Partial chlorine-chlorine intermolecular scattering functions for XCl4 liquids (X = C,Si, Ge,V, Ti,Sn) from neutron diffraction and the RISM

Combining neutron diffraction intermolecular scattering functions with RISM partial scattering function for X-X and X-Cl atom paris the Cl-Cl partial scattering functions are obtained. The systematic trends in Cl-Cl partial scattering functions and radial distribution functions in six different tetrachloride liquids have been investigated. The intermolecular nearest neighbour Cl-Cl distance of 0·377(14) nm corresponds well with the value of 0·34 nm adopted for the chlorine hard sphere diameter in the RISM calculations.     

四氯乙烯的同步辐射光电离研究

利用VUV同步辐射光源和反射式飞行时间质谱仪，在超声冷却条件下对四氯乙烯(C₂Cl₄)进行了光电离研究，通过测量各离子的光电离效率(PIE)曲线，得到了C₂Cl₄的电离势IP(C₂Cl₄) =(9.36±0.05)eV及C₂Cl₄光解离碎片离子C₂Cl₃⁺，C_{关键词： 真空紫外光电离 离子出现势 电离势 四氯乙烯}     

An E.S.R. study of electron irradiated K3IrCl6 in a NaCl host lattice

Electron irradiation of the diamagnetic [Ir^IIICl₆]^3- ion in a NaCl host lattice produces two paramagnetic species. ESR studies indicate that these slightly different species can be assigned to a [Ir^IICl₆]^4- complex, with 5d ⁷ low spin configuration, arising from the capture of an electron in a d_z ² orbital. The almost zero value for the quadrupolar interaction and the negative value for the core polarization field per unpaired spin are discussed in terms of a ligand field theory and the group overlap integral for the A _1g molecular orbital is calculated from the experimental data.     

Multiexponential decay of negative molecular ions as a result of target molecule distribution over vibrational states

The lifetimes of long-lived negative molecular ions SF₆⁻-, C₆H₅NO₂⁻, and C₆F₆⁻ are measured with a static mass spectrometer. A great spread in published data for the lifetimes of these ions is explained using a concept of multiexponential decay of molecular ions. The influence of the Boltzmann distribution of neutral target molecules over vibrational states on the lifetime of negative molecular ions is studied in terms of the Illenberger-Smirnov-Kompaneits simple statistical model. It is shown that this distribution has a profound effect on the multiexponential decay of molecular anions and, as a consequence, on the lifetime of negative molecular ions measured on different mass spectrometers.     

Outer vibrational turning points near dissociation in the B(3Π0u +) state of Br2 and Cl2

A [1, 0] Padé approximant to the long-range interaction energy is used to describe the outer limb of the Rydberg-Klein-Rees curve of the state B (³Π_0u ⁺) of Br₂ and Cl₂. Empirical values of C ₅ and C ₆ are obtained.     

Electron density in Si2 and Cl2

Self consistent field-Xα molecular orbital calculations have been performed for Si₂ and Cl₂ using both the scattered-wave (SW) and LCAO discrete-variational (DV) versions of the method. For Si₂ an SW calculation including f partial waves yields orbital densities in good agreement with those from methods which do not involve the muffin-tin approximation for the potential. The present results afford a further comparison relevant to the recent discussion (see, M. Schlüter et al. [9]) of the relative accuracy of various pseudocharge densities compared with real charge densities. The deformation density from the Xα-SW calculation is in good agreement with that from the DV-Xα method and also with that from the linear muffin tin orbital method (J. Harris and R. O. Jones [8]). Differences between the valence electron distribution which is usually discussed in connection with pseudopotential schemes, and the density distribution including the 2s and 2p core electrons are delineated. For Cl₂, the Xα-SW deformation density shows positive lobes along lines through the atoms perpendicular to the bond axis, is negative for most of the area between the atoms and also shows negative lobes behind the atoms. This deformation map is in good qualitative agreement with the DV-Xα map and also with recent ab initio results with the exception of a small region at the centre of the bond in which the DV-Xα and ab initio results show an excess of electrons compared with the promolecule whereas the Xα-SW results show a deficiency. Comparisons with X-ray results on solid chlorine are inconclusive so that experimental electron scattering data on gas phase chlorine will be required to resolve this difference.     

