAuCl₄, all decompose with loss of halogen to the mixed valence compound M₃Au₃X₈, sometimes via the intermediate M₂Au₂X₆. Tetraiodoaurates are not stable at room temperature. In the decomposition of NH₄AuCl₄, HCl, and Au(NH₃)Cl₃ are formed. KAuCl₄ decomposes directly into Au und KCl. The crystal lattices of the salts Rb₂Au₂Br₆ and Rb₃Au₃Cl₈ are monoclinic and built up from Rb⁺. AuX₂^?, and AuX₄^? ions. There exists a close structural relationship between Rb₂Au₂Br₆, Cs₂Au₂Cl₆, and the perovskite structure. Rb₂Au₂I₆ is isotypic with Rb₂Au₂Br₆. The Rb₃Au₃Cl₈ structure type is also observed for the M₃Au₃X₈ salts with M = NH₄, K, Rb; and X = Br, I. In the structure of Au(NH₃)Cl₃ there are discrete molecules in which Au(III) is surrounded by 3 Cl and 1 N atoms in square coplanar coordination. The infrared spectra of these compounds are discussed.     

Synthese,Struktur und Thermolyse der ternären Ammoniumnitrate (NH4)3[M2(NO3)(9] (M  La?Gd)

Synthesis, Structure, and Thermolysis of the (NH₄)₃[M₂(NO₃)₉] (M ? La? Gd) The ternary ammonium nitrates (NH₄)₃[M₂(NO₃)₉] (M ? La-Gd) are obtained as single crystals from a solution of the respective sesquioxides in a melt of NH₄NO₃ and sublimation of the excess NH₄NO₃. In the crystal structure of (NH₄)₃[Pr₂(NO₃)₉] (cubic, P4₃32, Z = 4, a = 1 377.0(1) pm, R = 0.038, R_w = 0.023) Pr³⁺ is surrounded by six bidentate nitrate ligands of which three are bridging to neighbouring Pr³⁺ ions. This results in a branched folded chain, held together by the NH₄⁺ ions which occupy cavities in the structure. (NH₄)₃[Pr₂(NO₃)₉] is the first intermediate product of the thermal decomposition of (NH₄)₂[Pr(NO₃)₅(H₂O)₂] · 2H₂O.     

Pressure-Induced Perovskite-to-non-Perovskite Phase Transition in CsPbBr3

The expanding range of optoelectronic applications of lead-halide perovskites requires their production in diverse forms (single crystals, thin- and thick-films or even nanocrystals), motivating the development of diverse materials processing and deposition routes that are specifically suited for these structurally soft, low-melting semiconductors. Pressure-assisted deposition of compact pellets or thick-films are gaining popularity, necessitating studies on the pressure effects on the atomic structure and properties of the resulting material. Herein we report the phase transformation in bulk polycrystalline cesium lead bromide from its three-dimensional perovskite phase (γ-CsPbBr₃) into the one-dimensional polymorph (δ-CsPbBr₃) upon application of hydrostatic pressure (0.35 GPa). δ-CsPbBr₃ is characterized by a wide bandgap of 2.9 eV and broadband yellow luminescence at 585 nm (2.1 eV) originating from self-trapped excitons. The formation of δ-CsPbBr₃ was confirmed and characterized by Raman spectroscopy, ²⁰⁷Pb and ¹³³Cs solid-state nuclear magnetic resonance, X-ray diffraction, absorption spectroscopy, and temperature-dependent and time-resolved photoluminescence spectroscopy. No such phase transition was observed in colloidal CsPbBr₃ nanocrystals.     

Kristallstrukturanalyse von (NH4)2NaInF6

Single Crystal Structure of (NH₄)₂NaInF₆ (NH₄)₂NaInF₆ has been synthesized via a novel route from In₂O₃, NaF and NH₄F and its crystal structure has been determined using single crystal techniques (Fm3 m, a = 8.6675(3) Å, Z = 4, 4 106 reflections, R = 0.007). The crystal structure derives from the elpasolite type of structure, the ammonium ions are not disordered.     

