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1.
The high-resolution infrared spectrum of cyclopropane (C3H6) has been measured from 100 cm−1 to 2200 cm−1. In that region we have identified 24 absorption bands attributed to six fundamental bands, five combination bands, three hot bands and 10 difference bands. Long pathlength spectra, up to 32 m, facilitated the identification and analysis of many previously unstudied infrared inactive, and Raman and infrared inactive vibrational states, including direct access to two forbidden fundamental states, ν4 and ν14. An improved set of constants for the ground vibrational state as well as for the fundamental vibrations ν7, ν9, ν10, ν11 are also reported. The spectral resolution of the measurements varied from 0.002 cm−1 to 0.004 cm−1.  相似文献   

2.
The emission spectrum of NbN has been reinvestigated in the 8000-35 000  cm−1 region using a Fourier transform spectrometer and two groups of new bands were observed. The bands observed in the 18 000-20 000 cm−1 region have been assigned to a new 3Π-X3Δ transition. Three bands with R heads near 19 463.8, 19 659.0 and 19 757.0 cm−1 have been assigned as 0-0 bands of the 3Π2-X3Δ3, 3Π1-X3Δ2 and 3Π-X3Δ1 subbands, respectively, of this new transition. Three additional ΔΩ = 0 bands have been observed in the 24 000-26 000  cm−1 region. A 0-0 band with an R head near 25 409.9 cm−1 has been assigned as a ΔΩ = 0 transition having X3Δ2 as its lower state while two additional bands with heads near 25 518.7 and 25 534.8 cm−1 were found to be ΔΩ = 0 bands having X3Δ1 as the common lower state. Two of these three bands are perhaps subbands of a 3Δ-X3Δ transition. Most of the excited levels are affected by perturbations.  相似文献   

3.
The Fourier transform gas-phase IR spectrum of 1,2,3-thiadiazole, C2H2N2S, has been recorded with a resolution of ca. 0.003 cm−1 in the 700-1100 cm−1 spectral region. Four fundamental bands ν6(A/; 1101.8 cm−1), ν7(A/; 1038.8 cm−1), ν9(A/, 858.9 cm−1), and ν13(A//; 746.2 cm−1) have been analyzed using the Watson model in A-reduction. Two additional bands, ν8 (A/; 894.6 cm−1) and ν12(A//; 881.2 cm−1) were assigned by their weak Q-branches. Ground state rotational and quartic centrifugal distortion constants as well as upper state spectroscopic constants have been obtained from fits. A number of weak global and local interactions are present in the bands. The resonances identified were qualitatively explained by Coriolis type perturbations with neighboring levels. Ground state rotational and quartic centrifugal distortion constants, anharmonic frequencies, and vibration-rotational α-constants predicted by quantum chemical calculations using a cc-pVTZ basis and B3LYP methodology, have been compared with the present experimental data, where there is generally good agreement.  相似文献   

4.
The Fourier transform infrared spectrum of gaseous thiophene, C4H4S, has been recorded in the 600-1200 cm−1 spectral region with a resolution of ca. 0.0030 cm−1. Five fundamental bands ν13 (B1, 712.1 cm−1), ν7 (A1; 840.0 cm−1), ν6 (A1; 1036.4 cm−1), ν5 (A1; 1081.5 cm−1) and ν19 (B2; 1084.0 cm−1) have been analysed by the standard Watson model (A-reduction). Ground state rotational and quartic centrifugal distortion constants have been obtained from a simultaneous fit of ground state combination differences from four of these bands and previous microwave transitions. Upper state spectroscopic constants have been obtained for all five bands from single band fits using the Watson model. A strong c-Coriolis resonance perturbs the close lying ν5 and ν19 bands. We have analysed this dyad system by a model including first and second order Coriolis resonance using the theoretically predicted Coriolis coupling constant . From this analysis we locate the previously unobserved ν19 band at 1083.969 cm−1. The rotational constants, ground state quartic centrifugal distortion constants, anharmonic frequencies, and vibration-rotational constants (α-constants) predicted by quantum chemical calculations using a cc-pVTZ basis with B3LYP methodology, are compared with the present experimental data, where there is generally good agreement. A complete set of anharmonic frequencies and α-constants for all fundamental levels of the molecule is given.  相似文献   

