22756-36-1Relevant articles and documents
RbBa2(N3)5: A new ternary azide
Vajenine, Grigori V.
, p. i85-i87 (2006)
Rubidium dibarium pentaazide, RbBa2(N3)5, was prepared from an aqueous solution of the binary azides at room temperature. It crystallizes in the monoclinic system (space group P2/n). Two central atoms of azide groups occupy the 2c (1) and 2b (1) positions, another azide group lies completely on a twofold axis (2f), while Rb atoms are situated in 2e (2) positions. The crystal structure of RbBa2(N 3)5 can be regarded as a distorted AlB7-type arrangement of the metal atoms, with the azide groups occupying the voids between the cations. This results in coordination numbers of 8 (Rb) and 10 (Ba). The N-N distances are in the range 1.169 (8)-1.190 (5) A, typical for the azide group.
A new polyoxocobaltate(II) anion in Rb2Co2O3
Sofin, Mikhail,Peters, Eva Maria,Jansen, Martin
, p. 2697 - 2700 (2002)
Rb2Co2O3 was prepared via the azide/nitrate route. Mixtures of the precursors Co3O4, RbN3 and RbNO3 in the molar ratios 6:17:1 were heated in a special regime up to 450°C and annealed at this temperature for 50 h in silver crucibles. Single crystals have been grown by subsequent annealing of prepared powder at 450°C for 500 h in silver crucibles, which were sealed in glass ampoules under dried Ar. According to the X-ray analysis of the crystal structure (Pnma, Z = 8, 11.729(2), 6.058 (1), 8.004(1) A) cobalt is trigonal planar coordinated by oxygen atoms. The CoO3-units share through all corners and build up an infinite two-dimensional ∞2Co2O3-network.
Synthesis and Structural Characterization of the layered Selenogallate RbGaSe2
Friedrich, Daniel,Schlosser, Marc,Pfitzner, Arno
, p. 1589 - 1592 (2017)
The chalcogenogallate RbGaSe2 was synthesized by thermal decomposition of rubidium azide in the presence of gallium selenide and selenium. RbGaSe2 crystallizes in the monoclinic space group C2/c (no. 15) with the lattice parameters a = 10.954(1) ?, b = 10.949(1) ?, c = 16.064(1) ?, β = 99.841(4)°, V = 1898.2(2) ?3, and Z = 16 (single-crystal data, 20 °C) in the TlGaSe2 structure type. Its crystal structure features anionic layers 2∞[Ga4Se84–] with a van der Waals distance of 3.30(1) ?. Thermal analysis revealed a melting point of about 930 °C. Using UV/Vis diffuse reflectance spectroscopy, a wide bandgap of 3.16 eV was determined for the colorless semiconductor. The bonding situation in the compound was further compared with the isotypic cesium phases based on the results from Raman spectroscopy and DFT calculations. The slight shifts of the Raman bands suggest a slightly higher covalency of the rubidium compound.
Alkali metal nitrido tecto metallates(VI) with networks of six-membered rings of corner-sharing tetrahedra [(MNN3/2)6] with M = Mo, W of the unexpected composition A9+x[M6N15] with A = Rb, Cs and 0 < x < 1
Stegen,Jacobs
, p. 639 - 644 (2000)
Reactions of metal powders of Mo and W respectively with amides and azides of Rb and Cs lead to the compounds Rb9+x[W6N15] and Cs9+x[M6N15] with M = Mo, W and 0 a matrix of the corresponding alkali metal. These metals result from the thermal decomposition of the amides and azides used in high molar ratios. The metals are washed out by liquid ammonia. Besides microcrystalline material of the above mentioned compounds single crystals suitable in size for x-ray structure determinations were isolated. The compounds crystallize in the space group R3c (No. 167) with Z = 6 and the following lattice constants: Rb9+x[W6N15]: a = 12.743(7) A, c = 27.794(8) A, c/a = 2.181 Cs9+x[Mo6N15]: a = 13.104(5) A, c = 28.430(9) A, c/a = 2.170 Cs9+x[W6N15]: a = 13.136(5) A, c = 28.472(6) A, c/a = 2.167 The metal centres of tetrahedra [MNN3/2] are condensated to cyclohexane analogue six-membered rings in chair-form via nitrogen atoms and axial ones connect them to a three-dimensional network. Nine - as to the formula unit - of the alkali metal atoms are located in vacancies of the anionic partial structure. The residual atoms with 0 x 1 centre the six-membered rings and are coordinated planar hexagonal by N neighbours.
