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aktualisiertes pdf - DPG-Tagungen

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MO 9.7 Mo 18:00 HS 332<br />

Dreiteilchen-Fragmentation von H3 und D3 — •Martin Jungen<br />

— Institut für Physikalische Chemie, Universität Basel<br />

Es wurde beobachtet, dass bereits tiefliegende Rydbergzustände von<br />

H3 und D3 nach H + H + H prädissoziieren können, freilich mit sehr geringer<br />

Rate, z.B. der Zustand 3pe ′ : 2 E ′ ab einer innern Energie, die ca.<br />

3 eV über der Dissoziationsgrenze liegt (s. den vorhergehenden Vortrag).<br />

Mit einer quantenchemische Studie der 6 tiefsten Elektronenzustände<br />

von H3 lässt sich ein möglicher Weg dieses Prozesses erkennen. Der 3pe ′<br />

Rydbergzustand m¨sste sich aus seinem D3h Gleichgewicht über oder<br />

durch eine niedrige Barriere zu einer linearen Geometrie verformen; er<br />

bliebe dort in einer lokalen Potentialmulde gefangen bis zu seinem durch<br />

nichtadiabatische Kopplung bewirkten Übergang auf die dissoziative Potentialfläche,<br />

welche in D∞h-Symmetrie zum Dreiteilchenaufbruch führt.<br />

MO 9.8 Mo 18:15 HS 332<br />

Photodissociation studies of state-selected molecular ions by<br />

velocity map ion imaging — •N. Hendrik Nahler, Olivier P.J.<br />

Vieuxmaire, Josephine A. Jones und Michael N.R. Ashfold —<br />

University of Bristol, School of Chemistry, Bristol BS8 1TS, UK<br />

High resolution ion imaging methods have been used to study the photodissociation<br />

of ground state Br + 2 ( 2 Πg) and BrCl + ( 2 Π) cations, with<br />

spin-orbit state specification, monitoring 79 Br + and 35 Cl + fragments as<br />

appropriate. The state-selected molecular ions are prepared by a 2+1<br />

REMPI scheme and than dissociated by absorption of a single photon<br />

from a second tunable dye laser. Image analysis allows precise determination<br />

of the dissociation energies of Br + 2 ( 2 Π3/2,g), Br + 2 ( 2 Π1/2,g), BrCl +<br />

( 2 Π3/2), and BrCl + ( 2 Π1/2) and values for the respective spin-orbit splitting<br />

constants. The values so derived for BrCl + are in excellent accord<br />

with those obtained from complementary photoelectron imagin studies.<br />

Photoexcitation of Br + 2 at wavelengths just above the first dissociation<br />

threshold yields ground state Br + and Br fragments, the recoil anisotropy<br />

of which is found to be sensitively wavelength dependent. Careful measurements<br />

of the angular anisotropy (β-parameter) versus the dissociation<br />

wavelength reveals the presence of high frequency structure, in the region<br />

up to the first excited [Br( 2 P3/2) + Br + ( 3 P1)] dissociation limit; this we<br />

attribute to predissociating vibrational levels in an adiabatic potential<br />

converging to this excited limit. The dissociation channels from BrCl +<br />

show predominantly parallel character. Branching ratios into the various<br />

Br + ( 3 PJ) and Cl ( 2 PJ) channels will be presented and discussed in the<br />

context of the various participating excited state potentials.<br />

MO 9.9 Mo 18:30 HS 332<br />

Dissoziative Photoionisation von Kohlenwasserstoffradikalen —<br />

•Thomas Schüßler 1 , Ingo Fischer 1 , Christian Alcaraz 2 und<br />

Wolfgang Roth 1 — 1 Institut für Physikalische Chemie, Am Hubland,<br />

97074 Würzburg — 2 LURE, Bât. 209, BP 34, Centre Universitaire<br />

Paris-Sud, 91898 Orsay, France<br />

Es werden Ionisierungsenergien und der H- bzw. H2-Verlust verschiedener<br />

kleiner organischer Kohlenwasserstoffsysteme vorgestellt, die mittels<br />

einer Synchrotronstrahlungseinrichtung gemessen wurden.<br />

Im Propargyl-Kation wurde etwa 3.5 eV oberhalb der Ionisierungsenergie<br />

ein H-Verlust beobachtet, nicht jedoch, wie vorhergesagt, der von<br />

H2.<br />

Das Ethyl-Kation verliert ein H2-Molekül 3.5 eV oberhalb seiner Ionisierungsenergie,<br />

was jedoch 1 eV oberhalb der theoretischen Aussagen<br />

liegt.<br />

Das Allyl-Kation verliert H2 etwa 2 eV oberhalb der Ionisierungsschwelle.<br />

MO 10 Femtosekundenspektroskopie: Schwingungsdynamik<br />

Zeit: Montag 16:30–18:00 Raum: HS 315<br />

MO 10.1 Mo 16:30 HS 315<br />

IR versus Raman Spectroscopy: Monitoring Vibrational Cooling<br />

after Electronic Excitation — •Arne Sieg, Tobias Schrader,<br />

Florian Koller, Wolfgang Schreier, Qingrui An, and Peter<br />

Gilch — Sektion Physik, Ludwig-Maximilians-Universität, Oettingenstr.<br />

67, D-80538 München, Germany<br />

Molecules undergoing ultrafast (∼ 100 fs) internal conversion processes<br />

(IC) are very suitable model systems for the examination of the vibrational<br />

dynamics related with chemical reactions. The detection of these<br />

dynamics can be performed by time resolved IR and Raman spectroscopy.<br />

In a combined study on the vibrational cooling of para-nitroaniline (pNA)<br />

both methods are compared. Only Raman spectroscopy gives access to<br />

the excitation of a stretch mode, which is shown to decay in ∼ 3 ps [1]. IR<br />

spectroscopy is better suited to monitor the frequency shift of this resonance.<br />