5.
The Fourier transform gas-phase infrared spectrum of pyrrole, C4H5N, has been recorded with a resolution of ca. 0.003 cm−1 in the 900-1500 cm−1 spectral region. Four fundamental bands, ν8(A1; 1016.9 cm−1), ν23(B2; 1049.1 cm−1), ν7(A1; 1074.6 cm−1), ν20(B2; 1424.4 cm−1) and the overtone band 2ν16(A1; 962.7 cm−1) have been analysed using the Watson model. The ν8 and 2ν16 bands are unperturbed; the ν7 and ν23 bands are locally perturbed, while the ν20 band is globally perturbed by weak c-Coriolis resonance. Upper state vibrational term values, and rotational and centrifugal distortion constants, have been obtained from fits using S-reduction and Ir-representation as well as A-reduction and IIIr-representation. A set of ground state rotational and centrifugal distortion constants using A-reduction was obtained from a simultaneous fit of ground state combination differences from all five bands and previous microwave and millimetre-wave data.  相似文献   

6.
The jet-cooled spectrum of pentafluoroethane (C2HF5) has been recorded between 1100 and 1325 cm−1 at a resolution of 0.0022 cm−1. A rotational temperature of approximately 10 K was achieved by expanding 50 Torr of C2HF5 in 500 Torr of helium. Transitions belonging to five different fundamental vibrations have been assigned and fit to a Watson Hamiltonian: the ν3 band at 1309.880494(189) cm−1, ν4 at 1200.734645(67) cm−1, ν5 at 1142.78147(33) cm−1, ν13 at 1223.334098(115) cm−1, and ν14 at 1147.394185(163) cm−1. The fit of the ν4 band has an rms deviation of 0.000436 cm−1 compared to the uncertainty in the experimental line position of 0.0002 cm−1. Satisfactory fits were achieved for the other four bands (ν3, ν5, ν13, ν14) at this cold temperature, with most of the centrifugal distortion constants fixed at the ground state values. Joint fits with previous work were attempted for the ν4 and ν13, successfully in the former case and unsuccessfully in the latter.  相似文献   

7.
The emission spectra of CaH and CaD have been recorded at high resolution using a Fourier transform spectrometer and bands belonging to the E2Π-X2Σ+ transition have been measured in the 20 100-20 700 cm−1 region. A rotational analysis of 0-0 and 1-1 bands of both the isotopologues has been carried out. The present measurements have been combined with the previously available pure rotation and vibration-rotation data to provide improved spectroscopic constants for the E2Π state. The constants ΔG(½) = 1199.8867(34) cm−1, Be = 4.345032(49) cm−1, αe = 0.122115(92) cm−1, re = 1.986633(11) Å for CaH, and ΔG(½)=868.7438(46) cm−1, Be = 2.212496(51) cm−1, αe = 0.036509(97) cm−1, re = 1.993396(23) Å for CaD have been determined.  相似文献   

8.
Assignments of the vibrational fundamentals of cis- and trans-1,3,5-hexatriene are reevaluated with new infrared and Raman spectra and with quantum chemical predictions of intensities and anharmonic frequencies. The rotational structure is analyzed in the high-resolution (0.0013-0.0018 cm−1) infrared spectra of three C-type bands of the trans isomer and two C-type bands of the cis isomer. The bands for the trans isomer are at 1010.96 cm−1 (ν14), 900.908 cm−1 (ν16), and 683.46 cm−1 (ν17). Ground state (GS) rotational constants have been fitted to the combined ground state combination differences (GSCDs) for the three bands of the trans isomer. The bands for the cis isomer are at 907.70 cm−1 (ν33) and 587.89 cm−1 (ν35). GS rotational constants have been fitted to the combined GSCDs for the two bands of the cis isomer and compared with those obtained from microwave spectroscopy. Small inertial defects in the GSs confirm that both molecules are planar. Upper state rotational constants were fitted for all five bands.  相似文献   

9.
The gas phase infrared emission spectrum of the A3Σ-X3Π electronic transition of SiC has been observed using a high resolution Fourier transform spectrometer. Three bands ν′ − ν″ = 0-1, 0-0, and 1-0 have been observed in the 2770, 3723, and 4578 cm−1 regions, where the 0-1 and 0-0 bands were observed for the first time. The SiC radical was generated by a dc discharge in a flowing mixture of hexamethyl disilane [(CH3)6Si2] and He. A total of 1074 rotational transitions assigned to the 0-1, 0-0, and 1-0 bands have been combined in a simultaneous analysis with previously reported pure rotational data to determine the molecular constants for SiC in the two electronic states. The principal equilibrium molecular constants for the A3Σ state are: Be = 0.6181195(18) cm−1, αe = 0.0051921(20) cm−1, re = 1.8020884(26) Å, and Te = 3773.31(17) cm−1, with one standard deviation given in parentheses. The effect of a perturbation was recognized between the ν = 4 level of X3Π and the ν = 0 level of A3Σ, and the analysis was carried out to determine the interaction parameter between the two states.  相似文献   

