EPR of gamma irradiation induced radicals in NaHCO3, CsHCO3 and Na2CO3

In this study gamma irradiated NaHCO₃, CsHCO₃ and Na₂CO₃ were investigated at room temperature. The radicals induced by gamma irradiation in NaHCO₃ were found to be CO⁻₃, HCO₃ and CO⁻₂; in CsHCO₃ the species were attributed to HCO₃; and in Na₂CO₃ to CO⁻₃ and CO⁻₂ radicals. The hyperfine parameters for the hydrogen in HCO₃, and the ¹³C nucleus in CO⁻₂ radical have been determined. The results were compared with literature data for similar compounds and the EPR properties of the CO⁻₂ radical were discussed.     

Struktur und Eigenschaften von Gd3I3C

Structure and Properties of Gd₃I₃C . The compound Gd₃I₃C is prepared by reaction of Gd, GdI₃ and C (2:1:1 mole) at 1 250 K in sealed Ta tubes. It is obtained as bronze-coloured needles which are air and moisture sensitive. The structure of Gd₃I₃C contains twin chains of C centered Gd₆ octahedra surrounded by I atoms capping all free edges like in the M₆X₁₂ cluster. The one-dimensional units are oriented along [010] and linked according to (GdGd_1/3Gd_2/2Gd_2/3C)₂IIII. Gd₃I₃C is metallic in the temperature range 300 K ≥ T ≥ 120 K, between 120 and 15 K the electrical resistance increases by 6 orders of magnitude. At high temperatures the susceptibility follows the Curie-Weiß law with a paramagnetic Curie temperature θ ≈ - 340 K. Two local maxima in the susceptibility at 100 K and 25 K indicate successive formation of antiferromagnetically ordered structures.     

Simple perturbation and perturbation-variation treatments of the 1sσg and 2pσu states of H

First-order wave functions and binding energies of the 1sσ_g and 2pσ_u states of H are calculated by simple methods for internuclear separations between 0.2 and 10_a0. An exact perturbation treatment of the lsσ_g state with a zeroth-order function of the form N exp (-sRλ/2) exp (sR μ2) yields only fair results. An alternative method starts with zeroth-order functions of the form N exp (-sRλ/2)[exp (-sRμ/2) ± exp (sRμ/2)] for the 1 and 2 states, respectively. An approximate first-order trial function is set up and the energies are determined variationally. For both states the results are comparable to those obtained by exact perturbation treatments of the same order.     

Synthesis and Crystal Structure of Tricaesium Heptaphosphide–Ammonia(1/3) Cs3P7·3 NH3

Recrystallization of Cs₃P₇ from liquid NH₃ yields the triammoniate Cs₃P₇·3 NH₃, which loses the weakly bound NH₃ of crystallization below 253 K. A low-temperature crystal-structure analysis shows that Cs₃P₇· NH₃ consists of a framework of heptaphosphanortricyclane anions P and Cs⁺ cations with NH₃ molecules completing the coordination of the cations. The framework is built from Cs₃P₇ layers connected by only few Cs…?P interactions, the interlayer gap being filled by a two-dimensional network of NH₃. The Cs₇P₇ part of the structure completes a family of alkali-metal-polyphosphide substructures which range from [RbP₇]^2? or [CsP₁₁]^2? chains over [Cs₂P_n]^? layers (n = 7, 11) to now [Cs₃P₇] frameworks.     

Upconversion properties of Er3+, Yb3+ and Tm3+ codoped fluorophosphate glasses

Er3+, Yb3+ and Tm3+ codoped fluorophosphate glasses emitting blue, green and red upconversion luminescence at 970 nm laser diode excitation were studied. It was shown that Tm3+ behaves as the sensitizer to Er3+ for the green upconversion luminescence through the energy transfer process: Tm3+:3H4+Er3+:4I 15/2-->Er3+:4I 9/2+Tm3+:3H6, and for the red upconversion luminescence through the energy transfer process: Tm3+:3F4+Er3+:4I 11/2-->Tm3+:3H6+Er3+:4F 9/2. Moreover, Er3+ acts as quenching center for the blue upconversion luminescence of Tm3+. The sensitization of Tm3+ to Er3+ depends on the concentration of Yb3+. The intensity of blue, green and red emissions can be changed by adjusting the concentrations of the three kinds of rare earth ions. This research may provide useful information for the development of high color and spatial resolution devices and white light simulation.     

