Synthesis of novel termetallic isopropoxides

Novel termetallic isopropoxides are reported which may be represented by the general formulae: [(PrⁱO)₃M(μ-OPrⁱ)₂Be(μ-OPrⁱ)₂Al(OPrⁱ)₂], [(PrⁱO)₂M(μ-OPrⁱ)₂Be(μ-OPrⁱ)₂Al(OPrⁱ)₂]₂ [where M = Ti(IV), Zr(IV) and Hf(IV)] and [(PrⁱO)₄M(μ-OPrⁱ)₂Be(μ-OPrⁱ)₂Al(OPrⁱ)₂] [where M = Nb(V) and Ta(V)]. Attempts to synthesize derivatives with the general formula, [(PrⁱO)₇M₂(μ-OPrⁱ)₂Be(μ-OPrⁱ)₂Al(OPrⁱ)₂] [where M = Ti(IV), Zr(IV) or Hf(IV)], were unsuccessful and in all such cases a mixture of M(OPrⁱ)₄ and [(PrⁱO)₃M(μ-OPrⁱ)₂Be(μ-OPrⁱ)₂Al(OPrⁱ)₂] was obtained. All these derivatives are soluble in common organic solvents and with the exception of titanium(IV) derivatives, they can be volatilised without noticeable disproportionation. These products have been characterized by elemental analyses, molecular weights, IR, ¹H NMR and (in representative cases) mass spectral studies also.     

Excess molar quantities of (a halogenated n-alkane + an n-alkane) A comparative study of mixtures containing either 1-chlorobutane or 1,4-dichlorobutane

Excess molar volumes V_m^E at 298.15 K were obtained, as a function of mole fraction x, for series I: {x1-C₄H₉Cl + (1 ? x)n-C_lH_{2l + 2}}, and II: {x1,4-C₄H₈Cl₂ + (1 ? x)n-C_lH_{2l + 2}}, for l = 7, 10, and 14. 10, and 14. The instrument used was a vibrating-tube densimeter. For the same mixtures at the same temperature, a Picker flow calorimeter was used to measure excess molar heat capacities C_{p, m}^E at constant pressure. V_m^E is positive for all mixtures in series I: at x = 0.5, V_m^E/(cm³ · mol^?1) is 0.277 for l = 7, 0.388 for l = 10, and 0.411 for l = 14. For series II, V_m^E of {x1,4-C₄H₈Cl₂ + (1 ? x)n-C₇H₁₆} is small and S-shaped, the maximum being situated at x_max = 0.178 with V_m^E(x_max)/(cm³ · mvl^?1) = 0.095, and the minimum is at x_min = 0.772 with V_m^E(x_min)/(cm³ · mol^?1) = ?0.087. The excess volumes of the other mixtures are all positive and fairly large: at x = 0.5, V_m^E/(cm³ · mol^?1) is 0.458 for l = 10, and 0.771 for l = 14. The C_{p, m}^Es of series I are all negative and |C_{p, m}^E| increases with increasing l: at x = 0.5, C_{p, m}^E/(J · K^?1 · mol^?1) is ?0.56 for l = 7, ?1.39 for l = 10, and ?3.12 for l = 14. Two minima are observed for C_{p, m}^E of {x1,4-C₄H₈Cl₂ + (1 ? x)n-C₇H₁₆}. The more prominent minimum is situated at x′_min = 0.184 with C_{p, m}^E(x′_min)/(J · K^?1 · mol^?1) = ?0.62, and the less prominent at x″_min = 0.703 with C_{p, m}^E(x″_min)/(J · K^?1 · mol^?1) = ?0.29. Each of the remaining two mixtures (l = 10 and 14) has a pronounced minimum at low mole fraction (x_min = 0.222 and 0.312, respectively) and a broad shoulder around x = 0.7.     

The photophysics of trans-stilbene

The fluorescence lifetime of trans-stilbene in dilute methylcyclohexane/iso-hexane solution has been measured and the mean S₁ radiative (k_F), radiationless (k_I) and cis-isomerization (k_C) rate parameters have been determined from ?90 to 60°C. S_i consists of a fluorescent trans (¹B_u^*) state (k_F⁰ = 6.0 × 10⁸ s^?1) which undergoes reversible thermal-activated rotational internal conversion (ΔH = 1.75 kcal mole^?1, ΔS = 10.6 cal deg^?1 mole^?1) to a non-fluorescent perp (¹A_g^*) state. p(¹A_g^*) lies 610 cm^?1 above t (¹B_u^*) with an intermediate S₁ potential maximum. p(¹A_g^*) undergoes internal conversion(k_I.^∞ = 5.8 × 10⁸ s^?1) to p (¹A_g) leading to cis-isomerization. This is the main isomerization channel over the whole temperature range.     

