An AB3 high-resolution NMR spectrum in the solid state: 31P in P4S3

A high-resolution ³¹P NMR spectrum has been recorded in polycyrstalline tetraphosphorus trisulphide P₄S₃. The spectrum exhibits the resolved doublet and quartet structure characteristic of an AB₃ type spectrum, with chemical shift difference 185 ± 2 ppm and J = 70 ± 3 Hz.     

Sub-doppler two-photon spectrum of asymmetric rotor molecules: analysis of the qqQ rotational branch of the S1(1B2u)141 ← S0(1A1g) system of benzene-d1

The Doppler-free two-photon excitation spectrum of the ^qqQ branch of the 14¹₀ vibrational band of the S₁(¹B_2u) ← S₀(₁A_1g) transition of benzene-d₁ has been recorded using a cw single-mode dye laser coupled to an external concentric resonator. The spectrum has been analysed using a non-rigid Watson Hamiltonian. More than 200 lines with J up to 20 have been assigned and the rotational constants which best reproduce the spectrum are A¹_v = 0.181435, B¹_v = 0.169990, C¹_v = 0.089055 cm⁻¹. The K_a = odd lines of the ^qqQ₅(J) subbranch show small and quite regular perturbations of 60 ± 5 MHz which are probably due to a coupling to another vibrational state of the S₁ manifold.     

Temperature dependence of a superexchange interaction determined from merging effect of copper(II) EPR lines

An analytical expression describing the shape of an EPR spectrum containing two lines from differently oriented exchange coupled copper(II) complexes is presented and used for the determination of the interdimer exchange integral J′ in [Co(en)₃]₂[Cu₂Cl₈] Cl₂-2H₂O crystal. The value 2J′ = 0.0072 cm^?1 is found at room temperature and decreases linearly with temperature as a result of thermal lattice vibrations.     

Doppler-free rotational spectrum of methyl iodide. Nuclear quadrupole,spin-rotation and nuclear shielding tensors of iodine

The ground-state microwave spectrum of methyl iodide has been measured between 59 and 240 GHz with a molecular beam spectrometer and by use of the Lamb dip method. The following molecular parameters have been accurately determined: B = 7501275.70(2) kHz; D_J = 6.3070(2) kHz; D_JK = 98.762(3) kHz; H_J = ?0.0051(6) Hz; H_JK = 0.04(2) Hz; H_KJ 4.51(3) Hz; eq. Q = ?1934.136 (5) MHz; C_⊥= ?17.40(6) kHz; C_| = ?19.4(5) kHz; x_J = ?1.41(4) kHz; x_K = ?38(1) kHz and x_d = 26.2(6) kHz. The last three constants characterize the interaction of centrifugal distortion with quadrupole coupling. The data are used to determine the elements of the iodine nuclear magnetic shielding tensor. Comparisons of the shielding are made for molecules which contain one iodine atom.     

The direct l-type resonance spectrum of CF3CCH in the vibrational state v10=3: Extension of the theory of reduction to H6n terms

