The molecular conformation and dipole moment of 1,4-thioxane from the microwave spectrum

The microwave spectrum of 1,4-thioxane, a heterocyclic analogue of cyclohexane, has been studied in the region 26.5–40 GHz. The molecule is a highly asymmetric rotor (k = ?0.0740917). From the analysis of the a-type transitions, the rotational constants determined are (in MHz) A = 4333.85, B = 3076.14 and C = 1991.96. A study of the Stark effect has yielded the dipole moment components (in Debye units) μ_a = 0.290 ± 0.003, gm_c = 0.0537 ± 0.0004, which give a total dipole moment of μ = 0.295 ± 0.003. These data are consistent with a chair conformation for the ring.     

Microwave spectrum,dipole moment and barrier to internal rotation of trans-methyl glyoxal

The microwave spectrum of the trans conformer of methyl glyoxal has been investigated in the frequency range from 8 to 40 GHz. The rotational constants have been determined for the A state: A = 9102.4332(31), B = 4439.8832(27) and C = 3038.9404(22) MHz. Quantitative measurements of the Stark effect have yielded the components of the electric dipole moment: μ_a = 0.1597(11), μ_b = 0.9620(7) and μ_total = 0.9751(7) D. From the splittings of rotational transitions the three-fold barrier to internal rotation of the methyl top has been found to be V₃ = 269.1 (3) cm^?1.     

Avoided-crossing molecular-beam spectroscopy of CH3SiF3

The avoided-crossing molecular-beam method has been applied to CH₃SiF₃ in the ground torsional state. Stark and hyperfine rotational anticrossings have been studied, along with barrier anticrossings in which the zero-field energy differences depend only on the torsionial splittings. For υ = 0, pure rotational spectra were measured forJ = 13 ← 12 and 14 ← 13 with a mm-wave spectrometer and for J = 1 ← 0 with the molecular-beam spectrometer. Stark and Zeeman studies have been carried out with conventional beam techniques. From a simultaneous analysis of existing microwave data for υ ? 2 and the current measurements, it was found that the moment of inertia of the methyl top I_α = 3.170(2) amu A², the effective rotational constants A^eff = 4059.522(22) Mhz, and the effective height of the barrier V₃^eff = 413.979(14) cm^?1. The true values of A and V₃ have been obtained within certain approximations. The rotational constant B and several distortion constants including D_K were evaluated. In addition to determining the electric dipole moment μ 2.33938(14) D, the data yielded values for the distortion dipole constants μ_D and μ_J, and the molecular g-factors g_| and g_⊥.     

Microwave spectrum of aminoborane,BH2NH2

The unstable species aminoborane, BH₂NH₂, has been identified as a reaction product of ammonia with diborane by microwave spectroscopy. The rotational constants determined are A = 138212 ± 4 MHz, B = 27487.83 ± 0.10 MHz and C = 22878.44 ± 0.11 MHz for ¹¹BH₂NH₂ and A = 138199 ± 6 MHz, B = 28420.36 ± 0.11 MHz and C = 23520.78 ± 0.12 MHz for ¹⁰BH₂NH₂. The dipole moment is 1.844 ± 0.015 D.     

Microwave spectrum,rotational constants and dipole moment of s-cis acrolein

The microwave spectrum of a second conformer of acrolein is reported for the first time. Ground-state rotational constants and quartic centrifugal distortion constants were determined from 42 transitions in the range 8–60 CHz. The small inertial defect establishes its planarity. The dipole moment of s-cis acrolein is μ_a = 2.010(5) D, μ_b = 1.573(3) D and μ_total = 2.552(3) D.     

Microwave spectrum and rotational isomers of epifluorohydrin

The microwave spectra of three rotational isomers of epifluorohydrin are Presented. The ground and 3 excited torsional states of one of the two gauche rotamers (III), and the ground states of the other gauche and cis rotamers (I & II), have been observed. The values of the ground state rotational constants. A, B, and C for rotamers I, II and III are 14 662.8, 3129.4, 2863.3; 10 645.8, 4050.2, 3679.1; and 14 833.1, 3210.2, 2933.9 MHz. The gaseous phase dipole components for the most abundant rotamer (III) are μ_a = 0.99 ± .02, μ_b = 2.90 ± .01 and μ_c = 0.0 ± .3, giving μ = 3.08 ± .02 D.     

Microwave spectrum and dipole moment of norbornane

The microwave spectrum of norbornane has been studied in the 26–40 GHz region. The rotational constantsA = 3694.246 MHz B = 3212.566 MHz, C = 2774.813 MHz and the dipole moment μ = 0.091(8) D have been determined. These values are compared with electron diffraction data.     