Synthesis and coordination chemistry of tetrabutyldithioimidodiphosphinates

Butyl substituted imidodithiophosphinates R₂P(S)NP (S)R′₂ (R=ⁿBuⁱBu^sBuR′=ⁿBuⁱBu^sBu) have been synthesised via an HBr elimination reaction between R₂P(S)NH₂ and R′₂P(S)Br The compounds were characterised spectroscopically Crystallographic and spectroscopic studies reveal ⁿBu₂P(S)NHP(S)ⁿBu₂ and ^sBu₂P(S)NHP(S)ⁱBu₂ to be hydrogen bonded transoid dimers and ⁱBu₂P(S)NHP(S)ⁱBu₂ to be a transoid hydrogen bonded chain Reactions of the imidodithiophosphinates with ZnCl₂ or MCl₂COD gave the coordination complexes M[R₂P(S)NP (S)R′₂]₂ (R=ⁿBuⁱBu^sBuR′=ⁿBuⁱBu^sBuM=ZnPd: R=ⁿBuⁱBu^sBuPt).     

Kinetics of hydroquinone chemisorption at polycrystalline platinum electrodes: The effect of surface roughness

The rate of hydroquinone (HQ) chemisorption from aqueous H₂SO₄ onto annealed (smooth) and platinized (rough) polycrystalline Pt has been studied. Previously, equilibrium adsorption measurements indicated that at smooth Pt surfaces, adsorption of HQ at c_HQ ⩽ 0.1 mM yielded flat (η⁶)-oriented species while adsorption at c_HQ ⩾ 1 mM resulted in edge (2,3-η²)-attached intermediates. Edge-attached species were not formed efficiently at roughened Pt surfaces. The present data show that the rate of η⁶-HQ chemisorption was significantly lower at roughened than at smooth surfaces. Analysis of the rate data gave the following enthalpies and entropies of activation at smooth (sm) and platinized (pt) surfaces: ΔH^≠_sm,0.1mM = 12.5 kJ/mol; ΔH^≠_sm,2mM = 8.3 kJ/mol; ΔS^≠_sm,0.1mM = −83 J/mol K; ΔS^≠_sm,2mM = −117 J/mol K; ΔH^≠_pt,0.4mM = 12.5 kJ/mol; ΔH^≠_pt,2mM = 12.5 kJ/mol; ΔS^≠_pt,0.4mM = −92 J/mol K; ΔS^≠_pt,2mM = −100 J/mol K. The similarity between ΔH^≠_{pt,0.4 mM}, ΔH^≠_{pt,2 mM} and ΔH^≠_{sm,0.1 mM}, and between ΔS^≠_{pt,0.4 mM}, ΔS^≠_{pt,2 mM} and ΔS^≠_{sm,0.1 mM} correlate with the earlier finding that adsorption of HQ onto roughened Pt surfaces occurred primarily in the flat orientation at all concentrations studied.     

The polarizability of a pair of hydrogen atoms at long range

The coefficients of R^?6 and R^?9 in the long-range expansion of the parallel and perpendicular components of the polarizability of a pair of hydrogen atoms at a separation R have been calculated. The results are A⁽⁶⁾₆ = 2558.59. A⁽⁶⁾_⊥ = 1268.25, A⁽⁸⁾₆ = 90639.5 and A⁽⁸⁾_⊥ = 22010.3 au. The values of A⁽⁶⁾₆ and A⁽⁶⁾₆ and A⁽⁶⁾_| are somewhat larger than previous theoretical estimates and much larger than the classical values of 729 and 182.25 au. The terms in R^?8 arise from distortion associated with the dispersion forces and from the field of the quadrupole moment induced by the field-gradient at each atom.     

