Electronic structure of arsabenzene: Microwave spectrum,dipole moment,and nuclear quadrupole coupling constants

The microwave spectrum of arsabenzene was analyzed; a dipole transitions were observed. The following rotational constants were obtained; A = 4871.03 ± 0.18 MHz, B = 2295.87 ± 0.01 MHz, C = 1560.10 ± 0.01 MHz. The dipole moment was 1.10 ± 0.04 D. The nuclear quadrupole coupling constants due to the ⁷⁵As nucleus were χ_aa = ?186.4 ± 0.1 MHz, χ_bb = 43.5 ± 0.2 MHz, χ_cc = 142.9 ± 0.2 MHz, and the asymmetry parameter, η = 0.533 ± 0.002. Analysis of the quadrupole coupling constants indicated that the population of the 4p orbitals on arsenic decrease in the order n_a > n_b > n_c.     

The microwave spectrum,structure and nuclear quadrupole coupling constants for stibabenzene

The microwave spectrum of 121-SbC₅H₅, 123-SbC₅H₅, β-dideutero 121-SbC₅H₃D₂ and 123-SbC₅H₃D₂ has been assigned in the region 26.5–40.0 GHz. The respective rotational constants and uncertainties are: A = 4512.69 ± 0.42, B = 1738.00 ± 0.01, C = 1254.51 ± 0.01; A = 4512.84 ± 0.30, B = 1729.80 ± 0.01, C = 1250.22 ± 0.01; A = 4176.18 ± 0.33, B = 1660.94 ± 0.01, C = 1188.15 ± 0.01; A = 4176.60 ± 0.61, B = 1652.94 ± 0.03, C = 1184.03 ± 0.03 (in MHz units). The structure is found to be planar, C_2v in symmetry. The $\text{d(}\text{Sb-C}\text{) = 2.050 ± 0.005}\text{A}\text{?}$ and ∠CSbC = 92.9° ± 1.0°. The nuclear quadrupole coupling constants for the 121 and 123 antimony isotopes are χ_aa = 456.4 ± 4.1 MHz, η = 0.396 ± 0.008, and χ_aa = 583.00 ± 5.3 MHz, η = 0.399 ± 0.008, respectively. Several alternate techniques using the coupling constants as data support a σ-donating property for antimony.     

Microwave spectrum,structure, dipole moment,and quadrupole coupling constants of isopropylamine

The microwave spectra of (CH₃)₂CHNH₂, (CH₃)₂CHNHD, and (CH₃)₂CHND₂ have been assigned and analyzed. Only c-type, R-branch transitions were identified. The observed spectra correspond to the trans rotamer, as shown by planar moments, the deuterium isotope effect, dipole moment components, and the N quadrupole coupling constants. The CN bond distance is shorter than that observed in methyl amine, as expected, and significantly longer than that in the analogous closed-ring compound cyclopropylamine.     

Microwave spectrum,centrifugal distortion constants,and quadrupole coupling constants of 3-chloropyridine

The microwave spectrum of 3-chloropyridine has been measured in the frequency region of 8.2 to 18 GHz. The rotational constants, centrifugal distortion constants, and the quadrupole coupling constants for the ³⁵Cl species are A = 5839.448 ± 0.027 MHz, B = 1604.152 ± 0.005 MHz, C = 1258.327 ± 0.004 MHz, Δ_J = 0.10 ± 0.01 KHz, Δ_JK = 0.36 ± 0.09 KHz, Δ_K = 1.18 ± 0.07 KHz, δ_J = ?0.008 ± 0.005 KHz, δ_K = 0.88 ± 0.20 KHz, χ_aa = ?70.04 ± 0.38 MHz, χ_bb = 36.68 ± 0.19 MHz. The values of rotational constants and quadrupole coupling constants for the ³⁷Cl species are A = 5840.052 ± 0.034 MHz, B = 1559.354 ± 0.01 MHz, C = 1230.739 ± 0.016 MHz, χ_aa = ?54.20 ± 1.26 MHz, χ_bb = 29.49 ± 0.48 MHz. The double bond character in the CCl bond is found to be 2%. The smaller than expected value of rotational constant A points to a “fattening” of the pyridine ring about the a-axis in contrast to 2-chloropyridine, where no such substitution effect was observed.     

