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1.
The rotational spectra of 12CH2F2 in seven of the nine fundamental vibrational states and also in overtone and combination states involving the ν4 mode were observed and assigned. Coriolis interactions between ν3 and ν7, ν2 and ν8, ν3 and ν9, and ν5 and ν7 were analyzed by using approximate expressions for the rotational levels. An effective Hamiltonian with the Coriolis term in the off-diagonal block was applied to stronger interaction between ν3 and ν9. Fermi resonance between ν3 and 2ν4 was found to be negligible. The ground state spectra of 12CH2F2 and of 13CH2F2 were remeasured to improve the accuracy of the rotational and centrifugal distortion constants. The Coriolis coupling constants and the energy differences between two vibrational levels in resonance, which were obtained through an analysis of the satellite spectra, are compared with the results derived from a normal coordinate analysis.  相似文献   

2.
Numerical methods for the analysis of high-resolution infrared spectra of symmetric top molecules perturbed by Coriolis interactions between degenerate and nondegenerate vibrational levels are discussed in the second order of approximation. Application to the high-resolution infrared spectra of the AsH3 molecule in the region of the fundamentals ν1, ν3 and ν2, ν4 yields considerably improved values of the molecular constants of AsH3, including the band origins rotational constants, Coriolis coupling constants, centrifugal distortion constants, and the parameter of the K-type doubling effect.  相似文献   

3.
Infrared spectra of thoformaldehyde, H2CS and D2CS, were observed in the gas phase at a resolution of better than 0.1 cm?1 from 4000 to 400 cm?1 using a Nicolet FTIR system. Vibrational band origins and rotational constants were determined for ν2, ν3, ν4, and ν6 of H2CS and for ν1, ν2, ν3, ν4, and ν6 of D2CS. The ν3, ν4, and ν6 bands of H2CS were analyzed as a set of three Coriolis interacting bands, and three Coriolis constants were determined; similarly the ν4 and ν6 bands of D2CS were analyzed as a pair of interacting bands and one Coriolis constant was determined. A general harmonic force field was determined, without constraints, to fit the vibrational wavenumbers, Coriolis constants, and centrifugal distortion constants. A zero-point (rz) structure was determined from the ground-state rotational constants, and the equilibrium (re) bond lengths were estimated.  相似文献   

4.
In the investigation of the 8 → 280 GHz region, 241 and 57 transitions of H12COOH and DCOOH, respectively, have been assigned to the ν7 and ν9 vibrational states coupled by a strong Coriolis resonance. The numerical analysis based on Watson's theory of centrifugal distortion coupled with the addition of Coriolis interaction allows us to obtain a set of parameters which fits the transitions well. The rotational spectra of the isotopic species HCOOD and DCOOD have also been investigated. In this investigation 55 and 67 transitions have been assigned to the ν7 and ν9 vibrational states of these two molecules, respectively. A very weak Coriolis resonance was detected. Two non-rigid independent rotors were thus employed and gave us a set of parameters which fits the transitions quite well. The rotational spectrum of the ground state of H12COOH, H13COOH, HCOOD, DCOOH, H12C16O18OH, and H12C18O16OH have been reinvestigated and a set of improved parameters was obtained for each species.  相似文献   

5.
The ν1 (CO stretching) and ν2 (CF stretching) bands of the FCO radical were observed with Doppler-limited resolution by an infrared diode laser spectrometer with Zeeman and source modulation. The FCO radical was generated by a 60-Hz discharge in one of the following three gas mixtures: O2 + C2F4, CO + SF6, and CO + C2F4, all diluted with He. The observed spectra were analyzed to determine the rotational constants, the centrifugal distortion constants, and the spin-rotation interaction constants. The band origins, 1861.6372(1) and 1026.1283(1) cm?1 [with standard errors in parentheses], which were obtained, were found to agree well with matrix data, 1857 and 1023 cm?1, respectively. The assignment of the observed spectra to the FCO radical was further supported by observing the ν1 band of F13CO, which was obtained from 13CO and SF6. The molecular structure and the force field of FCO are briefly discussed by using molecular constants obtained from the observed spectra.  相似文献   

