1981
DOI: 10.1088/0022-3700/14/11/016
|View full text |Cite
|
Sign up to set email alerts
|

Multiphoton excitation of vibration-rotation states in the ν3mode of SF6

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

1
16
0

Year Published

1982
1982
2006
2006

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 30 publications
(17 citation statements)
references
References 26 publications
1
16
0
Order By: Relevance
“…In the present work, the laser was tuned to the lines X = 10-40, corresponding to wavenumbers of 1/k = (953-925) cm À1 . The infrared activity of the m 3 band is very high, and overtone pumping is possible for rather moderate IR intensities (0.1-10 MW/cm 2 ) [36,40]. In the present work, we apply transverse single pass excitation of the SF 6 molecules with a continuous wave, line-tunable single mode CO 2 laser (Edinburgh Instruments, model PL 5, line bandwidth 100 MHz) at powers up to 50 W and intensities up to about 400 W/cm 2 .…”
Section: Excitation Of Sf 6 By Lines Of a Co 2 Laser And Data Evaluationmentioning
confidence: 99%
See 1 more Smart Citation
“…In the present work, the laser was tuned to the lines X = 10-40, corresponding to wavenumbers of 1/k = (953-925) cm À1 . The infrared activity of the m 3 band is very high, and overtone pumping is possible for rather moderate IR intensities (0.1-10 MW/cm 2 ) [36,40]. In the present work, we apply transverse single pass excitation of the SF 6 molecules with a continuous wave, line-tunable single mode CO 2 laser (Edinburgh Instruments, model PL 5, line bandwidth 100 MHz) at powers up to 50 W and intensities up to about 400 W/cm 2 .…”
Section: Excitation Of Sf 6 By Lines Of a Co 2 Laser And Data Evaluationmentioning
confidence: 99%
“…In the present work, we apply transverse single pass excitation of the SF 6 molecules with a continuous wave, line-tunable single mode CO 2 laser (Edinburgh Instruments, model PL 5, line bandwidth 100 MHz) at powers up to 50 W and intensities up to about 400 W/cm 2 . At these intensities, power broadening is expected to be essentially negligible [40]. The output of the CO 2 laser is shaped into a nearly parallel beam with about 8 mm diameter by a telescope and traverses a water-cooled ZnSe Brewster plate attenuator (II-VI company) which conserves the laser beam direction and profile.…”
Section: Excitation Of Sf 6 By Lines Of a Co 2 Laser And Data Evaluationmentioning
confidence: 99%
“…The major exception to this rule is the excitation of the v 3 mode of SF e by intense infrared radiation from a pulsed CO 2 laser. For this system, molecular parameters derived from high-resolution spectroscopy [4][5][6][7][8][9] have allowed quantitative calculations to be performed [10][11][12][13][14] and compared with experiments using gas-dynamically cooled SF 6 [15][16][17][18]. The refinement of such calculations and experiments, and their intercomparison, offers the best hope for gaining a full quantitative understanding of the initial stages of multiphoton absorption.…”
Section: Introductionmentioning
confidence: 99%
“…Several classical trajectory calculations have been carried out on the muhiphoton absorption and dissociation process [13][14][15][16][17]. A statistical mechanical theory has also been formulated [18] and several quantum dynamical calculations have been performed [13,15,[19][20][21][22][23][24][25]. A significant recent development has been the .application of Floquet theory [26], by Leasure and Wyatt [19][20][21][22], to the laser-induced multiphoton excitation of the vibrational-rotational levels of diatomic molecules.…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, we consider laser fields of more practical intensities (~GW era-2). Inclusion of rotational levels in laser-molecule calculations is essential [20,24] if a realistic simulation is to be carried out.…”
Section: Introductionmentioning
confidence: 99%