Verbindungen in den Systemen Kalium(Rubidium)/Gold/Antimon: K3Au3Sb2, Rb3Au3Sb2 und K1,74Rb0,26RbAu3Sb2

Compounds in the Systems Potassium(Rubidium)/Gold/Antimony: K₃Au₃Sb₂, Rb₃Au₃Sb₂, and K_1,74Rb_0,26RbAu₃Sb₂ Brittle, silver coloured single crystals of K₃Au₃Sb₂, Rb₃Au₃Sb₂ and K_1,74Rb_0,26RbAu₃Sb₂ were obtainded by reaction of the alkali metal azides (KN₃, RbN₃) with gold and antimon powder at 550°C. The structures of the isotypic compounds (R3 m, Z = 3) were determined by X-ray single-crystal diffractometer data: K₃Au₃Sb₂, a = 6,198(2) Å, c = 21,520(5) Å, R/R_w (w = 1) = 0,046/0,058, Z(F) ? 3σ(F) = 175, Z(Var.) = 14; Rb₃Au₃Sb₂, a = 6,443(3), c = 21,69(2), R/R_w (w = 1) = 0,059/0,082, Z(F) ? 3σ(F₀²) = 258, Z(Var.) = 14; K_1,74Rb_0,26RbAu₃Sb₂, a = 6,288(2) Å, c = 21,617(5) Å, R/R_w (w = 1) = 0,049/0,069, Z(F) ? 3σ(F) = 390, Z(Var) = 14. The compounds crystallize with the K₃Cu₃P₂-structure type. The Au? Sb partial structures consist of [AuSb_2/3] layers with linear Sb? Au? Sb dumb-bells and SbAu₃ pyramids. The layers are separated by two crystallographically independent alkali metal atoms along [001].     

The octant rule: XXIII. antioctant effects in γ,δ -unsaturated ketones.

The and -benzyl derivatives (1 and 2, respectively) of (+)-camphor have been synthesized and are found to exert a strong influence on the circular dichroism n→π^* Cotton effects: 1: Δε³⁰¹_max -0.36 (n- heptane) and 2: Δε³⁰²_max +3.22, relative to camphor: Δε³⁰⁴_max +1.8 (n-heptane). Evidence for electric dipole transition moment coupling in these γ, δ -unsaturated systems is found in the n→π^* UV: 1: ε²⁹¹_max 84 (n-heptane) and 2: ε²⁸⁵_max 303, relative to camphor: ε²⁹⁰_max 25.     

Rate constants for the reactions of OH radicals with CH3OCF2CF3, CH3OCF2CF2CF3, and CH3OCF(CF3)2

The rate constants for the reactions of OH radicals with CH₃OCF₂CF₃, CH₃OCF₂CF₂CF₃, and CH₃OCF(CF₃)₂ have been measured over the temperature range 250–430 K. Kinetic measurements have been carried out using the flash photolysis, laser photolysis, and discharge flow methods combined respectively with the laser induced fluorescence technique. The influence of impurities in the samples was investigated by using gas‐chromatography. The following Arrhenius expressions were determined: k(CH₃OCF₂CF₃) = (1.90) × 10⁻¹² exp[−(1510 ± 120)/T], k(CH₃OCF₂CF₂CF₃) = (2.06) × 10⁻¹² exp[−(1540 ± 80)/T], and k(CH₃OCF(CF₃)₂) = (1.94) × 10⁻¹² exp[−(1450 ± 70)/T] cm³ molecule⁻¹ s⁻¹. © 1999 John Wiley & Sons, Inc. Int J Chem Kinet 31: 846–853, 1999     

Atomic integrals containing rrr with λ, μ, ν ≥ −2

In this paper, the efficient evaluation of the atomic integrals I =∫rrrrrre^{?αr1?βr2?γr3}dτ with one or two factors r is described. These integrals are necessary for a lower-bound calculation for Li-like systems using the method of variance minimization or Temple's formula. © 1993 John Wiley & Sons, Inc.     

The reactions of CF3 and CD3 radicals with boron trimethyl

Hydrogen abstraction from boron trimethyl has been studied using the abstracting radicals CF₃ and CD₃, from the photolysis of the corresponding ketones over the temperature range of 150° to 300°C. The following Arrhenius parameters were obtained: The difference E – E in the case of BMe₃ is considered due, in part, to polar effects. An exchange reaction is proposed for both CF₃ and CD₃ in collisions with BMe₃: Radical combination of CF₃ and CH₂BMe₂ leads to a hot molecule which undergoes a β-fluoro rearrangement elimination process, or a stabilized molecule which can thermally decompose:      

Spectroscopic constants and molecular properties of A3Σu+, B3Πg,W3Δu,and B′3Σu− electronic states of the N2 molecule