Microwave spectrum,centrifugal perturbation,dipole moment,and conformation of 5-methyl-1,3-dioxane

The microwave spectrum of 5-methyl-1,3-dioxane was studied in the frequency range 12–35 GHz. The a and c type rotation transitions with J≤30 were identified. The rotational constants A = 4658.5244(33) MHz, B = 2383.3930(12) MHz, and C = 1724.28907(88) MHz and the quartic constants of the centrifugal distortion of the molecule in the ground vibrational state were determined. The components of the dipole moment were found, μ _a = 1.76 ± 0.01 D and μ _c = 1.10 ± 0.01 D; the net dipole moment of the molecule is μ = 2.08 ± 0.01 D. 5-Methyl-1,3-dioxane was calculated by the B3PW91/aug-cc-pVDZ density functional theory method. The calculated data are compared with the experimental data. The most stable conformation is the chair conformation with an equatorial orientation of the methyl group.     

Microwave spectrum and dipole moment of glycolic acid

More than 200 rotational transitions of glycolic acid (CH₂OHCOOH) have been assigned in the frequency range 18–40 GHz. Rotational constants and centrifugal distortion constants for the ground state and two vibrationally excited states were deduced. From Stark splittings the dipole moment was determined: μ_a = 1.913(5), μ_b = 0.995(14) and μ_total = 2.156(9) D.     

Microwave spectrum,centrifugal perturbation,dipole moment,and conformation of 4-methyl-1,3-dioxane

The microwave spectrum of 4-methyl-1,3-dioxane is studied in a frequency range from 16 GHz to 40 GHz. The rotational transitions of a-, b-, and c-types with J ≤ 57 are identified. The rotational constants (MHz) A = 4802.335(2), B = 2376.163(1), C = 1738.852(1) and the quartic constants of the centrifugal distortion are found for the ground vibrational state of the molecule. The components of the dipole moment (D) μ _a = 0.73(1), μ_b = 1.32(1), μ_c = 1.36(1) and the total dipole moment μ = 2.03(1) are determined. The experimental data obtained correspond to the chair conformation of the molecule with the equatorial orientation of the methyl group.     

Microwave spectrum,centrifugal distortion constants,dipole moment and quadrupole coupling constants of pentafluoropyridine

Pentafluoropyridine has been analysed in the frequency range of 8 to 18 GHz at dry ice temperature, using a conventional 100 kHz Stark modulated microwave spectrometer. The rotational constants and centrifugal distortion constants are A = 1481.539 ± 0.003 MHz, B = 1075.348 ± 0.004 MHz and C = 623.101 ± 0.001 MHz; and d_J = ?0.39 ± 0.06 kHz, d_JK = 1.86 ± 0.27 kHz, d_K = 0.70 ± 0.1 kHz, d_EJ = (0.3 ± 0.03) × 10^?6 and d_EK = (?1.5 ± 0.2) × 10^?6. The electric dipole moment has been found to be 0.98 ± 0.08 D and the values of the quadrupole coupling constants are x_aa = 1.94 ± 0.22 MHz, x_bb = ?4.08 ± 0.06 MHz and x_cc = 2.14 ± 0.22 MHz. A simple analysis based on Townes and Dailey theory points to a considerable increase in the π-electron density and excess charge on the nitrogen site.     

The microwave spectrum and structure of trifluoro-ethylene

The microwave spectrum of trifluoroethylene F₂C=CHF is reported, and a number of ground state and vibrationally excited state lines are assigned. The ground state rotational constants are: 10665.31, 3872.36, 2837.97 MHz. The dipole components are μ_a = 0.075 D, μ_b = 1.30 D, and μ_total = 1.30 D. Calculations of the inertia defect of the ground and excited states indicate that the equilibrium configuration is planar.     

Infrared-microwave double resonance study of the ν4 fundamental band of POF3

Three-level and four-level infrared-microwave double resonance effects have been observed in a POF₃ sample contained in a microwave waveguide Stark cell that was modified to permit transmission of radiation from a CO₂ infrared gas laser. In three-level double resonance experiments laser pumping of rotational states in the ν₄ = 1 vibrational state greatly increased the signal/noise for observation of Stark-shifted rotational transitions in the excited vibrational state. The frequencies of the observed excited state transitions were used to confirm the assignment of laser Stark spectra and to obtain independent measures of the rotational constant B and the dipole moment for ν₄ = 1. The observation of four level double resonances could be explained qualitatively by the assumption of dipole selection rules for collision-induced transitions. However, the intensities of the double-resonance effects could not be explained by this simple model.     

