Laser-induced photodissociation of He+2

The momentum distributions of He⁺ fragments from photodissociation of He⁺₂ ions have been recorded in a crossed-beams experiment. The discrete values of the kinetic energy releases can be predicted from the vibrational spacings in the ground state of the primary ions.     

The anisotropic van der waals potential for He-N2

We have calculated the spherical v₀ and anisotropic radial components v₂ and v₄ in the usual Legendre expansion for the rigid rotor He-N₂ potential using the method of Tang and Toennies Potential curves covering the range of internuclear distances from 2.5 to 8.0 Å, which includes the minimum region, arc presented and compared with a recent experimental potential derived from differential total cross sections.     

Fluorescence lifetimes in BO2 (A2Πu)

Fluorescence lifetimes and fluorescence quenching rates are reported for several vibronic levels in the A²Π_u electronic manifold of BO₂. The relationship of these results to earlier Hanle-effect measurements is discussed.     

Mise en évidence par spectroscopie infrarouge des espèces Ni(PH3)n(n = 1–4) Isolées en matrice

Ni(PH₃)_n species (where n = 1–4) were obtained by a co-condensation reaction of nickel vapour with phosphine, and stabilized at a low temperature in argon matrices. Infrared spectra in the Ni-P stretching vibration region provided evidence for their formation. Solid Ni(PH₃)₄ was isolated after removal of excess PH₃.     

Ab initio relativistic self-consistent-field (RSCF) wavefunctions for the diatomics Li2 and Be2

RSCF wavefunctions are calculated using the formalism of the authors. The results essentially agree with the non- relativistic calculations as expected because relativistic effects are negligible for these light atom diatomics.     

Gas phase electron diffraction study of tetravinyltin Sn(CHCH2)4

The tetravinyltin molecule has been studied by gas phase electron diffraction. The r_a structure analysis is based on the assumptions that a single conformer occurs in Sn(CHCH₂)₄ and that tin has a tetrahedral bond configuration. The preferred model (S₄ symmetry) predicts all four vinyl groups to be intermediate between staggered and eclipsed conformations. The structure refinement gives the following parameters (bond lengths, r_a, in nm, valence angles in degrees):

, SnCC = 121.9(0.6), CC = 0.1349(8), SnCH = 116.8(4.5),<C—H?_av. = 0.1098(14). The uncertainties given in parentheses represent three times the standard deviation values.The observed shortening of the

bond in Sn(CHCH₂)₄ from

in SnMe₄ (by 0.0027 nm) is equal to the shortening that occurs on going from

in ethane to

in propylene. With the corresponding Si and Ge derivatives, this effect is less pronounced.     

Preferential energy transfer from N2(A) to specific energy levels of Cu atoms

Emission spectra resulting from reaction of “clean” N₂(A³ Σ_u⁺) with copper atoms were studied using a flowing afterglow apparatus. The population distribution of the Cu states was calculated from the spectrum; it indicates that Cu atoms are excited by nearly resonant energy transfer processes. N₂(A,v') + Cu(²S_{$\text{1}\text{2}$}) → N₂(X, v) + Cu^* , and that the transfer is most efficient for N₂(A,v') → N₂(X,v) transitions with large Franck-Condon factors. The preferential energy transfer results in population inversion between some of the Cu states.     

1H and 13C NRM and infrared spectral studies on mixed ligand complexes of the type cis-[Co(en)2(Im)Cl]Cl2

A number of mixed ligand complexes of the type [Co(en)₂(Im)Cl]Cl₂ (Im = imidazole or a substituted imidazole) have been synthesized by reaction of trans-[Co(en₂Cl₂]Cl with the imidazole ligands. Electrical conductivity measurements support the ionic (1:2) formulation of the compounds, the electronic spectra is in agreement with an octahedral stereochemistry, and the IR and NMR (¹H and ¹³C) spectra strongly favour the cis configuration for the isolated complexes, [Co(en)₂(Im)Cl]Cl₂.Trans-[Co(en)₂Cl₂]Cl reacts with KNCS to form cis-[Co(en)₂(NCS)₂Cl, the crystal structure of which is briefly reported. This lends additional support in favour of the probable cis configuration of the above complexes.     