Geometric and electronic structure of ground and excited states of groupVA diatomics. A theoretical LCGTO-MP-LSD study

LCGTO-MP-LSD calculation was performed for the ground and several low-lying excited states of homo- (N₂, P₂, As₂, and Sb₂) and hetero-nuclear (PN, AsN, AsP, AsSb, SbN, and SbP) groupVA diatomics. For all the systems the ground state is found to be¹Σ⁺. For N₂ and P₂, the¹Σ _g ⁺ ground state is followed by the³Σ _u ⁺ ,³Π _g ,³Δ _u ,¹Π _g , and¹Δ _u low-lying exited states while for As₂ the order is found to be³Σ _u ⁺ ,³Δ _u ,³Π _g ,¹Δ _u ,¹Π _g . Finally for Sb₂ the relative stability of excited states is³Σ _u ⁺ ,³Δ _u ,¹Δ _u ,³Π _g ,¹Π _g . For the hetero-nuclear diatomics the¹Σ⁺ ground state is, in the case of PN, AsN, AsP, SbN, and SbP, followed by the³Σ⁺,³Δ,³Π,¹Π and¹Δ low-lying excited states while for the AsSb diatomic an inversion of stability of the two last singlets occurs. The calculated spectroscopic parameters (Re, ωe, andDe) are in good agreement with all the available experimental results while, theTe values are overestimated by about 0.5 eV. Mulliken population analysis shows that both homo- and hetero-nuclear groupVA diatomics are essentially triple bonded systems.     

Pulsed amperometric detection of sulfur compounds: Part II. Dependence of response on adsorption time

A mathematical model is developed for the response of PAD and is applied to data from the study of I_p as a function of t_ads for evaluation of the adsorption rate constants, and the maximum molar surface coverage for thiourea at a Pt electrode. The results are, respectively: k₁ = 4.1 × 10⁴ M⁻¹ s⁻¹, k₋₁ = 1.9 s⁻¹, and Γ₀ = 1.3 × 10⁻¹⁰ mol cm⁻². The calculated adsorption equilibrium constant (k₁/k₋₁) is 2.1 × 10⁴ M⁻¹, compared to 4.9 × 10⁴ M⁻¹ calculated from the plot of 1/I_p vs. 1/c^b for c^b > 1.0 × 10⁻⁴ M and t_ads = 8500 ms. Analytical calibration procedures are examined; linear plots of 1/I_p vs 1/c^b cannot be expected for cases of mixed transport-isotherm control of detector response.     

Fluorescence line narrowing spectroscopy of Eu in zinc-thallium-tellurite glass

The environment of Eu³⁺ in zinc-thallium-tellurite glass of the molar composition 60TeO₂-30TlO_0.5-9.9ZnO-0.1Eu₂O₃ was investigated by laser-induced fluorescence line narrowing (FLN) techniques using Eu³⁺ as a local site probe. From the site selective luminescence spectra of Eu³⁺ at 7 K, the energies of the Stark components of the ⁷F₁ and ⁷F₂ states were recorded and then the crystal field parameters B_nm were calculated assuming a C_2v site symmetry. The ratios B₂₂/B₂₀ and B₄₄/B₄₀ for each excitation energy within ⁷F₀-⁵D₀ transition were obtained and compared with the values calculated for Eu³⁺ in other types of glasses.     

Synthesis,characterization, and magnetic properties of mixed-valence europium-ammonia intercalation compounds of titanium disulfide

Europium-ammonia intercalation compounds of titanium disulfide have been synthesized by reaction of EuNH₃ solutions with TiS₂, characterized by thermogravimetric analysis and powder X-ray diffraction, and investigated by electron paramagnetic resonance, magnetization, and magnetic susceptibility measurements. These materials crystallize in a 3R-type structure in which every layer is occupied by intercalated species. The intercalation of NH₃ is accompanied by the formation of NH⁺₄ until a critical electron concentration of 0.22 mole el/mole TiS₂ have been transferred to the TiS₂ conduction band. Although Eu³⁺ is the predominant Eu species for x > 0.001, Eu²⁺ is also formed, possibly from the reduction of Eu³⁺ in the van der Waals gap. These mixed-valence compounds are best described by the formulas (Eu³⁺)_x′(Eu²⁺)_x″(NH⁺₄)_y′(NH₃)_y″TiS^{(3x′+2y″+y′)−}₂ for 3x′ + 2x″ + y′ < 0.22 and (Eu³⁺)_x′(Eu²⁺)_x″(NH₃)_y″TiS^{(3x′+2x″)−}_n2 for 3x′ + 2x″ ≥ 0.22.     

