Abstract:Measurements of photoelectron-photofragment angular correlation and energy partitioning in the dissociative photodetachment of O 4 2 ͑O 4 2 1 hn ! O 2 1 O 2 1 e 2 ͒ at 532 nm are reported. Using photofragment translational energy and photoelectron spectroscopy in coincidence, vibrationally resolved product translational energy distributions and a pronounced angular correlation between the photoelectron and photofragment recoil directions are observed. These results provide insights into the molecule-fixed phot… Show more
“…As shown by Continetti and co-workers for the case of nanosecond laser photodetachment, correlated photofragment and photoelectron velocities can provide a complete probe of the dissociation process. 113,114 The photofragment recoil measurement defines the energetics of the dissociation process and the alignment of the recoil axis in the laboratory frame, the photoelectron energy provides spectroscopic identification of the products, and the photoelectron angular distribution can be transformed to the recoil frame in order to extract vector correlations such as the photofragment angular momentum polarization. The integration of photoion-photoelectron timing imaging (energy and angular correlation) measurements with femtosecond time-resolved spectroscopy was demonstrated, using timing imaging detectors, in 1999 by C. C. Hayden and co-workers 115,116 at Sandia National Laboratories.…”
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“…As shown by Continetti and co-workers for the case of nanosecond laser photodetachment, correlated photofragment and photoelectron velocities can provide a complete probe of the dissociation process. 113,114 The photofragment recoil measurement defines the energetics of the dissociation process and the alignment of the recoil axis in the laboratory frame, the photoelectron energy provides spectroscopic identification of the products, and the photoelectron angular distribution can be transformed to the recoil frame in order to extract vector correlations such as the photofragment angular momentum polarization. The integration of photoion-photoelectron timing imaging (energy and angular correlation) measurements with femtosecond time-resolved spectroscopy was demonstrated, using timing imaging detectors, in 1999 by C. C. Hayden and co-workers 115,116 at Sandia National Laboratories.…”
Access and use of this website and the material on it are subject to the Terms and Conditions set forth at
NRC Publications Record / Notice d'Archives des publications de CNRC:http://nparc.cisti-icist.nrc-cnrc.gc.ca/npsi/ctrl?action=rtdoc&an=12338387&lang=en http://nparc.cisti-icist.nrc-cnrc.gc.ca/npsi/ctrl?action=rtdoc&an=12338387&lang=fr READ THESE TERMS AND CONDITIONS CAREFULLY BEFORE USING THIS WEBSITE.http://nparc.cisti-icist.nrc-cnrc.gc.ca/npsi/jsp/nparc_cp.jsp?lang=en Vous avez des questions? Nous pouvons vous aider. Pour communiquer directement avec un auteur, consultez la première page de la revue dans laquelle son article a été publié afin de trouver ses coordonnées. Si vous n'arrivez pas à les repérer, communiquez avec nous à PublicationsArchive-ArchivesPublications@nrc-cnrc.gc.ca.
“…For the case of nanosecond laser photodetachment, correlated photofragment and photoelectron velocities can provide a complete probe of the dissociation process [130,136]. The photofragment recoil measurement defines the energetics of the dissociation process and the alignment of the recoil axis in the LF, the photoelectron energy provides spectroscopic identification of the products and the photoelectron angular distribution can be transformed to the recoil frame in order to make measurements approaching the MF PAD.…”
Section: B Coincidence Techniquesmentioning
confidence: 99%
“…Thus, these detectors allow for full 3D velocity vector measurements, with no restrictions on the symmetry of the distribution or any requirement for image re-construction techniques. Very successful methods for full time-and-position sensitive detection are based upon interpolation (rather than pixellation) using either charge-division (such as "wedge-andstrip") [129] or crossed delay-line anode timing MCP detectors [130]. In the former case, the avalanche charge cloud is divided amongst three conductorsa wedge, a strip and a zigzag.…”
Section: Experimental Techniques a Photoelectron Spectrometersmentioning
“…Our coincidence momentum imaging apparatus is based on a measurement of electron and ion time of flight (TOF) with two multi-hit two-dimensional position sensitive detectors [23][24][25]. Similar apparatus are used by other groups as well [9,26,27]. A supersonic jet of CO 2 in the vertical direction crosses the photon beam in the horizontal direction.…”
We have measured photoelectron angular distributions in the molecular frame (MF-PADs) for O 1s photoemission from CO 2 , using photoelectron-O + -CO + coincidence momentum imaging. Results for the molecular axis at 0, 45 and 90• to the electric vector of the light are reported. The major features of the MF-PADs are fairly well reproduced by calculations employing a relaxed-core Hartree-Fock approach. Weak asymmetric features are seen through a plane perpendicular to the molecular axis and attributed to symmetry lowering by anti-symmetric stretching motion.(Some figures in this article are in colour only in the electronic version) Photoelectron angular distributions in the molecular frame (MF-PADs) have been investigated extensively for K-shell photoemission from the diatomic molecules CO and N 2 [1-9]. The MF-PADs for molecules aligned parallel to the electric vector of the linearly polarized light exhibit rich structure in regions of shape resonances and provide a dynamical window on the underlying partial-wave composition of the photoelectron as it scatters off the anisotropic potential of the ion. It is worth noting that the observed MF-PADs for N 2 display reflection
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