Dipole oscillator strength properties and dispersion energies for CI2

A recommended isotropic dipole oscillator strength distribution (DOSD) has been constructed for the chlorine molecule through the use of quantum mechanical constraint techniques and experimental dipole oscillator strength and molar refractivity data. It has been used to evaluate a variety of dipole oscillator strength sums, logarithmic dipole oscillator strength sums, and mean excitation energies for the molecule. A pseudo-DOSD for C1₂ is also presented which is used to obtain reliable results for the isotropic dipole-dipole dispersion energy coefficients C₆, for the interaction of Cl₂ with itself and forty-two other species, and the triple-dipole dispersion energy coefficient C₉ for (Cl₂)₃.     

On the composition-dependent isotope effect of HTSC in the two-band model

The oxygen isotope effect in high-T_C superconductors has been investigated on the basis of a two-band model where superconducting phase transition is induced by interband (mainly Coulombic) interaction. The isotope shift of T_C appears due to the dependence of averaged interband electronphonon coupling constant on oxygen mass. This coupling has a repulsive nature and gives a relatively small contribution to the total interaction inducing superconductivity. The calculated isotope effect exponent depending on the carrier concentration has been compared with the experimental one as a function of x for La_2-xSr_xCuO₄.     

A quasi analytical method for the calculation of virial coefficients for realistic intermolecular potentials

The difficulties of accurately representing the Ursell function, f, for molecules interacting with a Lennard-Jones potential by a hard sphere core and a truncated exponential series are discussed. The range of R for which a hard sphere approximates f with negligible error is established and the range of arguments in f is determined. The accuracy with which the exponential series, S_k , truncated after k terms, represents the function is established for several ranges of arguments. It is shown that it is possible to represent f accurately by a hard sphere core and S ₄ or S ₆ for all values of R except over a short range of R.

Values of B and C, accurate to within a few per cent, can be obtained analytically through approximating f by S ₄ or S ₆ and a hard core whose diameter is determined by the range of arguments for which the series is valid. More accurate values of B and C required additional approximations for f. Two of these, the repulsive square well and the Barker-Henderson radius, give accurate values of B and C at all temperatures that were examined.     

Microwave and infrared spectroscopy of the CH4—OCS complex

Pulsed molecular beam spectra of the CH₄-OCS complex have been recorded using both a molecular beam infrared diode laser and a Fourier transform microwave spectrometer. Analysis of the spectrum yields a near T shape structure with a centre of mass separation of 3.83 Å and a CH₄ centre of mass-OCS centre of mass-oxygen angle of 73°. Splittings attributed to the internal rotations of methane within the complex have been observed in the microwave spectrum. The rotational constants of the complex for the A and T librational states of CH₄ were determined. The differences (T-A) in the rotational constants were ΔA = 0.35, ΔB = ?1.60 and ΔC = ?1.85 kHz.     

Theoretical studies on the nature and strength of an intermolecular non-covalent Te•••π interaction

ABSTRACT

DFT and MP2 calculations were used to determine the nature of non-covalent tellurium–π interactions in R₂Te???C₆H₆ (R = H, F, Cl, CH₃) and C₄H₄Te???C₆H₆ systems. The results showed that the strength of Te···π interaction follows the order F₂Te > Cl₂Te > tellurophene > H₂Te > Me₂Te. Also, the F₂X···π system complexes (X = Te or Se, π system = C₆F₆, C₆(CH₃)₆, Cr(C₆H₆)₂ and coronene) were studied for investigating the direction of charge flow in Te···π interaction. The obtained data expressed that the existence of electron withdrawing group on Te atom increases the strength of Te???π interaction while the fluorine atoms on benzene ring decrease it. The breakdown of ΔE_int in the R₂Te···C₆H₆ (R = H, F, Cl, CH₃) and C₄H₄Te···C₆H₆ systems using two dispersion corrected DFT methods showed that when the R group on divalent tellurium atom is an electron withdrawing substituent, the contribution of ΔE_elstat and ΔE_orb in total interaction energy increases and the value of ΔE_int is relatively large. The present data also showed that the intermolecular Te···π interactions are slightly stronger than corresponding Se···π interactions.     

