Line positions and intensities of the v1+2v2+v3 and 2v2+2v3 of 16O3
| Parent link: | Journal of Molecular Structureer.— , 1957- Vol. 166, № 2.— 1994.— [P. 365–371] |
|---|---|
| Weitere Verfasser: | , , , |
| Zusammenfassung: | Title screen A study of high-resolution (0.006 cm−1) Fourier transform absorption spectra of 16O3around 3450 cm−1 has been performed, leading to the first analysis of the ν1 + 2ν2 + ν3 and 2ν2 + 2ν3 bands of this molecule. To increase the absorption strength of these very weak bands a White cell with path lengths of up to 36 m and pressures from 40 to 55 Torr was used. The rotational energy levels of the (121) and (022) vibrational states deduced from observed spectra have been satisfactorily reproduced using a Hamiltonian matrix which takes explicitly into account the Coriolis interaction between (121) ↔ (022) and (121) ↔ (220) and Darling-Dennison interaction between (022) ↔ (220). Furthermore about 60 and 20 line intensities, respectively, for the (121) and (022) bands were measured with an accuracy of about 6 and 12%, leading to the determination of the ν1 + 2ν2 + ν3 and 2ν2 + 2ν3 vibrational transition moments. Finally, a complete list of line positions, intensities, and lower state energies for both bands has been generated. Режим доступа: по договору с организацией-держателем ресурса |
| Sprache: | Englisch |
| Veröffentlicht: |
1994
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| Schlagworte: | |
| Online-Zugang: | http://dx.doi.org/10.1006/jmsp.1994.1201 |
| Format: | Elektronisch Buchkapitel |
| KOHA link: | https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=642618 |
MARC
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| 200 | 1 | |a Line positions and intensities of the v1+2v2+v3 and 2v2+2v3 of 16O3 |f S. Bouazza [et al.] | |
| 203 | |a Text |c electronic | ||
| 300 | |a Title screen | ||
| 330 | |a A study of high-resolution (0.006 cm−1) Fourier transform absorption spectra of 16O3around 3450 cm−1 has been performed, leading to the first analysis of the ν1 + 2ν2 + ν3 and 2ν2 + 2ν3 bands of this molecule. To increase the absorption strength of these very weak bands a White cell with path lengths of up to 36 m and pressures from 40 to 55 Torr was used. The rotational energy levels of the (121) and (022) vibrational states deduced from observed spectra have been satisfactorily reproduced using a Hamiltonian matrix which takes explicitly into account the Coriolis interaction between (121) ↔ (022) and (121) ↔ (220) and Darling-Dennison interaction between (022) ↔ (220). Furthermore about 60 and 20 line intensities, respectively, for the (121) and (022) bands were measured with an accuracy of about 6 and 12%, leading to the determination of the ν1 + 2ν2 + ν3 and 2ν2 + 2ν3 vibrational transition moments. Finally, a complete list of line positions, intensities, and lower state energies for both bands has been generated. | ||
| 333 | |a Режим доступа: по договору с организацией-держателем ресурса | ||
| 461 | |t Journal of Molecular Structureer |d 1957- | ||
| 463 | |t Vol. 166, № 2 |v [P. 365–371] |d 1994 | ||
| 610 | 1 | |a электронный ресурс | |
| 610 | 1 | |a труды учёных ТПУ | |
| 701 | 1 | |a Bouazza |b S. | |
| 701 | 1 | |a Barbe |b A. | |
| 701 | 1 | |a Mikhailenko |b S. N. |c physicist |c Associate Professor of Tomsk Polytechnic University, Candidate of physical and mathematical sciences |f 1962- |g Semen Nikolaevich |3 (RuTPU)RU\TPU\pers\34035 | |
| 701 | 1 | |a Plateaux |b J. J. | |
| 801 | 2 | |a RU |b 63413507 |c 20160412 |g RCR | |
| 856 | 4 | |u http://dx.doi.org/10.1006/jmsp.1994.1201 | |
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