6.
The millimeter- and submillimeter-wave spectrum of 13CD2F2 present in natural abundance in methylene fluoride-d2 (CD2F2) has been measured in the region 230-380 GHz. The spectrum was recorded using a frequency-modulated millimeter- and submillimeter-wave spectrometer. More than 200 rotational transitions in the ground state of 13CD2F2 with J≤45 and Ka≤8 have been assigned. A combined weighted least squares fit of the newly assigned transitions with previously reported microwave data has been carried out in the Watson's A- and S-reduced Hamiltonian. The data have been fitted with a standard deviation approaching the experimental accuracy, to provide improved values for the rotational and quartic centrifugal distortion constants, including sextic distortion constants for the ground state of 13CD2F2.  相似文献   

7.
The ν7 and ν9 fundamental bands of formic acid were studied by Fourier transform spectroscopy with a resolving power of 0.020 cm?1. Band centers obtained are ν7 = 626.158 cm?1 and ν9 = 640.722 cm?1. It was possible to determine rotational and centrifugal distortion parameters for both vibrational states v7 = 1 and v9 = 1 and also the two first-order Coriolis interaction parameters along z and x axes and the second-order Coriolis parameter along z axis. The stability of rotational and distortion parameters compared to ground state values confirms that a Watson type Hamiltonian is well adapted to such a problem.  相似文献   

8.
The rotational a-type spectra of isotopically enriched diazirine isotopomers, H212C14N15N and H212C15N2, have been recorded in the region between 8 and 300 GHZ; the latter isotopomer has been observed for the first time. Using Watson's A-reduced Hamiltonian, the rotational constants and the quartic and some sextic centrifugal distortion constants have been determined for the ground vibrational states.  相似文献   

9.
The rotational spectra of CD3I (v = 0; v3 = 1; v6 = 1) and of 13CD3I in its ground state were observed between 8 and 320 GHz. For the ground state of CD3I, pure quadrupole resonances were also measured by laser-radiofrequency double resonance. These data have been used to determine with high accuracy the rotational, centrifugal distortion, and hyperfine constants.  相似文献   

10.
The vibration-rotation bands ν1 + ν2 and ν2 + ν3 of ozone appearing in the 5.7 μm region have been recorded at a resolution of 0.019 cm?1 with a SISAM spectrometer. The rotational levels of the (110) and (011) vibrational states have been fitted using a Hamiltonian which takes into account the Coriolis interaction between these two states. The rotational and coupling constants deduced from this study have been used to calculate a list of the vibration-rotation lines which is of interest for high resolution studies of atmospheric spectra in the 1670–1890 cm?1 region.  相似文献   

11.
The rotational spectra of the first three vibrational states of nitric acid above 1000 cm−1, 7191, 6191, and 72, have been measured and analyzed. The 72 state, along with the previously published 71 state, show the rotational and centrifugal distortional constants have a near linear dependence on the υ7 vibrational quantum number. Large changes for several centrifugal distortion constants of the υ7 = n series of states are attributed to a c-type Coriolis resonance manifold between the ν7 and ν6 vibrational modes and the Hamiltonian reduction and representation used to fit the spectra. The 7191 and 6191 states have torsional splittings of 12.361(8) and 22.47(1) MHz, respectively. These splittings are large compared to 2.340(8) MHz of the 91 state and can be explained by a ∼1-2% mixing through anharmonic Fermi resonances with the 93 state, which has a large torsional splitting of ∼1760 MHz. The millimeter/submillimeter-wave spectrum of each state was fit separately to the experimental uncertainty of the measurements. The resultant rotational constants, distortional constants and inertial defects agree well with DFT calculations.  相似文献   

12.
The enriched 81Br isotopic species of bromofluoromethane has been investigated in the infrared and microwave regions. The rovibrational spectrum of the ν5 fundamental has been studied by high resolution FTIR spectroscopy, while the rotational spectra of the ground and v6 = 1 states have been observed by means of microwave spectroscopy. More than 2700 transitions have been assigned in the ν5 band and the analysis of the rovibrational structure reveals a first-order c-type Coriolis resonance with the v6 = 2 state. The present study improves the ground state constants available in the literature and enables the determination of further centrifugal distortion parameters together with the full bromine quadrupole coupling tensor. A set of spectroscopic parameters up to the sextic distortion terms for the vibrational excited states has been accurately evaluated for the first time.  相似文献   

13.
A high-resolution infrared spectrum of methane-d2 has been measured in the C-D stretching band region (2025–2435 cm?1). Rotational structures of the ν2 and ν8 bands have been assigned by use of the ASSIGN-diagram method, and the c-type Coriolis interaction between ν2 and ν8 has been analyzed. The band origins, ν2 = 2203.22 ± 0.01 cm?1 and ν8 = 2234.70 ± 0.01 cm?1, the rotational constants and the centrifugal distortion constants for the two bands, and the Coriolis coupling constant, ∥;ξ28c∥; = 0.182 ± 0.015 cm?1, have been determined.  相似文献   