The potential energy curves (PECs) of A³Σ, B³Π_g, W³Δ_u, and B^′3Σ electronic states of the N₂ molecule have been studied for internuclear separations from 0.05 to 2.0 nm using the full valence complete active space self‐consistent‐field method followed by the highly accurate valence internally contracted multireference configuration interaction (MRCI) approach in conjunction with the correlation‐consistent basis sets. Effects on the PECs by the core–valence correlation and relativistic corrections are taken into account. The way to consider the relativistic correction is to use the second‐order Douglas‐Kroll Hamiltonian approximation. The core–valence correlation correction is made with the cc‐pCV5Z basis set. And the relativistic correction is performed at the level of cc‐pV5Z basis set. To obtain more reliable results, the PECs determined by the MRCI calculations are also corrected for size‐extensivity errors by the Davidson modification (MRCI+Q). These PECs are extrapolated to the complete basis set limit. The spectroscopic parameters of ¹⁴N₂, ¹⁴N¹⁵N, and ¹⁵N₂ isotopologs have been evaluated and compared with those reported in the literature. Excellent agreement has been found between the present results and the Rydberg‐Klein‐Rees (RKR) data. With the PECs obtained by the MRCI+Q/CV+DK+56 calculations, the first 30 vibrational states for three species are computed for each electronic state. And for each electronic state of each species, the vibrational level G(ν), inertial rotation constant B_ν, and centrifugal distortion constant D_ν have been determined, which agree well with the RKR data. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2012     

Neutral and Cationic Hexanuclear Rhenium Phosphine Clusters with μ3‐(Phosphido‐Chalcogenido), μ3‐(Arsenido‐Chalcogenido), and μ3‐(Imido or Oxo‐Chalcogenido) Hetero Ligand Shells

Reactions of dry THF/MeCN solutions of Ca[Re₆SCl(Cl^a)₆] with silylated derivatives E(SiMe₃)₂ (E = PhAs, PSiMe₃, HN, O, S) and addition of trialkylphosphine PPr₃ afford in high yields and at room temperature either the neutral clusters [Re₆SX(PPr₃)] ( 1 : X = As, 2 : X = P) or the ionic compounds [Re₆SX(PPr₃)]²⁺ · [Re₆S₆Cl₈]^2– ( 3 : X = NH, 4 : X = O, 5 : X = S). The compounds 1 – 5 were characterised by X‐ray crystal structure analysis. A di‐substitution reaction occurs on the {Re₆SCl}⁴⁺ cluster core, where the two inner μ₃‐chloro ligands Clⁱ are substituted by X (X = As, P, NH, O, S) and all six terminal chloro ligands Cl^a are exchanged by terminal PPr₃‐ligands.     

Optical characterization of Sm3+ and Dy3+:ZnO-PbO-B2O3 glasses

Here, we present the results of the analysis of Sm(3+) or Dy(3+) (0.5 mol%) ions doped heavy metal oxide (HMO)-based zinc lead borate (ZLB) glasses. Optical measurements such as absorption, emission spectra, lifetimes, XRD, DSC profiles have been carried out. The emission spectrum of Sm(3+):ZLB has shown the emission transitions of (4)G(5/2)-->(6)H(5/2) (563 nm), (4)G(5/2)-->(6)H(7/2) (598 nm), (4)G(5/2)-->(6)H(9/2) (646 nm), (4)G(5/2)-->(6)H(11/2) (708 nm) with lambda(exc): 401 nm ((6)H(5/2)-->(4)F(7/2)). In the case of the Dy(3+):ZLB glass, emission transitions of (4)F(9/2)-->(6)H(15/2) (485 nm), (4)F(9/2)-->(6)H(13/2) (575 nm) and (4)F(9/2)-->(6)H(11/2) (664 nm) with lambda(exi): 447 nm ((6)H(15/2)-->(4)I(15/2)) have been identified. Energy level schemes relating to the emission mechanisms involved in Sm(3+) and Dy(3+) glasses have been given.     

The Protonation of [Pt3(m̈-CO)3(PCy3)3]

The cluster [Pt₃(m?-CO)₃(PCy₃)₃] can be protonated with HBF₄ · OEt₂ to form the cluster [Pt₃(m?-CO)₃(PCy₃)₃](m?₃-H) ⁺BF ( 2 ). This unstable compound was isolated and characterised by NMR and IR spectroscopy.     