10.
The absorption spectrum of the natural sample of nitrous oxide has been recorded at Doppler limited resolution with a Fourier-transform spectrometer in the spectral range 5000-10 000 cm−1. Ten cold bands (8Σ − Σ and 2Σ − Π), thirteen hot bands (11Π − Π, Σ − Σ, and Δ − Δ) of 14N216O and the 3ν3 band of 14N15N16O have been newly detected. The uncertainty of the line position determination is estimated to be about 0.005 cm−1 for unblended lines. The assignment of the spectrum has been done with the help of the prediction performed within the framework of the polyad model of effective Hamiltonian. The spectroscopic parameters Gv, Bv, Dv, Hv, and qv have been determined for all newly detected bands. The line intensities of 13 weak bands have been measured. The uncertainty of the obtained line intensity values varies from 7 to 13%.  相似文献   

11.
Line intensities of 13C16O2 have been measured between 5851 and 6580 cm−1 using CW-cavity ring down spectroscopy (CRDS) and in the 4700-5050 and 6050-6850 cm−1 regions using Fourier transform spectroscopy. As a result of the high sensitivity (noise equivalent absorption αmin∼3×10−10 cm−1) and high dynamics allowed by CW-CRDS, accurate line intensities of 2039 transitions ranging between 1.1×10−28 and 1.3×10−23 cm−1/(molecule cm−2) were measured with an average accuracy of 4%. These transitions belong to a total of 48 bands corresponding to the ΔP=9 series of transitions. Additionally, unapodized absorption spectra of 13C-enriched samples have been recorded using a high-resolution Bruker IFS125HR Fourier transform spectrometer. Spectral resolutions of 0.004 cm−1 (maximum optical path difference (MOPD)=225 cm) and 0.007 cm−1 (MOPD=128.6 cm), and pressure×path length products in the ranges 5.2-12 and 69-450 hPa×m have been used for the lower and higher energy spectral regions, respectively. Absolute line intensities have been measured in the 2001i−00001, 3001i−00001 (i=1, 2, 3) and 00031−00001 bands. An excellent agreement was achieved for the line intensities of the 3001i−00001 (i=1, 2, 3) bands measured by both FTS and CW-CRDS. The CW-CRDS and FTS experimental intensity data together with selected intensity information from the literature have been fitted simultaneously using the effective operators approach. Two sets of effective dipole moment parameters have thus been obtained, which reproduce the observed line intensities in the 2.0 and 1.6 μm regions within experimental uncertainties.  相似文献   

12.
Over 8000 line positions and intensities of phosphine (PH3) at 3 μm have been measured at 0.0115 cm−1 resolution with the McMath-Pierce Fourier Transform spectrometer at Kitt Peak. The observed line intensities ranged from 4.13 × 10−6 to 4.69 × 10−2 cm−2 atm−1 at 296 K, for line positions between 2724.477 and 3601.652 cm−1. This region spans eight interacting vibrational states: 3ν2 (2940.8 cm−1), 2ν2 + ν4 (3085.6 cm−1), ν2 + 2ν4 (3214.9 cm−1), ν1 + ν2 (3307.6 cm−1), ν2 + ν3 (3310.5 cm−1), 3ν4 (∼3345 cm−1), ν1 + ν4 (3426.9 cm−1), and ν3 + ν4 (3432.9 cm−1). Assignments have been determined for all the bands except 3ν4 (a weak band in a highly congested area) for a total of 4232 transitions. The total integrated intensity for this region is 5.70 cm−2 atm−1 near 296 K, and assigned lines account for 79% of the observed absorption. The two strongest bands in the region are ν1 + ν4 and ν3 + ν4 with band strengths at 296 K of 1.61 and 2.01 cm−2 atm−1, respectively. An empirical database of PH3 line parameters (positions, intensities, and assignments) is now available. Lower state energies (corresponding to assignments from this study) and line widths from the literature are included; default values are used for unassigned features.  相似文献   