Jahn—Teller effects in the mindo approximation: structures of the molecular cations of methane and the chloromethanes

The MINDO/3 technique gives geometries for (CH₄)⁺, (CCl₄)⁺ and the intermediate ions (CH_nCl_{4 ? n})⁺ (n = 1, 2, 3) which have symmetries in precise accord with the predictions of the Jahn—Teller effect. The ground state of (CH₄)⁺ has D_2d symmetry, with a C_3v structure ca. 45.6 kJ mol^?1 higher. (CCl₄)⁺ has a C_2v ground state, with a D_2d structure ca. 144 kJ mol^?1 higher: no bound state of C_3v symmetry could be found. (CH₃Cl)⁺ and (CHCl₃)⁺ both have C_s symmetry, and (CH₂Cl₂)⁺ has C_2v symmetry. The analogous fluoro ions are discussed briefly.     

A 31P and 119Sn NMR study of trichlorostannate derivatives of some chloride-bridged palladium(II) dimers

The chloride-bridged dimers [Pd(μ-Cl)(SnCl₃)L]₂ (L = P(p-tolyl)₃, P(p-C₆H₄OMe)₃, As(p-tolyl)₃, AsEt₃, PEt₃, PPrⁿ₃) have been synthesized and their ¹¹⁹Sn and, where relevant, ³¹P NMR spectra recorded. For the aryl phosphine and both arsine complexes the dimers exist as both the sym-trans and sym-cis isomers; however, for the PEt₃ and PPrⁿ₃ compounds, there is only one form, which we assign to the sym-trans structure. There is a geometric dependence of both ⁴J(¹¹⁹Sn, ¹¹⁷Sn) and ⁴J(¹¹⁹Sn, ³¹P). The dimeric complex with P(p-tolyl)₃ carbonylates 1-heptyne in the presence of excess SnCl₂, but is inactive in its absence.     

Fine structure of As−

The energies of the As^? fine structure components 4p^{4 3} P ₁ and 4p^{4 3} P ₀ have been determined relative to the 4p^{4 3}P₂ ground state by using photodetachment electron spectroscopy. Fine structure splittings of ΔE(³ P ₁ ? ³ P ₂) = 125(3) meV and ΔE(³ P ₀ ? ³ P ₂) = 166(5) meV have been obtained. It is the first experimental determination of the energy of the J = 1 level and an improvement of the accuracy for the J = 0 level. Previous isoelectronic extrapolations are consistent with the experimental values.     

The microwave spectrum of the unsymmetrical conformation of 1-chloro-2-methyl propane

The microwave spectrum of 1-chloro-2-methyl propane has been recorded and lines assigned to ³⁵Cl and ³⁷Cl species in the unsymmetrical conformation. The rotational and distortion constants in MHz are: C₄H₉³⁵Cl, A = 7527.05, B = 2146.21, C = 1793.59, Δ_JK = 4.15 × 10^?3, δ_j = ?8.0 × 10^?5; C₄H₉³⁷Cl, A = 7524.40. B = 2091.73, C = 1755.54, Δ_JK = 2.5 × 10^?3, δ_j = 2.0 × 10^?4.     

Modified low temperature solid state synthesis and photoluminescent properties of Y0.48Li1.5V1 ? x P x O4:Eu3+ (x = 0.2, 0.4, 0.6) nanophosphors

A modified low temperature solid state process has been proposed to systematically synthesize europium-doped yttrium phosphate-vanadates with general formula Y_0.48Li_1.5V_{1 ? x} P _x O₄:Eu³⁺ (x = 0.2, 0.4, 0.6). All the Y_0.48Li_1.5V_{1 ? x} P _x O₄:Eu³⁺ products were characterized by X-ray diffraction (XRD) and scanning electron microscope (SEM). The excitation and emission spectra were measured at room temperature. Y_0.48Li_1.5V_{1 ? x} P _x O₄:Eu³⁺ show the characteristic missions of Eu³⁺ (⁵ D ₀?⁷ F _{1, 2, 3, 4} transitions dominated by ⁵ D ₀?⁷ F ₂), intensities of the products were sensitive to the x value, and the x value had an obvious influence on the (⁵ D ₀?⁷ F ₂)/(⁵ D)₀?⁷ F ₁) intensity ratio of Eu³⁺. In addition, incorporation of Li⁺ ions in the phosphors reduce the amount of Y₂O₃, lower the cost of production, and cause a new phase Li₃VO₄.     

