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1.
The rotational spectra of formaldehyde, H212C16O and its isotopic species H213C16O, H212C18O, and H213C18O have been investigated in the ground vibrational state in the frequency region between 8 and 460 GHz. For most cases in which measurements of the a-type R- and Q-branch transitions already existed the accuracy of the line position has been improved to about 10 kHz. For H212C16O and H213C16O a large number of ΔKa = ±2 transitions were measured with similar accuracy. These new data when combined with all other available data and appropriate weightings lead to a set of ground state parameters which for the first time are compatible with infrared and ultraviolet data. The rotational constants (and 3σ standard deviations) obtained using Watson's A-reduced Hamiltonian are:
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2.
Ricardo Perez Yurii Utkin Jiaxiang Han Robert F. Curl 《Journal of Molecular Spectroscopy》2006,236(2):151-157
Two hot bands in the infrared spectrum of formaldehyde (H2CO) have been identified by means of tunable infrared laser spectroscopy using a jet-cooled sample. One band falls in the region 2760-2800 cm−1; it follows a-type selection rules and it has been assigned as the ν1 + ν4 − ν4 hot band. The other band falls in the region 2800-2860 cm−1; it follows b-type selection rules and it has been assigned as the ν5 + ν4 − ν4 hot band. The observations are restricted to low J and Ka levels. It has consequently been possible to ignore the effects of the extensive Coriolis couplings involving these levels in the analysis of the spectra and to model the rotational structure as that of a simple asymmetric top. Least-squares fits of the data have provided values for the band origins: 2774.2706(11) cm−1 for the ν1 + ν4 − ν4 and 2829.2621(8) cm−1 for the ν5 + ν4 − ν4 band. Term values for the upper vibrational levels involved in the transitions have been determined by use of the previously reported term values for the v4 = 1 level. 相似文献
3.
Weak transitions of the type ΔJ = ± 1, , ΔKc = ± 3 have been observed in H2CO and D2CO by the millimeterwave double resonance method and also by direct absorption with a Stark modulated spectrometer. The addition of these new transitions in a least-squares analysis, in which all previously known microwave and millimeterwave data are also included, results in an improved set of rotational and distortion constants. 相似文献
4.
Lu Kang 《Journal of Molecular Spectroscopy》2004,225(1):66-72
The rotational spectra of cyanophosphine, H2PCN, have been measured between 10 and 42.5 GHz by Fourier transform microwave spectroscopy. The rotational constants, centrifugal distortion constants, the 14N quadrupole coupling constant, and the nuclear spin-rotation coupling constants of 31P have been determined. Density functional ab initio calculations were performed, and the calculated values of the molecular constants are in excellent agreement with our experimentally determined results. The spectra of three isotopomers were measured, H2P12C14N, H2P13C14N, and H2P12C15N. The derived r0 structure is quite comparable to the ab initio predicted H2PCN equilibrium geometry. 相似文献
5.
The a type transitions of the microwave rotational spectra of cyanophosphaacetylene, H2PCCCN, have been investigated in the frequency region between 5 and 26.5 GHz by Fourier transformation microwave (FTMW) spectroscopy. Rotational, centrifugal distortion and 14N nuclear quadrupole coupling constants have been determined. Density functional theory level ab initio calculations were performed to predict the molecular constants, and the predicted values are in good agreement with our experimentally determined results. The 13C and 15N isotopomer transitions were also observed. The derived r0 structure is quite comparable to the calculated H2PCCCN equilibrium geometry. 相似文献
6.
The hyperfine structure in the ground-state rotational spectrum of methanimine was studied in the frequency range of 64-172 GHz by means of the Lamb-dip technique. This allowed to resolve, in some hyperfine components due to the 14N nucleus, doublets separated by only some tenth of kHz. We explain the splittings as due to magnetic interactions of the three protons with their molecular environment. The analysis of the experimental spectrum has been guided by quantum-chemical calculations of the hyperfine parameters. 相似文献
7.
Recent theories by Luryi et al. and by Harris et al. for the energy levels of an isolated pair of ortho-H2 molecules in nearly pure solid para hydrogen are compared. 相似文献
8.
The ν2 (CO stretching) vibration-rotation bands of H2CO and D2CO near 5.8 μm have been studied using the technique of laser Stark spectroscopy. The following vibrational and rotational constants have been determined:
Constant | H2CO | D2CO | Unit | |
1746.011 | 1701.620 | cm?1 | ||
281807.8 ± 6. | 141696.6 ± 7. | MHz | ||
38608.7 ± 5. | 32068.4 ± 7. | MHz | ||
33738.7 ± 3. | 25998.6 ± 10. | MHz | ||
μ″ | 2.328 ± 0.006 | 2.344 ± 0.006 | Debye | |
μ′ | 2.344 ± 0.006 | 2.364 ± 0.005 | Debye |
H212C17O | H213C17O | |||
281 965.0 (30) | 281 987.3 (19) | |||
37 812.287(45) | 36 776.790(25) | |||
33 214.523(31) | 32 412.920(19) |
H212C16O | H213C16O | H212C18O | H213C18O | |
A/MHz | 281 970.572 (24) | 281 993.258(135) | 281 961.94 (39) | 281 985.00 (93) |
B/MHz | 38 836.0456(13) | 37 811.0887(25) | 36 904.1693(66) | 35 859.256(10) |
C/MHz | 34 002.2034(12) | 33 213.9790(25) | 32 511.5311(63) | 31 697.868(10) |
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