γ-radiation-initiated polymerization of bulk styrene at high pressure

The polymerization of styrene in bulk at pressures up to 273 MPa and temperatures between 3 and 49°C with the use of γ-radiation as the initiator has been studied. The polymerization rate and the molecular weight of the polymer increased with increasing pressure; the molecular weight increased at a slightly faster rate. The difference in the rate is a theoretical expectation which has not previously been observed because chain-transfer reactions obscure the effect in chemically initiated systems. A small but significant retardation of the initiation reaction occurs as the pressure is increased. The results of previous workers are critically reviewed. Chain transfer at 25°C for pressures below 220 MPa is negligible when γ-radiation is the initiator. The activation energy for bulk polymerization decreased with increasing pressure from 28.1 kJ/mole at 0.1013 MPa to 22.3 kJ/mole at 203 MPa. Volumes of activation at 25°C for 0.1013 < p < 273 MPa were calculated to be Initiation, +4.0 < ΔV < +4.4 cm³/mole; polymerization; ?Δ = ?20.9 cm³/mole; degree of polymerization; ΔV = ?25.3 cm³/mole; propagation/termination; ?ΔV = ?22.7 cm³/mole.     

Schwingungsspektrum und Kraftkonstanten des Tetrakis-trimethylsilyl-hydrazin,[(CH3)3Si]2N-N[Si(CH3)3]2

The vibrational spectra (IR and RAMAN ) have been taken for tetrakis-trimethylsilyl-hydrazine. A complete assignment of all observed bands is given. The silicium-nitrogen vibrations are interpreted in terms of a D_2d configuration. Force constants of the GVFF are computed. The valency force constant of the nitrogen-nitrogen bond is comparable to that of N₂H. This proves the interaction of the silicium atoms with the free electron pairs of the two nitrogen atoms.     

The nature of the chemical bond in borazine (B3N3H6), boroxine (B3O3H3), carborazine (B2N2C2H6), and related species

The bonding problem in borazine (B₃N₃H₆), boroxine (B₃O₃H₃), and carborazine (B₂N₂C₂H₆) is successfully addressed through the consideration of the excited states of the constituent fragments, namely BH( ), NH( ), and CH( ). We propose the participation of resonant structures for all three species that help to explain the experimental findings. A discussion on the chemical pattern of the parental molecule benzene (C₆H₆) helps to make coherent the whole bonding analysis on the titled species.     

Zwei neue Ammoniakate des Scandiumtrichlorides,ScCl3(NH3) und ScCl3(NH3)2

Two New Ammoniates of Scandium Trichloride, ScCl₃(NH₃) and ScCl₃(NH₃)₂ Reactions of scandium with ammonium chloride in the presence of cupric chloride in sealed copper ampoules yield colorless single crystals of the two new ammoniates of scandium trichloride, ScCl₃(NH₃) und ScCl₃(NH₃)₂. The crystal structures were determined from single crystal data; they both crystallize with the triclinic crystal system. In ScCl₃(NH₃)₂ isolated unsymmetrical dimers of double octahedra, according to [Sc‐mer‐(NH₃)_3/1Cl_1/1Cl_(2/2)×2Sc(NH₃)_1/1Cl_3/1] are the characteristic structural features. The crystal structure of ScCl₃(NH₃) also contains double octahedra, [Sc(NH₃)_2/1Cl_2/1Cl_2/2]₂; these dimers are, however, connected via common edges forming infinite zig‐zag chains according to the formulation [Sc(NH₃)_1/1Cl_1/1Cl_4/2].     

·OH自由基引发CH3SSCH3•+自由基裂解反应机理的理论研究

采用UωB97X-D/6-311+G^**方法, 研究了气相、 甲苯和水中OH自由基(·OH)引发CH₃SSCH₃自由基阳离子(CH₃SSC{\mathrm{H}}_{\mathrm{3}}^{?}⁺, DMDS^?+)裂解的反应机理, 并讨论了溶剂效应对反应的影响. 结果表明, ·OH和DMDS^·+首先形成自由基耦合产物CH₃S(OH)SCH₃⁺(R1)和氢提取产物复合物[CH₂=SSCH₃+H₂O]⁺(R2); 随后R1裂解直接发生 S—S键断裂协同质子转移, 而R2裂解依次发生构象变化、 C=S键亲碳加成和S—S键断裂协同质子转移. 去质子化的裂解产物为CH₃SOH, CH₂=S和HSCH₂OH. 甲苯略微降低了裂解反应速控步骤的自由能垒. 水溶剂有利于R1裂解, 但不利于R2裂解, 尤其是单个水分子参与反应. 在气相、 甲苯和水中, 以·OH和DMDS^·+为初始反应物, 虽然速控步骤的自由能垒为167.6~202.8 kJ/mol, 但裂解反应均是放热反应(?154.3~?31.4 kJ/mol).