Molecular structure, nuclear quadrupole coupling constant and dipole moment of nitrogen trichloride from microwave spectroscopy

The rotational constants of four isotopic species of nitrogen trichloride have been obtained from transitions in the millimeter region. Two r_s structures have been obtained with the following average values of the parameters. rN−C1=1.7535 ± 0.0020 A.The Stark effect of the J = 3 ← 2 transition was analyzed to obtaine the value 0.39 ± 0.01 D for the dipole moment of NCl₃. The measurement of the separation of the two strongest hyperfine components of the J = 2 ← 1 transition yielded the value of −108 ± 3 MHz for the N---Cl bond axis quadrupole coupling constant.     

Quadrupole coupling constants and centrifugal distortion constants of 3-bromopyridine from its microwave spectrum

The microwave spectrum of 3-bromopyridine has been investigated in the frequency range of 12–18 GHz and 30–40 GHz at dry ice temperature. The rotational, centrifugal distortion and quadrupole coupling constants of the two isotopic species ⁷⁹Br and ⁸¹Br have been evaluated. From the quadrupole coupling constants, double bond character in the CBr bond has been found to be 2.2% and the group electronegativity of the pyridyl radical to be 2.34.     

The microwave spectrum and centrifugal distortion constants of propiolic acid

The microwave spectra of propiolic acid and propiolic acid-d have been measured up to J = 30. These have enabled accurate evaluation of the rotational and centrifugal distortion constants for each species. The measured frequencies are presented, along with some predictions of transitions unmeasured in the present work, but of potential use in radioastronomy.     

Further study of the microwave spectrum of chlorine lsocyanate: The substitution structure and nuclear quadrupole coupling

The microwave spectra of three further isotopic species of chlorine isocyanate (³⁵Cl¹⁵N¹²C¹⁶O, ³⁷Cl¹⁵N¹²C¹⁶O, ³⁵Cl¹⁴N¹³C¹⁶O) have been measured. From them we have obtained rotational constants, centrifugal distortion constants, and nuclear quadrupole coupling constants. The data are combined with earlier data (1) to confirm the planarity of the molecule, and to give a full substitution structure as follows: $\text{r}\text{(ClN) = 1.705 ± 0.005}\text{A}\text{?}$; $\text{r}\text{(NC) = 1.226 ± 0.005}\text{A}\text{?}$; $\text{r}\text{(CO) = 1.162 ± 0.005}\text{A}\text{?}$; < (ClNC) = 118°50′ ± 30′; < (NCO) = 170°52′ ± 30′, with Cl and O trans. We have also calculated the chlorine and nitrogen quadrupole coupling constants using the SCF-MO-CNDO method, and have obtained good agreement with the measured values. Evidence for in-plane π-bonding at nitrogen has been obtained.     

The microwave spectrum and centrifugal distortion constants of vinyl fluoride

The rotational spectrum of vinyl fluoride up to J = 40 has been assigned and measured in the frequency region 8–37 GHz. Both a- and b-type transitions were observed. These measurements have been combined with those made in other frequency regions to calculate refined rotational constants and to obtain all quartic and some sextic centrifugal distortion constants. A comparison is made between the quartic centrifugal distortion constants measured here and those calculated from vibrational data.     

Microwave spectrum,structure, quadrupole coupling constants,dipole moment,and barrier to internal rotation of N-methylhydroxylamine

The microwave spectrum has been observed and analyzed for five isotopic species of N-methylhydroxylamine. For the normal species the rotational constants (in Megahertz) are A = 38 930.771 ± 0.005, B = 3939.607 ± 0.002, and C = 8690.716 ± 0.001. These data show that the molecule exists in the trans conformation, with structural parameters that include the following: CN = 1.460, NO = 1.461, NH = 1.007, and OH = 0.962. Hyperfine structure analyses have yielded the complete inertial axis ¹⁴N quadrupole coupling constant tensor, and thus the tensor values in the electric field-gradient principal axis system as follows: χ_xx = 4.41 ± 0.30, χ_yy = 1.93 ± 0.45, and χ_zz = ?6.34 ± 0.30 MHz. The total electric dipole moment has been found to have the value μ_T = 0.71 D, and the barrier to internal rotation of the methyl group is 3.55 kcal/mole.     