This shift to lower wavenumbers relaxes with time constants of 1<br />

– 11 ps. It stems from anharmonic coupling to other vibrational modes.<br />

Therefore, this shift is an useful sensor for the population and dynamics<br />

of these low frequency modes. [1] Q. An, P. Gilch, Chem. Phys. Lett. 363<br />

(2002) 397<br />

MO 10.2 Mo 16:45 HS 315<br />

Solvent Effects on theVibrational Relaxation of para-<br />

Nitroaniline — •Wolfgang Schreier, Tobias Schrader, Arne<br />

Sieg, Florian Koller, Wolfgang Zinth, and Peter Gilch<br />

— Sektion Physik, Ludwig-Maximilians-Universität, Oettingenstr. 67,<br />

D-80538 München, Germany<br />

The re-distribution of excess energy released in photo-chemical processes<br />

in solution is crucial for the stabilization of the reaction products.<br />

Since these processes occur on the picosecond time scale their examination<br />

calls for advanced time resolved techniques and suitable model systems.<br />

Para-Nitroaniline (pNA) can serve as such a system. After photoexcitation<br />

pNA rapidly reforms its ground state and thereby releases<br />

25000 cm −1 of excess energy. Its transfer to the solvent surroundings has<br />

been studied in dependence of the solvent nature by optical pump-probe<br />

spectroscopy [1]. This yields a global measure for dynamics of the vibrational<br />

excitation. Here, time-resolved IR experiments on pNA yielding<br />

mode specific informations are presented. The temporal evolution of an<br />

IR line shape is evaluated and discussed in relation to solvent properties.<br />

[1] S.A. Kovalenko et al. J. Chem. Phys. 115 (2001) 3256<br />

56<br />

MO 10.3 Mo 17:00 HS 315<br />

Vibrational multi-level quantum coherences due to anharmonic<br />

couplings in intermolecular hydrogen bonds — •Nils Huse,<br />

Karsten Heyne, Jens Dreyer, Erik T.J Nibbering, and Thomas<br />

Elsässer — Max-Born-Institut für Nichtlineare Optik und Kurzzeitspektroskopie,<br />

Max-Born-Str. 2a, D-12489 Berlin<br />

Femtosecond 3-pulse photon echo studies of acetic acid dimers in solution<br />

reveal multi-level coherences of O-H stretching excitations caused<br />

by the anharmonic coupling between the high-frequency stretching and<br />

low-frequency hydrogen bond motions. We demonstrate for the first time<br />

that such multi-level coherences determine the nonexponential decay of<br />

the macroscopic O-H stretching polarization, whereas spectral diffusion<br />

processes play a minor role as echo peak shift measurements and dynamic<br />

hole burning show [1,2]. The dephasing time of individual vibrational<br />

transitions contributing to the overall polarization is approximately 200<br />

fs, much longer than the apparent rapid polarization decay.<br />

[1] N. Huse, K. Heyne, J. Dreyer, E.T.J. Nibbering, Th. Elsaesser,<br />

Phys. Rev. Lett. (91), 197401 (2003)<br />

[2] K. Heyne, N. Huse, J. Dreyer, E.T.J. Nibbering, Th. Elsaesser,<br />

Chem. Phys. Lett. (369), 591 (2003)<br />

MO 10.4 Mo 17:15 HS 315<br />

Femtosecond Vibrational Spectroscopy based on Stimulated<br />

Raman Scattering — •Stefan Laimgruber und Peter Gilch —<br />

Sektion Physik, Ludwig-Maximilians-Universität, Oettingenstr. 67, D-<br />

80538 München, Germany<br />

The urge to follow structural dynamics of reacting molecules by femtosecond<br />

techniques has led to the extension of vibrational spectroscopy<br />

(IR and Raman) to that time regime. Raman techniques often suffer from<br />

extremely low scattering cross sections. This drawback can be diminished<br />

be reverting to stimulated Raman scattering. In a novel implementation<br />

[1] of this technique, a femtosecond white light pulse and a spectrally<br />

narrow laser pulse are overlapped in the sample. This allows for the acquisition<br />

of complete Raman spectra within very short times (≤ 1 s).<br />

If a third femtosecond laser pulse excites the sample, Raman spectra of<br />

transient species can be recorded. Here, a novel set-up for this Raman<br />

spectroscopy is introduced and first results on model compounds are<br />

presented. Particular emphasis is laid on the amplification of the solute<br />

signal by a resonance enhancement. [1] M. Yoshizawa, and M. Kurosawa,

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