13.
The spectroscopic knowledge of sulfur hexafluoride, which is necessary for a correct remote sensing and monitoring of this species in the Earth’s atmosphere, is still very partial. In particular, the hot bands in the strongly absorbing ν3 region (near 948 cm−1) have not been analyzed yet. Their study implies the analysis of many vibrational levels and thus the spectroscopy of various fundamental, harmonic, and combination bands. The present work is a new contribution to this topic, concerning the ν2+ν4 combination band. The FTIR spectrum of this region has been recorded at room temperature with a resolution of 0.002 cm −1. The data have been analyzed thanks to the HTDS software (http://www.u-bourgogne.fr/LPUB/shTDS.html) developed in Dijon for XY6 octahedral molecules. Seven hundred and fifty-nine lines could be assigned up to J=112, and the standard deviation is 0.0022 cm−1. The distance between the two vibrational sublevels with respective symmetry F1u and F2u is 0.348 cm−1.  相似文献   

14.
The 10 μm region of thioformaldehyde (H2CS) has been recorded at high resolution (0.005 cm−1) using a Fourier transform spectrometer. H2CS was produced by low-pressure pyrolysis of a gas flow of C3H5SCH3 in Ar at 560 °C or CH3SCl at 1150 °C, which was introduced into a multipass White cell with an optical path length of 32 m. Forty scans were recorded for the range 750-1400 cm−1 at a total pressure of 0.15 mbar. A thorough analysis of the three lowest wavenumber fundamental bands, ν3, ν4 and ν6, which fall in this region, has been carried out using a Hamiltonian model, which takes explicitly into account the numerous resonances affecting the ro-vibrational energy levels; especially the massive A-type Coriolis resonance between the out-of-plane wagging mode, ν4, and the in-plane rocking mode, ν6. These two modes are only separated by 0.83 cm−1, and they are thoroughly mixed. From the fittings, the following band centers were derived: νo (ν4)=990.18213(40) cm−1, νo (ν6)=991.02021(50) cm−1 and νo (ν3)=1059.20476 (30) cm−1 where the uncertainties are one standard deviation. In addition, a number of relative line intensities were measured permitting the determination of relative values of the first-order transition moments and therefore relative band intensities for all three bands. Finally, a comprehensive list of line wavenumbers and relative intensities has been generated.  相似文献   

15.
The Fourier transform gas-phase IR spectrum of 1,3,4-thiadiazole, C2H2N2S, has been recorded with a resolution of ca. 0.003 cm−1 in the 800-1500 cm−1 spectral region. Five fundamental bands ν2(A1; 1391.9 cm−1), ν4(A1; 964.4 cm−1), ν5(A1; 894.6 cm−1), ν9(B1; 821.5 cm−1), and ν14(B2; 898.4 cm−1) have been analysed using the Watson model. Ground state rotational and quartic centrifugal distortion constants as well as upper state spectroscopic constants have been obtained from fits. The ν4 and ν9 bands are unperturbed while a strong c-Coriolis resonance perturbs the close-lying ν5 and ν14 bands. This dyad system has been analysed by a model including first and second order c-Coriolis resonance using the theoretically predicted Coriolis coupling constant . The ν2 band is strongly perturbed by a local resonance, and we obtain a set of spectroscopic parameters using a model including second order a-Coriolis resonance with the inactive ν10 + ν14 band. Ground state rotational and quartic centrifugal distortion constants, anharmonic frequencies, and vibration-rotational α-constants predicted by quantum chemical calculations using a cc-pVTZ basis and B3LYP methodology, have been compared with the present experimental data, where there is generally good agreement.  相似文献   

16.
The 2,3-13C2 isotopomer of butadiene was synthesized, and its fundamental vibrational fundamentals were assigned from a study of its infrared and Raman spectra aided with quantum chemical predictions of frequencies, intensities, and Raman depolarization ratios. For two C-type bands in the high-resolution (0.002 cm−1) infrared spectrum, the rotational structure was analyzed. These bands are for ν11 (au) at 907.17 cm−1 and for ν12 (au) at 523.37 cm−1. Ground state and upper state rotational constants were fitted to Watson-type Hamiltonians with a full quartic set of centrifugal distortion constants and two sextic ones. For the ground state, A0 = 1.3545088(7) cm−1, B0 = 0.1469404(1) cm−1, and C0 = 0.1325838(2)  cm−1. The small inertial defects of butadiene and two 13C2 isotopomers, as well as for five deuterium isotopomers as previously reported, confirm the planarity of the s-trans rotamer of butadiene.  相似文献   