The direct l-type resonance spectrum of CF₃CCH has been measured in the v₁₀=3 vibrational state by means of waveguide microwave Fourier transform spectroscopy in the range 8–26 GHz. Three types of direct l-type resonance transitions induced by the (Δk=Δl=±2) interaction could be observed: 140 transitions following the ΔJ=0, Δk=Δl=±2, Δ|l|=0, selection rule covering values of J=17–61 and G=|k−l| from 1 to 7, 94 transitions following the ΔJ=0, Δk=Δl=±2, Δ|l|=±2, selection rule covering values of J=26–57 and G from 15 to 24, 90 transitions following the ΔJ=0, Δk=Δl=±4 selection rule covering values of J=34–80 and G from 3 to 12 and 13 transitions following the ΔJ=0, Δk=Δl=±6, k=∓1, l=∓1⇔k=±5, l=±3 selection rule for J=71-83. 14 A₁–A₂ splitting transitions with kl=+1 were measured from J=33 to 49. Strong perturbations due to Δ(k−l)=±3 interactions made possible the observation of perturbation-allowed transitions with selection rule k=±4, l=±3⇔k=±3, l=∓1. Furthermore, the rotational transitions J=2–1, 3–2 and 4–3 have been measured. To make use of the multiple fitting concept, the theory of reduction developed for the v_t=2 vibrational state by Sarka and Harder [K. Sarka, H. Harder, J. Mol. Spectrosc. 197 (1999) 254] has been extended to the v_t=3 vibrational state including terms up to H₆₂. Owing to problems in the reproduction of data with low K and A₁–A₂ symmetry, two types of fits have been performed using five reduced forms of the effective Hamiltonian. The first type of fit used a reduced data set for which part of the transitions has been omitted. The unitary equivalence of the determined parameter sets has been demonstrated including newly derived relations for parameters in v₁₀=3. In the second type of fit, the complete data set has been included, yielding satisfactory results only in one reduction. In both type of fits, parameters up to sixth order have been determined including the axial rotational constant A and the Coriolis constant Aζ for both values of l. General features of the direct l-type resonance spectrum in a v_t=3 level are discussed.     

Millimeter wave spectrum of gaseous bismuth monofluoride (BiF)

Rotational transitions of gaseous bismuth monofluoride (BiF) have been observed for the first time. The molecules were produced in a double oven system and subsequently led into the absorption cell at a temperature of 700 °C. Transitions (F′,J + 1,v) ← (F,J,v) with J = 4,6 and 7 and v = 0–6 in the O⁺ electronic ground state have been measured in the 65–110 GHz region. The hyperfine structure due to the Bi nucleus is completely resolved. Analysis of the spectrum yields the following rotational and hyperfine constants: Y₀₁ = 6894.89594(84) MHz, Y₁₁ = ?45.0474(11) MHz, Y₂₁ = 81.69(45) kHz, Y₃₁ = 0.177(51) kHz, Y₀₂ = ?5.5440(73) kHz, eq_eQ(Bi) = ?1150.28(12) MHz, eq_IQ(Bi) = 4.20(12) MHz, c_Bi = ?30.0(5) kHz. In the Dunham constants Y_lm contribution due to interaction with 1⁺-level is included. The equilibrium distance, potential and vibrational constants are derived.     

Measurement of hyperfine splitting in the OH radical by a radio-frequency microwave double resonance method

The RFMDR technique is used to investigate the hydroxyl radical spectrum. The experiment allows to analyse the magnetic hyperfine structure for J = 7/2 and 9/2 in the ²Π_3/2 state and gives more complete and accurate results than in previous works.     

Tetranuclear copper(II) complex with the heterocyclic azomethine ligand: Crystal structure and magnetic properties

A tetranuclear copper(II) complex based on azomethine, which is the condensation product of 1-phenyl-3-methyl-4-formylpyrazol-5-one with 1,3-diaminopropan-2-ol, is synthesized. The complex includes two different tetranuclear clusters: symmetrical and unsymmetrical. They have a pseudo-cubane structure and are in a ratio of 1 : 2. The quantum-chemical calculation shows that the “unsymmetrical” conformer does not correspond to the local minimum on the molecular potential energy surface. Its existence is thus determined by the crystalline packing effects. According to the results of measurements of the temperature dependence of the magnetic susceptibility, the ground spin state is a singlet caused by the overall antiferromagnetic interaction between the copper ions. Accepting the molar magnetic susceptibility of the complex to be equal to the sum of susceptibilities of the “symmetrical” and “unsymmetrical” clusters and assuming that the spin-Hamiltonian for both clusters includes three exchange parameters, the temperature dependence of the magnetic susceptibility of the complex is satisfactorily described with the following parameters of the model: J _1A = ?178, J _2A = 80, J _3A = 18, J _1B = ?26, J _2B = ?74, J _3B = 46 cm^?1, g _A = g _B = 2.05.     