Preparation and characterization of organic–inorganic hybrid compound [N(C<Subscript>4</Subscript>H<Subscript>9</Subscript>)<Subscript>4</Subscript>]<Subscript>2</Subscript>Cu<Subscript>2</Subscript>Cl<Subscript>6</Subscript>

Organic–inorganic hybrid sample [N(C₄H₉)₄]₂Cu₂Cl₆ was prepared via the reaction between copper chloride and tetrabutylammonium chloride. The compound was characterized by X-ray powder diffraction, IR, Raman, differential scanning calorimetry (DSC), DTA-TGA analysis and electrical impedance spectroscopy. DSC studies indicate a presence of one-phase transition at 343 K. The complex impedance of compound [N(C₄H₉)₄]₂Cu₂Cl₆ have been investigated in temperature and frequency ranges 300–380 K and 200 Hz–5 MHz, respectively. The Z′ and Z″ versus frequency plots are well fitted to an equivalent circuit model. The circuits consist of the parallel combination of bulk resistance R _p and constant phase elements CPE. The frequency dependence of the conductivity is interpreted in term of Jonscher's law: s(w) = s_dc + Awⁿ \sigma (\omega ){ } = {\sigma_{\rm{dc}}} + { }A{\omega^n} . The conductivity follows the Arrhenius relation. The variation of the value of these elements with temperatures confirmed the availability of the phase transition at 343 K detected by DSC and electrical measurements.     

Application of Nutations to Studying the Exchange Processes by the Method of Nuclear Quadrupole Resonance Spectroscopy

A method of direct determining the discontinuous rotational reorientation angles from NQR exchange spectra based on recording of two-dimensional nutations of magnetization after the mixing period is suggested. The possible modification of the Jeener pulse sequence with independently varying duration of pulses for obtaining a 2D exchange nutation spectrum is described. Shapes of singularities in the 2D nutation spectrum of CCl₂- and CCl₃-group reorientations, which depend on the angle _S between C–Cl bonds and on the asymmetry parameter for nonequivalent positions of nuclei participating in the exchange are examined. The 2D exchange NQR nutation spectra of ³⁵Cl in powders prepared from C₂Cl₄ and C₂Cl₆ molecular crystals are modeled. The advantages and capabilities of the method are discussed.     

Site–site potential function and second virial coefficients for linear molecules

The second virial coefficients for several linear molecules were calculated using the 2CLJ potential including the electrostatic and induction effects with modified mixing rules for unlike pairs. Least squares fits of experimental values for B(T) were used to calculate the energy parameters σ and ε in the LJ core potential for N₂, O₂, Cl₂, F₂, CO, CO₂, NO, N₂O, C₂H₆, C₂F₆ and the strongly polar molecules CH₃Cl, CH₃F, CH₃CF₃, CH₃CHF₂, and CF₃CH₂F. The analysis takes into account rotation of the dipole out of the molecular axis. The calculated results for the second virial coefficient agree well with experimental data. In addition, the effect of the induction terms on the potential for calculating the second virial coefficient is shown to be important only for the molecules with strong dipole or quadrupole moments.     

On the delay mechanism of Cl<Stack><Subscript>2</Subscript><Superscript>−</Superscript></Stack> diatomic anion dissociation up to the microsecond timescale

The dissociative capture of slow electrons by tetrachlorethylene (C₂Cl₄) has been investigated by resonant electron capture negative ion mass spectrometry. Metastable ions with fractional mass numbers 7.5, 17.5, and 19 corresponding to the C₂Cl₄⁻ → Cl⁻ + C₂Cl₃ and Cl₂⁻ → Cl⁻ + Cl decays occurring at the microsecond timescale have been detected. It has been revealed that Cl₂⁻ anions, which are fragment ions, can dissociate at the microsecond timescale, which is very surprising for a system with one internal degree of freedom. This process is assumingly attributed to the rotational excitation of Cl₂⁻ anions. Thus, the experimental estimate of the time of rovibronic relaxation in the Cl₂⁻ anion has been obtained.     

一种利用混合介质测量SBS介质布里渊线宽的方法

提出了一种利用双池受激布里渊散射(SBS)系统选用混合介质,进而测量SBS介质布里渊线宽的方法.在紧凑双池SBS系统的放大池中放入待测介质,在振荡池中放入布里渊频移可调的混合介质,测出放大池待测介质增益系数随布里渊频移偏离的洛伦兹曲线,该曲线半高处的线宽即为待测介质的布里渊线宽.实验上在Nd:YAG调Q激光系统中,选用CCl₄/C₆H₆混合介质,测量了四氯乙烯(C₂Cl₄)、六氯丁二烯(C_{关键词： 受激布里渊散射 混合介质 布里渊线宽}     

