1887
banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Spectroscopy and femtosecond dynamics of the ring opening reaction of 1,3-cyclohexadiene
Rent:
Rent this article for
USD
10.1063/1.2345203
/content/aip/journal/jcp/125/13/10.1063/1.2345203
http://aip.metastore.ingenta.com/content/aip/journal/jcp/125/13/10.1063/1.2345203
View: Figures

Figures

Image of Scheme 1.
Scheme 1.
Image of FIG. 1.
FIG. 1.

Resonance enhanced ionization scheme involving the potential energy surfaces of the 1,3-cyclohexadiene/1,3,5-hexatriene system. In the one-color two-photon ionization scheme, a laser pulse with photon energy populates first the state and then the ground state of the ion. Rapid energy transfer occurs from the state to the state upon excitation, of which the early parts bear signature in the photoelectron spectrum. In the two-color three-photon ionization scheme, a second photon of energy brings the molecules to a valence state, from which the Rydberg states are populated by internal conversion. A third laser photon ionizes the molecules.

Image of FIG. 2.
FIG. 2.

The time-of-flight mass spectrum obtained upon resonance enhanced one-color two-photon ionization of CHD with femtosecond laser pulses at .

Image of FIG. 3.
FIG. 3.

One-color two-photon ionization-photoelectron spectra obtained from ionization via the transient state, for laser wavelengths between 275 and , as indicated.

Image of FIG. 4.
FIG. 4.

A comparison of the photoelectron spectrum (upper trace, dashed) with the Rydberg absorption spectrum (lower trace, solid line) obtained by Merchán et al. (Ref. 46) illustrating the similarity of the spectra. The photoelectron spectrum, taken at , is plotted against the scale at the top of the graph, while the absorption spectrum is plotted against the scale at the bottom. The absorption spectrum was digitized and reproduced with permission from Merchán et al. (Ref. 46).

Image of FIG. 5.
FIG. 5.

(a) Peak widths vs laser wavelengths, resulting from the deconvolution of the photoelectron spectra. Plotted is the full width at half maximum of the Gaussian fits. (b) Peak intensities vs laser wavelengths.

Image of FIG. 6.
FIG. 6.

The Rydberg spectrum of 1,3-cyclohexadiene obtained by exciting through the valence levels using a two-color three-photon ionization process and a one-color four-photon ionization process. The observed peaks are assigned by their principal quantum numbers and quantum defects. For the one-color spectrum the laser wavelength was , while for the two-color spectrum the laser wavelengths were 400 and .

Image of FIG. 7.
FIG. 7.

The time-resolved decay dynamics of 1,3-CHD (solid dots) obtained by delaying the photon with respect to the photon. The instrument function, which was obtained using azulene, is plotted as hollow circles. The fits for the temporal profile of the CHD signal were obtained with a rise time of and a decay time of . The inset shows the logarithmic plot of the decay curve and the exponential fit for the latter part of the time delay.

Loading

Article metrics loading...

/content/aip/journal/jcp/125/13/10.1063/1.2345203
2006-10-02
2014-04-21
Loading

Full text loading...

This is a required field
Please enter a valid email address
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Spectroscopy and femtosecond dynamics of the ring opening reaction of 1,3-cyclohexadiene
http://aip.metastore.ingenta.com/content/aip/journal/jcp/125/13/10.1063/1.2345203
10.1063/1.2345203
SEARCH_EXPAND_ITEM