Synthesis and crystal structure of Rb3AgO2
Sofin,Friese,Nuss,Peters,Jansen
, p. 2500 - 2504 (2002)
Rb3AgO2 was prepared via the azide/nitrate route. Stoichiometric mixtures of the precursors (Ag2O, RbN3 and RbNO3) were heated in a special regime up to 450°C and annealed at this temperature for 50 h in silver crucibles. Single crystals have been grown by subsequent annealing of the as prepared powder at 450°C for 500 h in silver crucibles, which were sealed in glass ampoules under dried Ar. According to the X-ray analysis of the crystal structure (P212121, Z = 16, a = 12.800(1), b = 12.848(1), c = 14.329(1) A, 6566 independent reflections, R(all) = 0.0795, Rw(all) = 0.0218), Rb3AgO2 is isostructural with K3AgO2. The structure can be derived from the fluorite structure type. Silver is linearly coordinated by oxygen atoms, while Rb has pseudo-tetrahedral coordination. The crystal under investigation was composed of four twin individuals.
K5Mn3O6and Rb8Mn5O10, new charge ordered quasi one-dimensional oxomanganates (II, III)
Nuss, Jürgen,Dasari, Prasad L. V. K.,Jansen, Martin
, p. 316 - 321 (2015/03/04)
K5Mn3O6 and Rb8Mn5O10 have been synthesized via the azide/nitrate route from stoichiometric mixtures of MnO and KNO3/ KN3, or RbNO3/RbN3, respectively. The two new members of manganese (II/III) mixed-valent oxides have been studied by single-crystal X-ray diffraction, magnetic susceptibility measurements and density functional theory calculations (DFT). Both crystal structures [K5Mn3O6: Pna21, Z = 4, a = 1632.43(7), b = 970.07(4), c = 616.48(3) pm, R1 = 0.051; Rb8Mn5O10: P21/c, Z = 8, a = 1223(2), b = 2717(3), c = 1220(2) pm, β = 118.25(2)° , R1 = 0.086] display quasi one-dimensional [MnO2]n-- chains, composed of edge sharing MnO4 tetrahedra. Complete charge ordering of Mn2+ and Mn3+ is observed along the chain direction with repetition units [-Mn3+-Mn2+-Mn,2+-] resulting for K5Mn3O6, and [-Mn3+-Mn2+-Mn2+-Mn3+-Mn2+-] for Rb8Mn5O10. Magnetic susceptibility data as well as DFT calculations indicate strong anti-ferromagnetic intra-chain coupling to be present already at ambient temperature, and above. Rb8Mn5O10 features threedimensional spin ordering below TN = 10.9 K, mediated by ferromagnetic coupling between the chains, while such a 3D coupling appears to be frustrated in K5Mn3O6.
Synthesis, crystal structures, and vibrational spectra of novel azidopalladates of the alkali metals Cs2[Pd(N3) 4] and Rb2[Pd(N3)4]·2/3H 2O
Afyon, Semih,Hoehn, Peter,Somer, Mehmet
, p. 1301 - 1306 (2011/01/05)
The transparent dark orange compounds Cs2[Pd(N3) 4] and Rb2[Pd(N3)4]·2/3H 2O are synthesized by reaction, of the respective binary alkali metal azides with K2PdCl4 in aqueous solutions. According to single-crystal X-ray diffraction investigations, the novel ternary azidopalladates(II) crystallize in the monoclinic space group P21/c (no. 14) with a = 705.7(2) pm, b = 717.3(2) pm, c = 1125.2(5) pm, β= 104.58(2)°, mP30 for Cs2[Pd(N3)4] and a = 1041.4(1) pm, b = 1292.9(2) pm, c = 1198.7(1) pm, β= 91.93(1)°, mP102 for Rb2[Pd(N3)4].2/3H2O, respectively. Predominant structural features of both compounds are discrete [PdII(N3)4]2- anions with palladium in a planar coordination by nitrogen, but differing in point group symmetries. The vibrational spectra of the compounds are analyzed based on the idealized, point group C4h, of the spectroscopically relevant unit, [Pd(N 3]2- taking into account the site symmetry splitting due to the symmetry reduction in the solid phase.
