Synthesis and Characterization of the Rubidium Thiophosphate Rb6(PS5)(P2S10) and the Rubidium Silver Thiophosphates Rb2AgPS4, RbAg5(PS4)2 and Rb3Ag9(PS4)4

The metal thiophosphates Rb₂AgPS₄ ( 2 ), RbAg₅(PS₄)₂ ( 3 ), and Rb₃Ag₉(PS₄)₄ ( 4 ) were synthesized by stoichiometric reactions, whereas Rb₆(PS₅)(P₂S₁₀) ( 1 ) was prepared with excess amount of sulfur. The compounds crystallize as follows: 1 monoclinic, P2₁/c (no. 14), a = 17.0123(7) Å, b = 6.9102(2) Å, c = 23.179(1) Å, β = 94.399(4)°; 2 triclinic, P$\bar{1}$ (no. 2), a = 6.600(1) Å, b = 6.856(1) Å, c = 10.943(3) Å, α = 95.150(2)°, β = 107.338(2)°, γ = 111.383(2)°; 3 orthorhombic, Pbca (no. 61), a = 12.607(1) Å, b = 12.612(1) Å, c = 17.759(2) Å; 4 orthorhombic, Pbcm (no. 57), a = 6.3481(2) Å, b = 12.5782(4) Å, c = 35.975(1) Å. The crystal structures contain discrete units, chains, and 3D polyanionic frameworks composed of PS₄ tetrahedral units arranged and connected in different manner. Compounds 1 – 3 melt congruently, whereas incongruent melting behavior was observed for compound 4 . 1 – 4 are semiconductors with bandgaps between 2.3 and 2.6 eV and thermally stable up to 450 °C in an inert atmosphere.     

K9CeP4S16, a new thio­phosphate of cerium with discrete [Ce(PS4)4]9− anions

The structure of nona­potassium cerium tetra­phos­phorus hexa­deca­sulfide, a zero‐dimensional material isostructural with Rb₉CeP₄Se₁₆, is reported.     

A macrocycle-assisted nanoparticlization process for bulk Ag2S

We report herein a new nanoparticlization process for the bulk-to-nano transformation of Ag₂S by incorporating both top-down and bottom-up approaches. Bulk Ag₂S was dissolved in solution with the assistance of a macrocyclic ligand, hexamethylazacalix[6]pyridine (Py[6]), to produce polynuclear silver sulfide cluster aggregates. All Ag–S cluster aggregates obtained in three crystalline complexes were protected by Py[6] macrocycles. Removing the protective Py[6] macrocycles by protonation led to the generation of unconventional Ag–S nanoparticles with a large energy gap. Theoretical calculations by a hybrid DFT method demonstrated that the silver sulfide clusters with high Ag/S ratio exhibited more localized HOMO–LUMO orbitals, which consequently enlarged their band gap energies. These experimental and theoretical studies broaden our understanding of the fabrication of nanomaterials by virtue of the advantages of both bottom-up and top-down methods and meanwhile provide a viable means of adjusting the band gap of binary nanomaterials independent of their size.     

Molten Ag2SO4‐based Ion‐Exchange Preparation of Ag0.5La0.5TiO3 for Photocatalytic O2 Evolution

Ag_0.5La_0.5TiO₃ with an ABO₃ perovskite structure was synthesized by a newly developed ion‐exchange method. Molten Ag₂SO₄ instead of traditional molten AgNO₃ was used as Ag⁺ source in view of its high decomposition temperature (1052 °C), thereby guaranteeing the complete substitution of Ag⁺ for Na⁺ in Na_0.5La_0.5TiO₃ with a stable ABO₃ perovskite structure at a high ion‐exchange temperature (700 °C). Under full‐arc irradiation, the O₂‐evolution activity of Ag_0.5La_0.5TiO₃ was about 1.6 times that of Na_0.5La_0.5TiO₃ due to the optimized electronic band structures and local lattice structures. On the one hand, the substitution of Ag⁺ for Na⁺ elevated the VBM and thus narrowed the band gap from 3.19 to 2.83 eV, thereby extending the light‐response range and, accordingly, enhancing the photoexcitation to generate more charge carriers. On the other hand, the substitution of Ag⁺ for Na⁺ induced a lattice distortion of the ABO₃ perovskite structure, thereby promoting the separation and migration of charge carriers. Moreover, under visible‐light irradiation, Ag_0.5La_0.5TiO₃ displayed notable O₂ evolution whereas Na_0.5La_0.5TiO₃ showed little O₂ evolution, thus demonstrating that the substitution of Ag⁺ for Na⁺ enabled the use of visible light to evolve O₂ photocatalytically. This work presents an effective route to explore novel Ag‐based photocatalysts.     