A CNDO/2 investigation of the CH3/CF3 substitution effect

The variation of the A-C bond lengths with substitution of methyl by perfluoromethyl in molecules of the kind A(CH₃ )_n is investigated using the CNDO/2 method. Calculations were performed with A as fluorine, oxygen, nitrogen, sulphur and phosphorous and n = 1, 2 or 3. The variation of the A-C bond length can be explained qualitatively by combining two effects, (1) changes in the covalent bond order and (2) changes in the ionic bond strength. While the covalent bond order decreases in all cases, the extent of the decrease depending largely on the electronegativity of A, the ionic bond order increases for fluorine, oxygen, nitrogen and sulphur and decreases in the case of phosphorous. The variations in the ionic bond strength are found to depend on the electronegativity of A as well as on the number of substituted methyl groups.     

The orientational correlation parameter g2 of symmetrical benzene derivatives

Values for the orientational correlation parameter of liquid 1,3,5-trifluorobenzene and 1,3,5-trimethylbenzene at 295 K are reported. The results were obtained by combining the Cotton-Mouton constants and the intensity of the reorientational contribution to the depolarized Rayieigh scattering. The g₂ values are compared with the ratio of Rayleigh and single-particle rerorientation times, to which they are related in some models of molecular reorientation.     

Symmetry adapted versus symmetry broken wavefunctions: the 1s core level ions of O+2

It is shown that, for O₂, in a MC SCF determination of the core ionization potentials employing the full Molecular point group, very few (N-1)-particle configurations are required in order to account for the symmetry breaking in the corresponding Hartree-Fock calculations.     

Vibrational spectroscopic investigations of snse8-n molecules

The fundamental vibrations of 13 cyclic S_nSe_8-n (n = 7—2) molecules have been calculated using a modified Urey—Bradley force field with 9–14 independent force constants whose values have been adapted from those of Se₈ and S₈. Calculated wavenumbers are compared to those obtained by Raman spectroscopy for sulfur—selenium phases prepared by recrystallizing quenched molten mixtures of the elements as previously described. Agreement between the observed spectra and calculated wavenumbers is closest by assuming the existence of selenium—selenium bonds and the absence of isolated selenium atoms in S_nSe_8-n molecules. It is assumed that sulfur—selenium phases are mixed crystals with the following components in varying concentrations: 1,2-S₆Se₂, 1,2,3-S₅Se₃, 1,2,3,4-S₄Se₄, 1,2,5,6-S₄Se₄, 1,2,3-S₃Se₅ and 1,2-S₂Se₆. The presence of S₈ and Se₈ in some of the phases is indicated by the Raman spectra.     

Picosecond time-resolved Sn← S1 absorption spectrum of the tetracyanobenzene-toluene complex

The time-resolved absorption spectrum of the lowest excitcd singlet state (S₁) over the range 3 — 10 ps after 0.5 ps pulse excitation of the charge-transfer complex of 1,2,4,5-tetracyanobenzene and toluene shows an evolution with a 5 ± 3 ps time constant due to changes in configurations of the complex in S₁ associated with the reorientational relaxation of the solvent.     

Effect of quadratic interactions on the resonance raman scattering of T × t2 jahn-teller systems

Raman excitation profiles and depolarization dispersion curves are calculated for T × t₂ Jahn-Teller systems that are subject to quadratic vibronic (Renner-Teller) coupling as well as frequency changes of the active vibrational mode.     