Long- and short-range order in the Pd<Subscript>6</Subscript>B monoclinic superstructure and M<Subscript>6</Subscript>X<Subscript>5</Subscript> and M<Subscript>6</Subscript>X allied superstructures

Symmetry analysis of the Pd₆B monoclinic superstructure (space group C2/c) formed in the cubic (with the B1 structure) solid solution of boron in palladium (PdB _y ) has been carried out. The formation of this superstructure proceeds as a first-order phase transition via the disorder-order channel including nine nonequivalent superstructure vectors of four stars {k ₁₀}, {k ₄}, {k ₃}, and {k ₀}. For the Pd₆B monoclinic super-structure (space group C2/c), the distribution function for boron atoms is calculated and the interval of admissible values of the long-range order parameters is defined. It is shown that the transition channel determined in this way coincides with the channel in which the M₆X monoclinic superstructure (space group C2) is formed; therefore, the Pd₆B superstructure can also be described in space group C2 to the same degree of accuracy. The higher symmetry of the monoclinic model (space group C2/c) suggests that it describes the structure of the Pd₆B phase (Pd₆B□₅), as well as of mutually inverse phases M₆X□₅ and M₆X₅□, more adequately than the model with space group C2. It is shown that superstructures of the M₆X□₅ type (space groups C2/c, C2, C2/m, and P3₁) and inverse superstructures of the M₆X₅□ type with the same space groups have the positions of the nearest surrounding of metal atoms by two types of nonmetallic sublattice sites located in the first and second coordination spheres.     

ESR studies of Cl2- (VK) centre trapped in irradiated Ca(ClO3)2 . 2H2O single crystals

A Cl₂- centre has been trapped in X or γ-irradiated Ca(ClO₃)₂. 2H₂O single crystals at 298 K, when the irradiated crystals were illuminated with ultra-violet light (360 nm). This centre is formed at the expense of ClO₂ centres in this crystal. This Cl₂ ^- centre is trapped at two magnetically inequivalent sites in the crystal lattice and these sites become equivalent when the static magnetic field is parallel or perpendicular to the b axis. At many orientations this centre reveals ‘super-hyperfine’ interaction with a proton (I = 1/2) of the water of crystallization. The magnetic parameters are close to those observed in alkali chlorides and the E.S.R. spectrum has been fitted to an orthorhombic spin hamiltonian. The principal g values are g_xx = 2·035, g_yy = 2·033 and g_zz = 2·000 and those of the A values are A_xx = 15·0, A_yy = 31·0 and A_zz = 109·0 G. The shfs parameters are A _‖' = 5·0 A _⊥' = 1·0 G. The V_K centre trapped in this lattice is exceptionally stable at room temperature.     

Cluster–cluster fusion

An experimental study of molecular fusion in fullerene–fullerene collisions is presented and the theoretical interpretation of the cross section is reconsidered in terms of phase space arguments and competition with direct collision induced dissociation. The form and absolute magnitude of the cross sections for C⁺₆₀+C₇₀ (or C⁺₇₀+C₆₀) and C⁺₇₀+C₇₀ can be understood, however, the much smaller cross section for C⁺₆₀+C₆₀ remains a puzzle. The fragmentation behaviour of the hot fusion product is well described by a maximal entropy model indicating equipartition of the centre of mass collision energy followed by statistical fragmentation. To cite this article: E.E.B. Campbell et al., C. R. Physique 3 (2002) 341–352.     

The effect of the hydrogen fluoride chain on the aromaticity of C6H6 in the C6H6···(HF)1–4 complexes

The effect of the hydrogen fluoride chain ((HF)_n) on the aromaticity and π character of C–C bonds of C₆H₆ in the C₆H₆···(HF)_n (n = 1–4) complexes were investigated using density functional theory employing RM05 functional. It was found that the binding energy between C₆H₆ and different (HF)_n chains showed a maximum at n = 3 (C₆H₆···(HF)₃). Also, the π–hydrogen interaction (πHI) and the bifurcated fluorine interaction (BFI) increased and decreased the π character of the C–C bond of C₆H₆, respectively. In addition, the change of aromaticity of the C₆H₆ due to the interaction with the HF chains was also studied using three different aspects such as aromatic fluctuation index (FLU), average two centre index (ATI) and proton nuclear magnetic resonance (HNMR) spectrum. The most change in the aromaticity happens when the C₆H₆ interacts with (HF)₃ chain. The variation of aromaticity with the binding energy and the summation of two-body terms were investigated and very good linear correlations were observed.