Über die Trithiocyanatoargentate Rb2Ag(SCN)3 und Cs2Ag(SCN)3

On the Trithiocyanatoargentates Rb₂Ag(SCN)₃ and Cs₂Ag(SCN)₃ The trithiocyanatoargentates Rb₂Ag(SCN)₃ and CsAg(SCN)₃ are obtained by crystallization from highly concentrated aqueous solutions. In the crystal structures the Ag atoms are surrounded tetrahedrally by the S atoms of 4 SCN groups. These Ag(SCN)₄ tetrahedra are connected by common corners to polymer \documentclass{article}\pagestyle{empty}\begin{document}$ {}_\infty ^1 \left[{{\rm Ag}\left({{\rm SCN}} \right)_2 \left({{\rm SCN}_{2/2}} \right)} \right] $\end{document}¹[Ag(SCN)₂(SCN)_2/2] anion in Rb₂Ag(SCN)₃, whereas dimeric Ag₂(SCN)₆ anions were found in the Cs compound.     

Two new phosphate langbeinites,Rb2YbTi(PO4)3 and Rb2Yb0.32Ti1.68(PO4)3, investigated at 293 and 150 K

The rubidium ytterbium titanium phosphates Rb₂YbTi(PO₄)₃, (I), and Rb₂Yb_0.32Ti_1.68(PO₄)₃, (II), have been structurally characterized from X‐ray data collected at both 293 and 150 K. Compound (II) is blue owing to the presence of mixed‐valence titanium (41% Ti³⁺ + 59% Ti⁴⁺). Both (I) and (II) belong to the langbeinite structure type, with mixed Yb/Ti populations in the two crystallographically independent octahedral sites (of symmetry 3). Ytterbium favours one of these sites, where about two‐thirds of the Yb atoms are found. The O‐atom displacement parameters are large in both compounds at both temperatures.     

A new chalcogenide homologous series A2[M(5+n)Se(9+n)] (A = Rb, Cs; M = Bi, Ag, Cd)

The ternary and quaternary selenides, beta-CsBi3Se5, Rb2CdBi6Se11, CsAg(0.5)Bi(3.5)Se6, CsCdBi3Se6, Rb2Ag(1.5)Bi(7.5)Se13, and Cs2Ag(1.5)Bi(7.5)Se13, are all members of the new homologous series A2[M(5+n)Se(9+n)] and crystallize in structures related to each other in a systematic way; these compounds are mid gap semiconductors and are of interest as thermoelectric materials.     

Zur Kenntnis des Rb2PbO3-Typs: Über Rb2ZrO3, Rb2SnO3 und Rb2TbO3

According to X-ray powder work, orthorhombic Rb₂ZrO₃ [a = 10.7, b = 7.40, c = 5.87 Å] and Rb₂SnO₃ [a = 10.7, b = 7.49, c = 5.75 Å] are isotypic with Rb₂PbO₃. Discussion of different structural models and the Madelung Part of Lattice Energy (MAPLE) shows that the annormal Coordination Number of M⁴⁺ (CN = 5) is caused by the type of formula.     