The rotational spectra of the ground and first excited bending states of deuterium isocyanide,DNC, up to 2 THz

The pure rotational spectrum of deuterium isocyanide (DNC) was recorded in the frequency range from approximately 680 to 1985 GHz. Twenty-one new transitions in the vibrational ground and first excited bending states (01^e,f 0) have been assigned, namely R-branch transitions from J=9←8 to 25←24. In a least squares analysis of these new transition frequencies together with previously reported millimeter-wave data, spectroscopic parameters up to sextic order could be derived with high precision for both states. Furthermore, the ℓ-type doubling constant q and its centrifugal distortion terms q_J and q_JJ were obtained for the first excited bending state.     

Laser fluorescence studies of HF rotational relaxation

Rotation relaxation of HF in HF-Ar mixtures was observed using a laser infrared fluorescence technique. A specific vibrational-rotational state of HF was excited, and the fluorescence from HF was monitored. Total rotational energy-transfer rates, and individual state-to-state transition probabilities were obtained for υ = 1, J = 3 (ΔJ = ± 1, ±2) and υ = 1, J = 5; (ΔJ= ±1, ?2, ?3). The transition probabilities decreased with increasing ΔE_J,J, the energy transferred from R → T (rotation to translation). The data were fitted to a simple exponential model k_JJ, α exp(-ClΔE_J,J'l). C was estimated to be 1.55 ± 0.25 kcal^?1 mole.     

Rotationally resolved (3 + 1) rempi of H 2 via the B1Σ+u state

In the paper, we compare the results of our ab initio calculations for the ro-vibrational branching ratios resulting from a (3+1) REMPI of H₂ via the B¹Σ⁺_u state with the experimental data of Pratt, Poliakoff, Dehmer and Dehmer. These results indicate that non-Franck-Condon effects are less important here than in the (3+1) REMPI of H₂ via the C¹Π_u state. We observe that the ΔJ = ±3 peaks in the photoelectron spectrum are of negligible strength and that the ratio of ΔJ = +1 to ΔJ = −1 peak is independent of the ionic vibrational state. A detailed analysis indicates that these features arise as a result of a dynamic interference between the do and dμ ionization channels and do not imply either the smallness of the d-wave or the smallness of the j_t = 3 angular momentum coupling terms.     

Anomalous rotational state distribution for the O2 photofragment in the UV photodissociation of ozone

The coherent anti-Stokes Raman scattering (CARS) spectrum of O₂(¹Δ_g) formed in the photodissociation of ozone at 266 nm is presented. An anomalous propensity for even (J = 2,4,6, …) retational states is observed. This propensity effect is discussed in terms of symmetry restrictions and dynamical bias in the photolysis.     

The Fourier transform and diode laser spectrum of the ν2 band of diazomethane

The infrared spectrum of the ν₂ band (NN stretching) of gaseous diazomethane at 2100 cm^?1 has been measured by means of an interferometer and a tunable diode laser spectrometer. For the first time the rotational J and K_a structure of this A-type parallel band has been resolved. Since the spectrum was found to be perturbed it was not possible to fit the upper state levels to an overall hamiltonian. Nine subbands have been analysed with the support of millimeter wave data for the ground vibrational state. Term values for the ν₂ = 1 vibrational state with K_a up to 5 have been obtained and subband origins, effective rotational constants B and centrifugal distortion constants D and H were determined for each K_a substate.     

Octopole moment of CH3D

The magnitude of an effective octopole moment of CH₃D has been obtained as ΩCH₃D = (5.6 ± 1.5) × 10^?34 esu cm³ by a comparison of calculated and measured values of self-broadened linewidths for J = 6 → 7 transitions in the pure rotational spectrum of this molecule.     

