Our system is currently under heavy load due to increased usage. We're actively working on upgrades to improve performance. Thank you for your patience.
1991
DOI: 10.1063/1.461617
|View full text |Cite
|
Sign up to set email alerts
|

Laser induced dispersed fluorescence spectra of jet cooled NO2: The complete set of vibrational levels up to 10 000 cm−1 and the onset of the X̃ 2A1–Ã 2B2 vibronic interaction

Abstract: The laser induced dispersed fluorescence spectra (L.I.D.F.S.) of jet cooled NO2 molecules in emission from 11 different vibronic levels located between 22 006 and 23 625 cm−1 was recorded. The corresponding variety of Franck–Condon accesses has allowed the observation of the complete set of the 191 lowest vibrational levels of the X̃ 2A1 ground state, located up to 10 000 cm−1. The vibrational band origins were measured to within typically 0.3 cm−1, assigned (n1, n2, n3), and fitted with a 24 coefficient Dunha… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

16
118
0
1

Year Published

1994
1994
2014
2014

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 170 publications
(135 citation statements)
references
References 31 publications
16
118
0
1
Order By: Relevance
“…Consequently, overtime it became a benchmark system for a variety of spectroscopic and dynamics studies concerning theoretical and experimental aspects of photodissociation, intramolecular vibrational redistribution, nonadiabatic couplings [1,2,3,4,5,6,7,8,9,10,11,12,13]. The numerous nonadiabatic interactions are reflected in a complex photodissociation dynamics.…”
Section: Introductionmentioning
confidence: 99%
“…Consequently, overtime it became a benchmark system for a variety of spectroscopic and dynamics studies concerning theoretical and experimental aspects of photodissociation, intramolecular vibrational redistribution, nonadiabatic couplings [1,2,3,4,5,6,7,8,9,10,11,12,13]. The numerous nonadiabatic interactions are reflected in a complex photodissociation dynamics.…”
Section: Introductionmentioning
confidence: 99%
“…3,4 The photoexcitation of NO 2 via the first excited state is known to be very complex due to a conical intersection coupling the ground and first excited states. The effect of this conical intersection has been extensively studied in the frequency 5,6 and more recently also the time domain. [7][8][9][10] Depending on the typical time scale of the dissociation dynamics, femtosecond pump-probe laser spectroscopy can be used.…”
Section: Introductionmentioning
confidence: 99%
“…[35,36] This has also been shown in theoretical studies of HCOH isomerizations. [37] On the other hand, results when using the two lowest 1 2 A and 1 2 A PESs indicate that the 1 2 A PES might play an important role along with quantum [28] effects at temperatures below 400 K. However, for temperatures above 1000 K the results using only the 1 2 A PES reasonably match with the experimental results, e.g. for 1500 and 2700 K. This can be explained by noting that the well of the electronically excited C-state of NO 2 (C 1 2 A ) is comparatively small and leads to redissociation of NO 2 at high temperatures [11].…”
Section: Thermal Rate Coefficientsmentioning
confidence: 96%
“…Two symmetric minima are observed for the same R 3 Jacobi distance which is measured from the center of mass of O 2 to the N atom. Some features of our ground state PES are summarized in Table 1 and compared to results from previous calculations [13] (using icMRCI+Q/cc-pVQZ with CASSCF(13,10)) and to experiments [28,29,30,31,32] (high-resolution microwave spectroscopy [29] and laser induced fluorescence [31]). Good agreement with previous computations and experiments was found from the methods used in the present work.…”
Section: The Ground State 1 2 a Pesmentioning
confidence: 99%