Lithium Intercalation into ATi2(PS4)3 (A = Li,Na, Ag)

Comparison of the electrochemical insertion of lithium into ATi₂(PS₄)₃ with A = Li, Na, Ag and ATi₂(PO₄)₃ with Li, Ag is striking. Whereas only four lithium per formula unit (Li/f.u.) can be inserted reversibly into the phosphates, up to 7 and 10 Li/f.u. can be inserted reversibly in the thiophosphates with A = Li and Ag. Moreover, the Ag⁺ to Ag⁰ reduction in AgTi₂(PO₄)₃ is not reversible, but in AgTi₂(PS₄)₃ it is reversible. Strong hybridization of the Ag-5s and host antibonding bands stabilizes the formal valences Ag⁰, Ti⁺, and (PS₄)⁴⁻ in the discharged state of AgTi₂(PS₄)₃; but only the formal valence Ti²⁺ is accessible in LiTi₂(PS₄)₃. Unfortunately the large volume change associated with the lithium insertion renders the structure progressively more amorphous on cycling, which causes the capacity to fade quite dramatically on further cycling. The thiophosphates transform to the phosphates on heating in air.     

A new quaternary thiophosphate,RbNb2(S2)3(PS4)

The structure of the new quaternary thio­phosphate rubidium diniobium tris­(di­sulfide) tetra­thio­phosphate, RbNb₂(S₂)₃(PS₄), is made up of one‐dimensional [Nb₂(S₂)₃(PS₄)^?] chains along the [101] direction, and these chains are separated from one another by Rb⁺ ions. The chain is basically built up from [Nb₂S₁₂] units and tetrahedral [PS₄] groups. The [Nb₂S₁₂] units are linked together to form a linear [Nb₂S₉] chain by sharing the S–S prism edge. Short and long Nb—Nb distances [2.888 (2) and 3.760 (2) Å, respectively] alternate along the chain, and the anionic species S₂^2? and S^2? are observed.     

Über Hexafluoroindate(III): A2TllnF6 (A=Rb,Cs), (RbTI)BlnF6 (B= Na,Ag, K) und A2AglnF6 (A=Rb,TI,Cs)

On Hexafluoroindates(II1): A₂TlInF₆ (A = Rb, Cs), (RbTI)BInF₆ (B = Na, Ag, K), and A₂AgInF₆ (A = Rb, TI, Cs) By heating the binary components in a closed system are new prepared the compounds Rb₂AgInF₆, Rb₂CsInF₆, (RbTl)NaInF₆ (RbTI)AgInF₆, (RbTI)KInF₆, Tl₂AgInF₆, Cs₂AgInF₆ and Cs₂TlInF₆, all cubic, colourless Elpasolithes, as well as Rb₂TlInF₆, according to powder photographs tetragonal. The Madelung Part of Lattice Energy, MAPLE, is calculated and discussed.     

A new type of mixed anionic framework in microporous rubidium copper vanadyl(V) phosphate,Rb2Cu(VO2)2(PO4)2

In dirubidium copper bis[vanadyl(V)] bis(phosphate), Rb₂Cu(VO₂)₂(PO₄)₂, three different oxo complexes form an anionic framework. VO₅ polyhedra in a trigonal bipyramidal configuration and PO₄ tetrahedra share vertices to form eight‐membered rings, which lie in layers perpendicular to the a axis of the monoclinic unit cell. Cu atoms at centres of symmetry have square‐planar coordination and link these layers along [100] to form a three‐dimensional anionic framework, viz. [Cu(VO₂)₂(PO₄)₂]_∞²⁻. Intersecting channels in the [100], [001] and [011] directions contain Rb⁺ cations. Topological relations between this new structure type and the crystal structures of A(VO₂)(PO₄) (A = Ba, Sr or Pb) and BaCrF₂LiF₄ are discussed.     

Synthesis and crystal structure of a new representative of the Rb2U2MoO10 uranomolybdate series

A new representative of the Rb₂U₂MoO₁₀ uranomolybdate series, was synthesized; its single crystals were grown and studied by X-ray diffraction. The atomic crystal structure was solved: monoclinic system, space group P2₁/c, a = 8.542(1) Å, b = 15.360(2) Å, c = 8.436(1) Å, b = 104.279(3)°, R ₁ = 0.064 for 1817 independent reflections with F > 4σ(F). The crystal structure is built of negatively charged infinite corrugated [U₂MoO₁₀] _2∞ ^δ? layers, which are linked through rubidium cations arranged between them. The compound was studied by IR spectroscopy; the absorption bands in the spectrum were assigned.     