Microwave spectrum,molecular structure,and nuclear quadrupole coupling constants of 3-bromopropene

The microwave spectra of the two ⁷⁹Br and ⁸¹Br isotopic species of 3-bromopropene were measured in the frequency region 14–23 GHz. The R and Q branches for a- and b-type rotational transitions of one conformer, skew, have been assigned and the rotational constants of the ground state have been determined to be A = 19 247.56 MHz, B = 1975.339 MHz, and C = 1914.761 MHz for ⁷⁹Br species, and A = 19 234.26 MHz, B = 1961.417 MHz, and C = 1901.563 MHz for ⁸¹Br species, respectively. By the analysis of the second-order perturbation treatment of the quadrupole interaction, it is found that the χ_ab element of the χ tensor primarily contributes to the anomalous hyperfine splittings. The matrix elements of products of direction cosines in terms of the symmetric top wavefunctions have been derived. The nuclear quadrupole coupling constants have been determined χ_aa = 384.2 MHz, χ_bb = ?71.9 MHz, χ_cc = ?276.3 MHz, and |χ_ab| = 358.7 MHz for ⁷⁹Br species and χ_aa = 283.2 MHz, χ_bb = ?55.6 MHz, χ_cc = ?227.6 MHz, and |χ_ab| = 296.0 MHz for ⁸¹Br species.     

Microwave spectrum,structure, dipole moment,quadrupole coupling constant,and internal motion of thioformamide

The r_s structure of thioformamide has been determined from the microwave spectra of the normal as well as isotopic species of the molecule. The structural parameters obtained assuming the planarity of the molecule are $\text{NH}{}_{\mathrm{c}}\text{= 1.001}{}_8\text{± 0.006}\text{A}\text{?}\text{,}\text{NH}{}_{\mathrm{t}}\text{= 1.006}{}_5\text{± 0.003}\text{A}\text{?}\text{,}\text{CN}\text{= 1.358}{}_2\text{± 0.003}\text{A}\text{?}\text{,}\text{CS}\text{= 1.626}{}_2\text{± 0.002}\text{A}\text{?}\text{,}\text{CH}{}_{\mathrm{a}}\text{= 1.09}{}_6\text{± 0.08}\text{A}\text{?}\text{, ?}\text{H}{}_{\mathrm{c}}\text{NH}{}_{\mathrm{t}}\text{, = 121°42′ ± 40′, ?}\text{H}{}_{\mathrm{c}}\text{NC}\text{= 117°55′ ± 40′, ?}\text{H}{}_{\mathrm{t}}\text{NC}\text{= 120°22′ ± 30′, ?}\text{NCS}\text{= 125°16′ ± 15′ ?}\text{NCH}{}_{\mathrm{a}}\text{= 108°}{}_{\mathrm{5\prime }}\text{± 5°,}\text{and}\text{?}\text{SCH}{}_{\mathrm{a}}\text{= 126°}{}_{\mathrm{39\prime }}\text{± 5°}$.The dipole moment is calculated from the Stark effects of the three transitions to be μ_a = 3.99 ± 0.02 D, μ_b = 0.13 ± 0.25 D, and μ_total = 4.01 ± 0.03 D, where the c component is assumed to be zero.The quadrupole coupling constant of the ¹⁴N nucleus is estimated using the doublet splittings observed for six Q-branch transitions; χ_cc - χ_bb = ?5.39 ± 0.15 MHz and χ_aa = 2.9 ± 1.2 MHz.Two sets of vibrational satellites are observed and assigned to the first excited state of the amino wagging and the NCS bending vibrations, respectively. The relative intensity measurement gives the vibrational energies of 393±40 cm^?1 and 457 ± 50 cm^?1 for NH₂CHS and 293 ± 30 cm^?1 and 393 ± 40 cm^?1 for ND₂CHS. The amino wagging inversion vibration in the molecule is discussed in comparison with that in formamide. It is most probable that the thioformamide molecule is also planar without any potential hump to the amino inversion at the planar configuration.     

The microwave spectrum,structure, and dipole moment of amino acetonitrile

The microwave spectra of three isotopic species of amino acetonitrile (NH₂CH₂CN, NHDCH₂CN, and ND₂CH₂CN) have been investigated to learn something about the structure and bonding in this and similar compounds. The only rotamer observed is the form in which both NH bonds are gauche to the CN group and the structure is quite rigid. From the available data only the bond angles are well determined. The amino NCC angle is 114.5(3)°, the HCH angle is 103(2)°, the HNC angle is 109.6(4)°, and the HNH angle is 107(1)°. The dipole moment components are μ_a = 2.577(7) D and μ_b = 0.5754(10) D; these agree quite well in magnitude and direction with the sum of the acetonitrile and methyl amine dipoles. The rigidity of the molecule and its preference for the form in which the amino protons are closest to the triple bond confirms a suggestion based on earlier studies on similar molecules that there is a strong hydrogen bonding interaction between the amino group and the nitrile group, although in this molecule dipole-dipole forces also probably play a significant role in determining the structure and its rigidity.     