First-order stark effect and electric dipole moment of H3P … HC15N by pulsed-nozzle fourier-transform microwave spectroscopy

The first-order Stark effect in the J = 4 ← 3, K = 1 transition of the weakly bound dimer H₃P … HC¹⁵ N has been obeserved and measured by pulsed-nozzle Fourier-transform microwave spectroscopy under the selection rules ΔM = O and ΔM = ± 1. The electric dipole moment μ= 4.046(47) D determined for H₃P … HC¹⁵ N has been interpreted in terms of an enhancement Δμ = 0.60 D on dimer formation.     

Stark effect measurement on Ca79Br X2Σ+

Using a molecular beam laser—microwave double resonance experiment, high-precision Stark effect measurements were performed on the electronic and vibrational ground state of Ca⁷⁹Br. The dipole moment was determined to be μo = 4.364(20)D. Furthermore the use of labeling techniques has been demonstrated in which a ground-state rotational transition is induced to label a specific hyperfine component of an optical emission line.     

Spectra and structure of small ring compounds: Part XXX. Microwave spectrum of 1,1-difluoro-1-silacyclopent-3-ene

The microwave spectrum of 1,1-difluoro-l-silacyclopent-3-ene has been recorded from 26.5 to 40.0 GHz. Only A-type transitions were observed. The R-branch assignments have been made for the ground state and the first three excited states of the ring puckering vibration. It is shown that the five-membered ring structure is planar from the values of the components of the dipole moment, as well as from the value of the inertial defect as a function of the ring puckering quantum number. From the relative intensity measurements, it is concluded that the first excited state of the ring puckering vibration has a frequency of 38 ±7 cm^?1 and that the vibration is nearly harmonic. The components of the dipole moment were determined by the Stark effect to be μ_a = 2.02 ±0.06 D, μ_b = 0, and μ_c = 0.0 ±0.09 D. All of the observed data are consistent with a molecule of C_2v symmetry and the possible reasons for this structure are discussed.     

Stark quantum beat spectroscopy of polyatomic molecules

We derive analytical expressions for Stark quantum beat signals of polyatomic molecules and discuss them with regard to molecular and geometrical parameters. The general treatment is specified for near prolate asymmetric rotor molecules and a method for determining rotational constants and all components of the dipole moment of electronically excited polyatomic molecules is presented. The method is tested and illustrated for the vibrationlessS ₁ state of deuterated propynal (HC ≡ CCDO,C _s symmetry) and its lowest frequency non-totally symmetric state 12¹. The results of the vibrationless state are compared with structural data reported in the literature. For the 12¹ state we obtainA=1.5004(43) cm^?1,B=0.16131(34) cm^?1,C=0.14623(34) cm^?1, and the components of the electric dipole moment in the molecular plane μ _a =?0.88(2)D, μ _b =1.03(2)D. Furthermore, it is shown that the modulation depth of Stark quantum beat signals can be utilized to quantify the contribution of the individual components of the transition moment to the total emission.     

The microwave spectrum and electronic structure of cyanogen azide

The rotational spectrum of cyanogen azide has been assigned and yields values of A = 38.06737 GHz, B = 3.18517 GHz and C = 2.93357 GHz. The measured dipole moment components of μ_a = 2.96 D, μ_b = 0.44 D. μ_total = 2.99 D are compared with those computed using a CNDO/2 approach for NCN₃ and several related molecules.     

Microwave spectrum,barrier to internal rotation and dipole moment in 5-methyl-pyrimidine

The microwave rotational spectrum of 5-methyl-pyrimidine has been investigated in the region from 8 to 27 GHz, the three types of lines to be expected for a molecule of this symmetry and with a very low sixfold barrier hindering internal rotation of the methyl top have been found: m = 0; |m| ≠ 0,3; |m| = 3n. From the m = 0 (a-type transitions) the rotational constants A′ (less methyl top) = 6108.41, B = 2642.198, C = 1844.196 MHz and the dipole moment μ = 2.881D have been determined. From the wide splitting of the lines |m| = 3, |k| = 1 the potential barrier has been derived as V₆ = 11.73 cal/mole.     

Microwave-optical double resonance of a supersonic beam: ICI B3Π(O+) v = 0

Several microwave transitions have been observed between hyperfine levels in I³⁵Cl B³Π(0⁺) v=0 using the technique of microwave-optical double resonance. The ICI was cooled to 3 K in a seeded supersonic expansion, allowing examination of low J lines. Values for the rotational constant, B₀ = 0.085873(6) cm^?1, and quadrupole coupling constant cQqI = ?664(9) MHz, were determined.