Measurement and interpretation of the integrated infrared intensities of C2H2 and C2D2

The absolute IR intensities of acetylene and perdeuterio acetylene have been measured using the Wilson-Wells-Penner-Weber method. The intensity data have been analyzed in terms of dipole moment derivatives, bond charge parameters and atomic polar tensors. The experimentally determined intensity parameters have been compared with the corresponding values obtained from ab initio calculations.     

Calorimetric and spectroscopic studies of the critical phase transition in (CH3NH3)2[SnCl6]

(CH₃NH₃)₂[SnCl₆] undergoes a critical phase transition at 154.32 ± 0.06 K with the critical exponents α = 0.36 ± 0.04, α' = 0.19 ± 0.02, the critical entropy ratio 0.062 and the total transition entropy (1.60 ± 0.18) R. Infrared spectral change favors the order-disorder mechanism of the transition proposed from the thermodynamic data.     

Crystal structures and phase transition of Rb2TeBr6 (300-12.5 K)

Using 298 and 160(3) K diffractometer intensity data the structure of Rb₂TeBr₆ has been determined by single crystal X-ray technique and refined to a final R_w of 0.041 and 0.037, respectively (K₂PtCl₆ type structure, space group Fm3m, Z = 4 with a₂₉₈ = 10.773(4) Å and a₁₆₀ = 10.713(6) Å). The powder diffraction pattern from 300 to 12.5 K was recorded by a low-temperature Guinier diffractometer and camera. Below 45(5) K a second-order phase transition leads to a tetragonally distorted structure corresponding to a softening of the T_1g(Γ) rotary phonon. The powder pattern measured with the diffractometer at 12.5 K was used for structural refinement (R = 0.092). This low-temperature phase shows a ferrorotative displacement of the TeBr₆-octahedra with a tilt angle of 4.7(1) deg. (space group $\text{I4}\text{m}\text{, Z = 2, a = 7.4726(3)}$ Å and c = 10.7008(5) Å). The structural results indicate that there is no stereochemical activity of the lone pair electrons at Te(IV) even at very low temperatures. Phase transitions of Rb₂TeBr₆ and Rb₂TeI₆ (A_2g(X)-condensation) are compared. The results of a lattice dynamic calculation shows that only the T_1g(Γ) condensation can be explained with a rigid ion model.     

Investigations of vanadium oxide bronzes θ-(Fe1−yAly)xV2O5

The vanadium oxide bronzes θ-(Fe_1?yAl_y)_xV₂O₅ are Curie-Weiss paramagnets and hopping semiconductors. The samples studied were synthesized by direct solid-state reaction and investigated by the X-ray diffraction, differential thermal analysis, electrical resistivity, magnetic susceptibility, and Mössbauer techniques. The crystal lattice parameters, effective magnetic moments of Fe³⁺ cations, Curie-Weiss temperatures, and the values of ⁵⁷Fe hyperfine interaction parameters were determined. Endothermic effects were observed for some of the samples.     

Ab inttio structural analysis of some saturated 3- and 4-membered rings

Complete geometry optimizations of the ground states of ten 3- and 4-membered ring compounds have been carried out by ab initio SCF calculations using the gradient method at the 4–21 level. For sulfur, an optimized 3-3-21 basis has been constructed, and the importance of including d-functions is demonstrated. The main purpose of the study was to determine local orientations and geometries of the molecular CH₂-groups, information that is very difficult to obtain from experiment. A simple interaction model seems to account for the CH₂-group distortions in the 3-membered rings considered here, and also for similar structural deformations previously reported in a series of cyclopropyl derivatives.     

Br2 in an ar matrix: an example of complete damping of the resonance raman scattering amplitude in the discrete resonance limit

Raman scattering and relaxed fluorescence is observed upon cw laser excitation resonant with the lower vibrational manifold of the X(¹Σ_o+u) → B(³Π_o+u) transition of matrix isolated Br₂ at liquid He temperatures. The excitation profile of the relaxed fluorescence maps out the resonances, but neither detectable enhancement of Raman scattering nor resonance fluorescence is observed.