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1.
《Journal of Molecular Spectroscopy》1987,122(2):365-370
The spectra of the 2ν1 + ν3 and 3ν3 bands of 14N16O2 have been recorded by means of high-resolution Fourier transform spectroscopy and have been extensively analyzed. The (2 0 1) and (0 0 3) rotational levels deduced from the analysis have been reproduced within the experimental uncertainty using a Hamiltonian which takes into account the Coriolis interaction coupling the vibrational states of the diads {(2 2 0), (2 0 1)} and {(0 2 2), (0 0 3)}. Finally, precise sets of vibrational energies, and spin-rotation, rotational, and coupling constants have been derived for these vibrational states. 相似文献
2.
Fundamental spectroscopical parameters of the weak ν1+3ν2
1-ν2
1+ν3 band of CO2 are reported using a high-resolution, direct-absorption spectrometer, based on a distributed feed-back diode laser emitting
at 2 μm. Line intensities and self-broadening coefficients have been measured for the first time with high accuracy, for nine
lines of the R branch, from R(44) up to R(59). Comparison with available data has been made, and a generally good agreement
has been found.
Received: 30 August 1999 / Published online: 24 March 2000 相似文献
3.
《Journal of Molecular Spectroscopy》1987,122(1):130-134
Numerous transitions belonging to the a2ν2 ← sν2 hot bands of 14NH3 and 15NH3 have been identified and assigned in the long-path Fourier transform spectra of ammonia. The data have been processed to obtain effective molecular parameters for the a2ν2 states of 14NH3 and 15NH3. 相似文献
4.
利用拉曼光谱技术测量了CH_3CN和CD_3CN在常温常压下的拉曼光谱,根据微扰理论建立了新的费米共振理论模型,结合同位素替换方法计算了CH_3CN的ν-2~ν_3+ν_4费米共振耦合系数,并且与利用传统Bertran公式计算结果进行了对比。新的费米共振理论模型利用振动能级的跃迁偶极矩实现了费米共振参数的计算,不仅能够计算未发生费米共振时两费米共振双线的初始光谱强度,而且还能够计算两费米共振双线的初始频率。最后,对利用Bertran公式计算获得的结果产生较大误差的原因进行了分析。 相似文献
5.
Analysis of the Vibrational-Rotational Structure of 2ν1, ν1 + ν3, and 2ν3 Bands of the D2Se Molecule
Zhabina E. A. Onopenko G. A. Ulenikov O. N. Burger G. Jerzembeck W. 《Russian Physics Journal》2002,45(5):483-487
The absorption spectrum of the D2Se molecule in the region of 21, 1 + 3, and 23 absorption bands is registered with a high-resolution Fourier spectrometer and is studied theoretically for a Hamiltonian model with allowance for resonant interactions among (200), (101), and (002) vibrational states. 相似文献
6.
7.
《Journal of Molecular Spectroscopy》1987,121(1):150-166
The ν3 and 2ν80 parallel bands of propyne (methyl acetylene) at 2137.88 and 2066.33 cm−1 have been studied at 0.006 cm−1 resolution. Their Fermi resonance and interaction with the ν8 + 2ν9, ν7 + ν9, and ν8 + ν9 + ν10 levels have been investigated. Molecular constants were determined from the assignment of 1150 lines. However, the rms error of 0.0028 cm−1 showed the presence of additional perturbations which cannot be uniquely identified. 相似文献
8.
《Journal of Molecular Spectroscopy》1987,124(1):162-171
The microwave spectrum of silyl acetylene in the 4ν10 state has been investigated from 29 to 79 GHz. After an assignment by graphical methods deduced from approximate analytical formulas, molecular constants have been determined through an analysis by direct diagonalization. Some slight anomalies appear. A comparison is made between the constants of the different nν10 states. 相似文献
9.
V. Zéninari B. Parvitte D. Courtois V.A. Kapitanov Yu.N. Ponomarev 《Applied physics. B, Lasers and optics》2001,72(8):953-959
By using a tunable diode laser spectrometer with one absorption White cell for low pressure and one photoacoustic cell for
high pressure, line shape parameters of the R3 triplet of the 2ν3 band of methane at 1.65 μm were measured. The absorption line was recorded by using the wavelength modulation spectroscopy
technique with first harmonic detection. The broadening and shift coefficients were obtained by fitting the first harmonic
absorption signal while varying the pressure of different perturbing gases: air and noble gases (helium, neon, argon, krypton
and xenon). We present here the results for the R3 triplet. The observed shift and broadening coefficients behaviors are discussed.
Received: 17 November 2000 / Revised version: 19 February 2001 / Published online: 27 April 2001 相似文献
10.
11.
12.
《Journal of Molecular Spectroscopy》1987,124(2):437-442
Infrared measurements have been made on SO2 between 450 and 602 cm−1 with a resolution of 0.005 cm−1. The B-type bands due to the bending mode transitions 010-000 and 020-010 have been assigned and analyzed for the 32S16O2 molecule. A total of 3007 transitions were measured and fit for 32S16O2 with a standard deviation of 0.0004 cm−1. Ro-vibrational constants are given that fit the current measurements and the pure rotational transitions reported in the literature. 相似文献
13.
利用分辨率为0.06cm~(-1)的付里叶变换光谱技术研究了CH_3CN分子的v_1,v_4,v_5,v_7和v_2+v_4五个带。观察到了六百多条谱线,并利用最小二乘方方法对这些线进行了拟合,得到了一些新的分子常数。原有的常数也得到了很大的改进。 相似文献
14.
《Journal of Molecular Spectroscopy》1987,123(1):145-160
An infrared laser sideband spectrometer operating in the CO2 laser region with 8- to 18-GHz sidebands has been used to record 266 transitions in the ν3 band and 84 transitions in the 2ν3 ← ν3 band of 12CH3F. The accuracy of the measured frequencies is estimated to be 1–3 MHz. A millimeter/submillimeter-wave spectrometer has been used to record the spectra of 48 pure rotational transitions in the ground vibrational state and 55 transitions in the v3 = 1 vibrational state with an accuracy of 20–90 kHz. The new measurements have been combined with previous radio frequency and infrared laser results to derive sets of constants for the ground, v3 = 1, and v3 = 2 states for this molecule. Tables of the vibrational dependence of the parameters and of the near coincidences of the ν3 and 2ν3 ← ν3 band transitions with CO2 laser frequencies are given. 相似文献
15.
16.
The ν3 fundamental band (CO stretch) of HDCO at 1724 cm?1 has been studied using both conventional infrared absorption and CO laser Stark spectroscopy. In addition to the excited-state (v3 = 1) rotational constants, improved constants for the ground state of HDCO have been obtained by combining previous microwave data with some infrared combination differences. The following constants were determined:
Constant | Ground state | state | Units |
1724.267 | cm?1 | ||
198 119.75 | 198 210.4 | MHz | |
34 910.646 | 34 676.6 | MHz | |
29 561.488 | 29 331.3 | MHz | |
2.3302 | 2.3486 | D | |
0.195 | 0.190 | D |