17.
The far infrared and infrared spectra of formamide (HCONH2) have been recorded at high resolution (0.00125 cm−1) in the region of 90-1060 cm−1. Over 20,000 transitions from the out-of-plane NH2 wagging motion (n12 = 1 ← 0 fundamental, n12 = 2 ← 0 overtone, n12 = 2 ← 1 difference bands), torsion (n11 = 1 ← 0 bands), and out-of-phase NCO/NH2 bend (n9 = 1 ← 0 bands) have been assigned. Molecular parameters have been obtained for the ground state and the unperturbed n12 = 1 state. The least-squares fit calculations were completed with the microwave data available in the literature. The complicated resonance system between the n12 = 2, n11 = 1, and n9 = 1 states has been investigated carefully. Thus, we have been able to verify almost all resonances (avoided crossing) existing in the region J, K investigated. In the coupled Hamiltonian used for the fit, all Watson’s reduced parameters, including the octic ones and 16 Coriolis coupling parameters were taken into account. The rms deviation obtained from the fit was 0.000247 cm−1.  相似文献   

18.
The main aim of the work is to transfer the high accuracy of the CO2 laser bands around 10 μm to far infrared regions around 400 and 250 cm−1 for secondary standards. The bands ν1 + ν2 and 3ν2 of CS2 were measured on the Bruker IFS 120 HR Fourier spectrometer in Oulu with special care and calibrated against CO2. In the second stage the ν2 region around 400 cm−1 was measured at a resolution of 0.001 cm−1. This spectrum was calibrated against 3ν2 internally with the CS2 band system using ladders formed with rotational lines in the bands ν2, 2ν2 − ν2 and 3ν2 − 2ν2. Further, the difference band ν1 − ν2 at 263 cm−1 together with accompanying hot bands was measured on a similar spectrometer in Lund, Sweden, but with a synchrotron radiation source. Using corresponding chains of lines as above this region was calibrated with ν1 + ν2. In this way, problems with conventional calibration could be avoided. Without the effect of the pressure shifts the absolute accuracy of 2.0 × 10−6 and 8.4 × 10−6 cm−1 has been achieved at 400 and 250 cm−1, respectively. Simultaneously the same calibration accuracy is also transferred to residual water lines around the CS2 far infrared bands and the best H2O lines will be given with literature comparisons. In addition to the calibration new results from the observed hot bands of CS2 in the region of the bands ν1 + ν2 and 3ν2 will be given.  相似文献   

19.
High-resolution spectra of VO have been reinvestigated in the 12 000-31 000 cm−1 region. VO was produced in a vanadium hollow cathode lamp by discharging 1.5 Torr of Ar and the spectra were recorded using a Fourier transform spectrometer. The oxygen needed to produce VO was present in the system as an impurity. Three new bands observed in the 21 000-22 100 cm−1 region have been attributed to a new 2Δ-12Δ electronic transition of VO. Two bands, with origins near 21 044 and 22 038 cm−1, have been assigned as the 0-1 and 0-0 bands of the 2Δ3/2-12Δ3/2 sub-band while a weak band with an origin near 21 975 cm−1 has been assigned as the 0-0 band of the corresponding 2Δ5/2-12Δ5/2 sub-band. A rotational analysis of these sub-bands has been obtained and spectroscopic constants have been extracted. The 12Δ state is known from the previous analyses of the doublet transitions of VO in the near infrared. The present observation has allowed the determination of the vibrational interval ΔG1/2 and the equilibrium rotational constants for the 12Δ3/2 state.  相似文献   

20.
The infrared spectrum of propynal, C2HCHO, is studied at high resolution (0.003 cm−1) in the range 570-640 cm−1. The relatively intense ν11 (CC-H out-of-plane bend, 693 cm−1) and ν7 (CC-H in-plane bend, 651 cm−1) fundamental bands are linked by a strong a-type Coriolis interaction. The somewhat weaker ν8 (CCO in-plane bend, 614 cm−1) fundamental has a significant Fermi-type interaction with the “dark” background state 3ν9 (∼618 cm−1). About 1400 lines are assigned and analyzed in terms of a four-state fit in order to obtain accurate band origins, rotational and centrifugal distortion parameters, and Fermi and Coriolis interaction parameters. This represents the first systematic high-resolution infrared study of propynal.  相似文献   

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