A new phosphate,KMgY(PO4)2, isostructural with xenotime

A new phosphate, KMgY(PO₄)₂, isostructural with xenotime, was firstly reported in detail. It crystallizes in tetragonal system with space group I4₁/amd (No. 141). The cell parameters were obtained from X-ray powder diffraction data with a=0.6886, c=0.6025 nm, Z=2. The proposed structure of KMgY(PO₄)₂ was further confirmed by its vibrational spectra, IR and Raman spectra, which were also compared with those of iso-structural YPO₄.     

A new binding mode for thio­sulfate in six‐coordinate poly­[[(1,10‐phenanthroline‐κ2N,N′)­cadmium(II)]‐μ‐thio­sulfato]

In the novel title six‐coordinate cadmium complex, [Cd(S₂O₃)(C₁₂H₈N₂)]_n, the anion binds to three different six‐coordinate cationic centres through all four external atoms, an unprecedented coordination mode for thio­sulfate metal‐organic complexes. This connectivity leads to strongly linked dimers, connected to form interleaved double chains, which in turn interact through remarkably short π–π bonds between their phenanthroline groups.     

Synthesis and characterization of six new quaternary actinide thiophosphate compounds: Cs(8)U(5)(P(3)S(10))(2)(PS(4))(6)(,) K(10)Th(3)(P(2)S(7))(4)(PS(4))(2), and A(5)An(PS(4))(3), (A = K, Rb, Cs; An = U, Th)

Six new actinide metal thiophosphates have been synthesized by the reactive flux method and characterized by single-crystal X-ray diffraction: Cs(8)U(5)(P(3)S(10))(2)(PS(4))(6) (I), K(10)Th(3)(P(2)S(7))(4)(PS(4))(2) (II), K(5)U(PS(4))(3) (III), K(5)Th(PS(4))(3) (IV), Rb(5)Th(PS(4))(3) (V), and Cs(5)Th(PS(4))(3) (VI). Compound I crystallizes in the monoclinic space group P2(1)/c with a = 33.2897(1) A, b = 14.9295(1) A, c = 17.3528(2) A, beta = 115.478(1) degrees, Z = 8. Compound II crystallizes in the monoclinic space group C2/c with a = 32.8085(6) A, b = 9.0482(2) A, c = 27.2972(3) A, beta = 125.720(1) degrees, Z = 8. Compound III crystallizes in the monoclinic space group P2(1)/c with a = 14.6132(1) A, b = 17.0884(2) A, c = 9.7082(2) A, beta = 108.63(1) degrees, Z = 4. Compound IV crystallizes in the monoclinic space group P2(1)/n with a = 9.7436(1) A, b = 11.3894(2) A, c = 20.0163(3) A, beta = 90.041(1) degrees, Z = 4, as a pseudo-merohedrally twinned cell. Compound V crystallizes in the monoclinic space group P2(1)/c with a = 13.197(4) A, b = 9.997(4) A, c = 18.189(7) A, beta = 100.77(1) degrees, Z = 4. Compound VI crystallizes in the monoclinic space group P2(1)/c with a = 13.5624(1) A, b = 10.3007(1) A, c = 18.6738(1) A, beta = 100.670(1) degrees, Z = 4. Optical band-gap measurements by diffuse reflectance show that compounds I and III contain tetravalent uranium as part of an extended electronic system. Thorium-containing compounds are large-gap materials. Raman spectroscopy on single crystals displays the vibrational characteristics expected for [PS(4)](3)(-), [P(2)S(7)](4-), and the new [P(3)S(10)](5)(-) building blocks. This new thiophosphate building block has not been observed except in the structure of the uranium-containing compound Cs(8)U(5)(P(3)S(10))(2)(PS(4))(6).