Volumetric properties of aqueous solutions of amino acids from the singular to critical temperature

The partial volume -V ₂ ⁰ of amino acids in aqueous solution is assumed to be zero for T = 227 K (singular temperature) and T= T _c (critical temperature). The literature data for -V ₂ ⁰(T) of ten amino acids at 278–328 K are reproduced by the two-parameter equation with a standard deviation of 0.06–0.16 cm³/mol. Only for asparagine and tryptophan the standard deviation exceeds 0.3 cm³/mol. In the case of glycine and alanine, the relation -V ₂ ⁰(T) in the high temperature range is obtained. -V ₂ ⁰ is divided into contributions (?-H ₂ ⁰/?p) _T and —T·(?-S ₂ ⁰/?p) _T . Their dependence on the temperature and amino acid nature is discussed. Positive values of ?-C ₂ ⁰/?p) _T characterize amino acids as water structure breakers; however, the differentiation of compounds by this feature is not successful. The behavior of amino acids in aqueous solutions is compared with the behavior of urea.     

Determination of the population,depopulation and the anisotropic spin lattice relaxation rates in the photoexcited triplet state of phenazine. A light modulation-EPR study

The photoexcited triplet state of phenazine in toluene glasses at 35 K is investigated by light modulation-EPR spectroscopy. From the transient EPR spectra and the kinetics in the three canonical orientations (p = x, y, z) the rate parameters are determined. Thus, the depopulation rate constants k_p, the anisotropic spin lattice relaxation rate constants W_p, and the ratios between the population constants A_p are calculated: k_x = (2.2 ± 0.3) × 10² s^?1, k_y = (0.21 ± 0.04) × 10² s^?1, k_z = (0.06 ± 0.03) × 10² s^?1, W_x = (8.6 ± 0.9) × 10³ s^?1, W_y = (11.0 ± 1.0) × 10³ s^?1, W_z = (14.0 ± 1.4) × 10³ s^?1, and A_x: _Ay:A_z ≈ 1:0.04:0.02. It is concluded therefore that the in-plane spin state |τ_x > is the active one.     

Layer-by-layer assembly of multilayer films of polyoxometalates and tris(phenanthrolinedione) complexes of transition metals

A series of organic-inorganic composite films were prepared by the layer-by-layer self-assembly method containing the phendione complexes of transition metals [M(phendione)₃]²⁺ (M=Fe²⁺, Co²⁺, phendione=1,10-phenanthroline-5,6-dione) and the polyoxometalates (POMs). UV-vis spectroscopy was used to follow the fabrication process of (BW₁₂/[M(phendione)₃]²⁺)_n (BW₁₂=BW₁₂O₄₀⁵⁻, M=Fe²⁺, Co²⁺) and (Co₄(PW₉)₂/[M(phendione)₃]²⁺)_n (Co₄(PW₉)₂=Co₄(H₂O)₂(PW₉O₃₄)₂¹⁰⁻, M=Fe²⁺, Co²⁺) multilayer films. Electrochemical studies on the films illustrate that the POM species exhibit well-defined redox peaks and the phendione species show pH-dependent electrochemical behavior. The photoluminescent properties were investigated to show the (BW₁₂/[Fe(phendione)₃]²⁺)_n film with low-energey red photoluminescence at 672 nm.     

Reevaluation of electronic polarization energies in organic molecular crystals

Effective electronic polarization energies for positive P⁺_eff and negative P⁻_eff charge carriers in polyacene crystals have been reevaluated. By comparing the P⁺_eff and P⁻_eff values obtained from the analyses of reported energy parameters with calculated data, it is shown that the widely accepted assumption that P⁺_eff = P⁻_eff in polyacene crystals is not valid. By applying recently reported data on optical E^opt_G and adiabatic E^ad_G energy gap values, the contribution of molecular (vibronic) polarization in the total effective polarization energies W⁺_eff and W⁻_eff has been estimated, and modified energy diagrams for polyacene crystals have been presented. Further, due to practically constant values of observed and calculated P⁺_eff and P⁻_eff in polyacenes, the gap energies between positive and negative charge carrier conduction levels have been estimated for several related aromatic hydrocarbons.     

Hyperfine structure measurements of103Rh

Hyperfine structure has been measured in 28 states of¹⁰³Rh below 34,000 cm^?1. The magnetic dipole interactionA constants in the metastable states 4d ⁸ 5s ⁴ P _5/2,3/2,² P _3/2,1/2,² D _5/2,3/2,² G _9/2,7/2 and 4d ⁷ 5s ^{2 4} F _{9/2,7/2,5/2,3/2} have been determined using the laser radio-frequency double-resonance method and in the states 4d ⁸ 5p ⁴ D _{7/2,5/2,3/2,1/2},⁴ G _7/2,5/2,⁴ F _{9/2,7/2,5/2,3/2},² G _9/2,7/2,² F _7/2,5/2 and² D _5/2,3/2 by high-resolution laser spectroscopy.