Phase transitions and thermodynamic properties of (NH4)3VO2F4 cryolite

Calorimetric measurements performed in a wide temperature range on (NH₄)₃VO₂F₄ have shown the presence of four heat capacity anomalies at T₁ = 438 K, T₂ = 244 K, T₃ = 210.2 K, T₄ = 205.1 K associated with the first order phase transitions. In accordance with the permittivity behavior, the structural transformations are of nonferroelectric nature. Pressure dependence of the phase transition temperatures has been studied by DTA under pressure. The entropy of phase transitions is analyzed mainly in the framework of the orientational disordering of NH₄⁺ and VO₂F₄^3? ions in a cubic phase.     

Metallampullen als Mini‐Autoklaven: Synthese und Kristallstrukturen der Ammoniakate [Al(NH3)4Cl2][Al(NH3)2Cl4] und (NH4)2[Al(NH3)4Cl2][Al(NH3)2Cl4]Cl2

Metal Ampoules as Mini‐Autoclaves: Syntheses and Crystal Structures of [Al(NH₃)₄Cl₂][Al(NH₃)₂Cl₄] and (NH₄)₂[Al(NH₃)₄Cl₂][Al(NH₃)₂Cl₄]Cl₂ The salts [Al(NH₃)₄Cl₂]⁺[Al(NH₃)₂Cl₄]^–≡AlCl₃ · 3 NH₃ ( 1 ) and (NH₄⁺)²[Al(NH₃)₄Cl₂]⁺[Al(NH₃)₂Cl₄]^–(Cl^–)₂≡ AlCl₃ · 3 NH₃ · (NH₄)Cl ( 2 ) have been obtained as single crystals during the reactions of aluminum and aluminum trichloride, respectively, with ammonium chloride in sealed Monel metal containers. The crystal structure of 1 was determined again [triclinic, P‐1; a = 574.16(10); b = 655.67(12); c = 954.80(16) pm; α = 86.41(2); β = 87.16(2); γ = 84.89(2)°], that of 2 for the first time [monoclinic, I2/m; a = 657.74(12); b = 1103.01(14); c = 1358.1(3) pm; β = 103.24(2)°].     

Studies on the Chemistry of [Cd(NH3)4](MnO4)2. A Low Temperature Synthesis Route of the CdMn2O4+x Type NOx and CH3SH Sensor Precursors

Abstract. [Tetraamminecadmium(II)] bis(permanganate) ( 1 ) was prepared and its crystal structure was elucidated with XRD‐Rietveld refinement and vibrational spectroscopic methods. Compound 1 has a cubic lattice consisting of a 3D hydrogen‐bonded network built as four by four distorted tetrahedral blocks of [Cd(NH₃)₄]²⁺ cations and MnO₄^– anions, respectively. The other four permanganate ions are located in a crystallographically different environment, placed in the cavities formed by the attachment of the building blocks. A low‐temperature (≈100 °C) solid phase quasi‐intramolecular redox reaction producing ammonium nitrate and amorphous CdMn₂O₄ could be established. Neither solid phase nor aqueous solution phase thermal deammoniation of compound 1 can be used to prepare Cd(MnO₄)₂ and [Cd(NH₃)₂(MnO₄)₂]. During deammoniation of compound 1 in aqueous solution a precipitate consisting of Cd(OH)₂ forms. Additionally, solid MnO₂ and ammonium permanganate (NH₄MnO₄) forms. The solid phase deammoniation reaction (toluene used as heat convecting medium) with subsequent aqueous leaching of the ammonium nitrate formed has proved to be an easy and convenient technique for the synthesis of amorphous CdMn₂O_4+x type NO_x and MeSH sensor precursors. The 1 ‐ D perdeuterated complex was also synthesized to distinguish the N–H(D) and O–H(D) fragment signals in the TG‐MS spectra and to elucidate the vibrational characteristics of the overlapping Mn–O and Cd–N frequencies.