14.
Infrared spectra of CH2F2 and CD2F2 have been measured under a medium resolution. The vibration-rotation bands of CD2F2 fundamentals have been analyzed and the assignment for the fundamentals of CD2F2 is given. In addition, a number of overtone and combination bands are observed for CH2F2, which helps to clarify the vibrational assignment for CH2F2. A normal coordinate treatment has been carried out: The force constants in a modified Urey-Bradley as well as the general valence force fields have been determined, the vibrational frequencies and the centrifugal distortion constants obtained from microwave spectroscopy being used. The force constants of the methylene fluoride molecule are discussed in connection with those of the related molecules. Special features of the CH2F2 and CD2F2 spectra are also described.  相似文献   

15.
The ground state millimeter-wave spectra of CH3NCH2 and CD3NCD2 have been measured. The rotational constants, centrifugal distortion constants, and barrier hindering internal rotation of the methyl group have been determined for both species. For the parent species Iα and ?(i,a) were also obtained, and for the perdeuteriated species the quadrupole coupling constants of 14N were determined.  相似文献   

16.
Three spectra of D216O between 2170 and 3090 cm?1 have been recorded with a Fourier transform spectrometer having a resolution of about 5 × 10?3 cm?1. A careful analysis of the bands 2ν2, ν1, and ν3 has led to a largely extended and more precise set of rotational levels belonging to the vibrational states (000), (020), (100), and (001). From this set, we have then been able to determine improved rotational constants for the ground state (000) and precise vibrational energies, rotational and coupling constants for the three interacting states (020), (100), and (001). The Fermi-type interaction between (020) and (100) as well as the Coriolis-type interactions between (100) and (001) and between (020) and (001) have been explicitly taken into account. Many vibrorotational resonances were detected and are discussed.  相似文献   

17.
The equilibrium bond length and the shape of the complete potential energy curve for the methyl radical CH3 are determined. This is done by fitting the experimental data [mainly from C. Yamada, E. Hirota, and K. Kawaguchi, J. Chem. Phys.75, 5256–5264 (1981)] using the nonrigid invertor Hamiltonian and a model anharmonic potential function. As a result the v2 (out-of-plane bending) dependence of the rotational constants is explained and the v2 dependence of the spin-rotation coupling constants is modeled. In addition, some of the vibrational energies and rotational, centrifugal distortion, and spin-rotation constants are predicted for the 13CH3, 12CD3, and 12CT3 isotopes.  相似文献   

18.
Rotational structure in the perpendicular fundamentals ν6, ν7, and ν8, and in the parallel component of 2ν9 of CD3CCH are fully analyzed at a resolution of 0.2–0.3 cm?1. The A1-E Coriolis resonances between ν4 and ν7, and ν5 and ν8 are analyzed by computer contour simulations. These permit accurate location of the parallel fundamentals, and determination of the associated Coriolis interaction constants. The fundamental vibrations ν5 and ν8 in CD3CCH lie only 4 cm?1 apart, and constitute the closest accidental Coriolis resonance yet studied by the simulation technique. The force field of methyl acetylene, constrained according to the hybrid orbital model, is calculated, using the recently determined molecular structure, and fitting all observed data, many of which have been revised in a number of recent studies.  相似文献   

19.
A high-resolution diode laser spectrum of the 882-cm?1 band of s-tetrazine has been obtained. A complete rotational analysis of this band, incorporating quartic and sextic centrifugal distortion coefficients, has been carried out. The rotational constants A, B, and C have been determined with an accuracy better than 10?5 cm?1. The analysis has shown the band to be A-type and, on this basis, the vibrational assignment of this band has been revised from ν12 to ν14.  相似文献   

20.
The J = 1 ← 0 and J = 2 ← 1 microwave rotational transitions of SiH3F and SiD3F have been measured for the ground and the v2 = 1, v3 = 1, v5 = 1, and v6 = 1 vibrational states, for which the various rotational and vibration-rotation interaction constants have been obtained. Both molecules show an X-Y Coriolis resonance between the ν2 and ν5 vibrational states, whose separation are 29 and 8 cm?1, respectively. In the case of SiD3F the resonance is very strong and an exact numerical diagonalization of the energy matrix was employed.  相似文献   

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