Resonance in the rotational dependence of the isotope-selective reaction between IiCl(A 3Π1) and acetylene

The rotational dependence of the isotope selective reaction between IⁱCl(A ³Π_l, υ′, J′) and acetylene (C₂H₂, C₂D₂) forming the photoaddition product 1,2-iodo-chloro-ethyene was studied for ν′ = 19 and ν′ = 20. The enrichment factor in the photoproduct shows resonances for J′ = 32, ν′ = 19 and J′ = 6, υ′ = 20.     

Collision rotational transfers in NaH A1Σ+ by He,Ar or H2 (and in KH A1Σ+ by H2)

The total and relative rotational transfer cross sections σ_total and σ_Ji-Jf, by collisions of NaH A¹Σ with He, Ar or H₂, are measured from υ′ = 4 and υ′ = 11, J₁′ = 6. The σ_total increase as υ′ increases. They are similar for He and H₂ but much greater for Ar especially at large υ′. In NaH A¹Σ⁺ the bond goes from covalent to ionic as υ′ increases: σ_total is very sensitive to an attractive potential due to the interaction of the permanent electric dipole moment of the molecule with the polarizability of the atom (α_Ar = 11 au, α_He = 1.37 au). The σ_Ji-Jf decrease monotonously as |J_f-J_i| increases and may be fitted by a scaling law. The variation with ΔJ depends on the colliding gas but does not change appreciably with υ′: most of the transfers could take place on the repulsive part of the interaction potential, the shape of which would not depend on υ′.     

Microwave spectrum of N2D4, 14N quadrupole coupling constants,and the barrier to inversion of the amino group

The microwave spectrum of N₂D₄ has been observed and analyzed. Based on five low-J rotational transitions the effective rotational constants are: A = 74712.9 ± 1.9 MHz, B = 18500.42 ± 0.46 MHz, and C = 18439.91 ± 0.46 MHz. The quadrupole coupling constants of the ¹⁴N nuclei are X_aa = 4.23 ± 0.04 MHz, X_bb = 1.98 ± 0.05 MHz, and X_cc = ?2.25 ± 0.05 MHz. Using the observed ground state inversion splittings for N₂D₄ and N₂H₄ the barrier to inversion of a single amino group is computed to be 5.00 kcal mol^?1.     

Measurement of deuterium quadrupole coupling in CH3OD

K = 1 → 0 transitions in CH₃OD for J = 1, 2, 3 and 4 E₂-type states were measured using a beam maser spectrometer with 6 kHz linewidth (fwhm). Analysis of J = 1 and J = 2 spectra provided a deuterium quadrupole coupling strength along the O-D bond dijection of eg_zzQ = 303 ± 12 kHz.     

Rotational isomerism. A gas-phase 1H nuclear magnetic resonance study of 1-bromo-2-chloroethane

The average vicinal coupling constants of 1-bromo-2-chloroethane at different temperatures have been obtained in a gas-phase ¹H NMR study of 1,2-disubstituted ethanes. Analysis of the experimental data, assuming a ”static” model with constant values for the vicinal coupling constants of the individual rotamers, yielded unacceptable results. A ”dynamic” model, which takes into account the torsional vibrations, has therefore been developed and used to analyse the gas-phase results. The values at 305 K for the vicinal coupling constants of the individual rotamers are: trans rotamer J_T = 13.6 Hz, J'_t = 4.9 Hz; gauche rotamer $\text{1}\text{2}$(J_G1 + J_G2) = 0.9 Hz, $\text{1}\text{2}$(J'_G1 + J'_G2) = 7.8 Hz. These couplings are temperature-dependent with J_T changing about four times as much as the other coupling constants. Analysis of the average vicinal coupling constants, measured in different solvents, with the “dynamic” model gave values for the vicinal coupling constants of the individual rotamers in excellent agreement with those from the gas-phase data. The value of $\text{1}\text{2}$(J_G1+ J_G2) decreases noticeably with increasing dielectric constant of the solution. This can be explained by changes in the average dihedral angle between the coupling protons, in the gauche rotamers, which leads to changes of J_G1 and J_G2 in the same direction.