The microwave spectrum,structure, and dipole moment of propiolyl fluoride

The microwave spectrum of propiolyl fluoride has been observed in the frequency region 12.5–40 GHz. Rotational transitions have been assigned for the ground and two excited vibrational states of the normal isotopic species and for the ground vibrational state of the deuterated species. In each case, values for the rotational constants and centrifugal distortion constants have been obtained. The molecule has been shown to be planar and structural calculations suggest no anomalies in any of the internuclear parameters. Stark effect measurements have yielded a value of 2.98 ± 0.02 Debyes for the dipole moment.     

The microwave spectrum of methyl chlorodifluoroacetate: Methyl internal rotation and chlorine nuclear electric quadrupole coupling

A chirped pulse microwave spectrometer has been used to record microwave spectra of the ³⁵Cl and ³⁷Cl isotopologues of methyl chlorodifluoroacetate, CClF₂C(O)OCH₃, between 8 GHz and 16 GHz. The target compound was spectroscopically examined as it participated in a supersonic expansion of argon. Only one conformer was observed. The rotational spectra were recorded with sufficient resolution to observe (i) splittings due to the internal rotation of the methyl group, and (ii) splittings from the coupling of the chlorine quadrupolar nucleus. A total of 785 transitions have had quantum numbers assigned. Analysis of the spectra observed has produced an experimental barrier to the methyl group internal rotation, V₃, of 370(2) cm⁻¹. It is noted that this barrier is a little lower than that determined for methyl acetate [V₃ = 425 cm⁻¹, J. Sheridan, W. Bossert and A. Bauder, J. Mol. Spectrosc., 80 (1980) 1-11], and this is rationalized through a comparison of molecular structures. Lastly, all components of both the ³⁵Cl and ³⁷Cl chlorine nuclear electric quadrupolar coupling tensor have been determined.     

The breakdown of the Born-Oppenheimer approximation for a diatomic molecule: The dipole moment and nuclear quadrupole coupling constants

In the Born-Oppenheimer approximation the dipole moment of the vibrational levels of a ¹Σ electronic state of a heteronuclear diatomic molecule can be expressed as a power series in [$\text{(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v +}\text{1}\text{2}\text{)}$], where v is the vibrational quantum number, and to order $\text{(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)}{}^2$ this expression is

$\text{μ}{}_{\mathrm{v}}\text{=[μ}{}_{\mathrm{e}}\text{+(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)}{}^2\text{μ}{}_{\mathrm{c}}\text{]+μ}{}_1\text{[(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v+}\text{1}\text{2}\text{)]+μ}{}_2\text{(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v+}\text{1}\text{2}\text{)]}{}^2$

Similarly the nuclear quadrupole coupling constant eQq of each nucleus in the molecule can be expressed as

$\text{eQq=[eQq}{}_{\mathrm{e}}\text{+(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)}{}^2\text{eQq}{}_{\mathrm{c}}\text{]+eQq}{}_1\text{[(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v+}\text{1}\text{2}\text{)]+eQq}{}_2\text{(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v+}\text{1}\text{2}\text{)]}{}^2$

In this paper the effect of the breakdown of the Born-Oppenheimer approximation on the expressions for μ_v and eQq for an isolated ¹Σ ground electronic state of a heteronuclear diatomic molecule is determined. The effect is to change only μ_c and eQq_c and, therefore, to alter the relationship between the μ_v or eQq values of two isotopes of a molecule. The intensities of the lines in the rotation and rotation-vibration spectrum are also slightly modified by this effect.For the HCl molecule we find that

$\text{μ}{}_{\mathrm{v}}\text{=[1.0908+(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(164)]+8.6[(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v+}\text{1}\text{2}\text{)]?9.5[(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v+}\text{1}\text{2}\text{)]}{}^2\text{D}$

where the second term (+164 D) would have the value ?4 D in the Born-Oppenheimer approximation. Similarly for the ³⁵Cl nucleus of the HCl molecule we have

$\text{eQq=[?66.806+(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(2460)]?472.23[(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v+}\text{1}\text{2}\text{)]+750[(}\text{B}{}_{\mathrm{e}}\text{ω}{}_{\mathrm{e}}\text{)(v+}\text{1}\text{2}\text{)]}{}^2\text{MHz}$

where the second term (+2460 MHz) would be ?110 MHz in the Born-Oppenheimer approximation.