The chain manganates K29Mn17O34, Rb 11Mn8O16, and Cs4Mn 3O6: a new family of mixed-valent one-dimensional transition metallates
Pfeiffer, Steffen,Nuss, Juergen,Jansen, Martin
, p. 23 - 29 (2010/05/01)
Air and moisture sensitive K29Mn17O34, Rb11Mn8O16 and Cs4Mn 3O6 were prepared via the azide/nitrate route from stoichiometric mixtures of the precursors Mn2O3, AN 3 and ANO3 (A = K, Rb, Cs) in special containers provided with silver inlays. Their compositions can be generalized as A xMnO2 with x varying between 1.703 and 1.333. According to the X-ray analysis of the crystal structures [K29Mn 17O34: lma2, Z = 4, a = 93.149(3), b = 10.0063(3), c = 6.0621(2) A, 6585 independent reflections, R1 = 0.053, wR(all) = 0.143; Rb11Mn8O16: F222, Z = 16, a = 12.2096(4), b = 20.1595(7), c = 43.712(2) A, 11534 independent reflections, R1 = 0.042, wR(all) = 0.131; Cs4Mn3O6: C222, Z = 8, a = 12.790(3), b = 21.123(4), c =8.179(2) A, 2212 independent reflections, R1 = 0.051, wR(fall) = 0.122], the main feature of all three crystal structures are 1∞MnO2n- chains built up from partially distorted edge-sharing MnO4 tetrahedra. The alkali metal ions fill the space between the anionic entities forming honeycomb like arrangements. In all cases manganese is in a mixedvalent state but no full charge ordering is noticeable. The variations of the charges along the MnO 2n- chains seem to be best described in terms of charge density waves. The magnetic susceptibilities show the dominance of strong antiferromagnetic interactions for the rubidium and the cesium compounds, whereas ferro- or ferrimagnetic interactions prevail in the potassium compound.
The AFeO2 (A=K, Rb and Cs) family: A comparative study of structures and structural phase transitions
Ali, Naveed Zafar,Nuss, Juergen,Sheptyakov, Denis,Jansen, Martin
, p. 752 - 759 (2010/06/13)
Structures and phase transitions for the isostructural series of compounds KFeO2, RbFeO2 and CsFeO2 have been systematically studied by synchrotron X-ray high resolution powder diffraction experiments and in case of CsFeO2 also by single crystal diffractometry. At room temperature, all of the three compounds crystallize in the orthorhombic (Pbca) KGaO2 type of structure consisting of a three dimensional network of corner-sharing [FeO4/2]- tetrahedra, which at elevated temperatures shows a reversible phase transformation to a cubic structure (space group Fd over(3, -) m). For KFeO2, RbFeO2 and CsFeO2 this phase transformation takes place at 1003 K, 737 K and 350 K respectively, as confirmed by differential scanning calorimetry and X-ray diffraction. Upon heating through the transitions the major structural changes are driven by the onset or enhancement of librational motion of the FeO4 tetrahedra. Due to this phenomenon the Fe-O-Fe bonds appear to step-wise getting straight, seemingly approaching 180° within the time and space averaged structure.
RbGa3S5 und CsGa3S5 - Zwei neue strukturtypen
Schlosser, Marc,Frettloeh, Vanessa,Deiseroth, Hans-Joerg
, p. 94 - 98 (2009/04/20)
The title compounds RbGa3S5 and CsGa 3S5 were synthesized by a solid state reaction starting from GaS, S and MN3 (M = Rb, Cs) as alkaline metal source. They crystallize in the space group P21/su