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The dynamics of a chemical reaction is an essential information that must be obtained to obtain a detailed vision of the mechanism of that reaction. The chemical phenomenon studied is photoinduced by a laser. This excitation occurs without geometric change of the reactive system, but the potential gradients in the excited state give the system the necessary impetus for the reaction. Temporal information allows for the exploration of the passage of the reactive system through geometric conformations and electronic configurations that are very distant from those accessible in the Franck-Condon region.

Exciton relaxation in clusters and isolated nanoparticles

We combined time-resolved photoelectron spectroscopy on isolated species with high-level data processing to address a question that generally falls under materials science: the dynamics of electronic relaxation towards the formation of a self-trapped exciton (STE). These excitons are common excited states in ionic crystals, silica, and rare gas matrices. They are associated with a strong local distortion of the matrix. Argon aggregates were taken as a model system. They are initially excited to a Wannier exciton at 14 eV, and their evolution towards the formation of an STE exhibited an unusual type of vibronic relaxation where the electronic excitation of the aggregate decreases linearly over time at a rate of 0.59 eV/ps. The decay was monitored for 3.0 ps, and the formation of STE occurred in about 5.1 ps.

Cluster Isolated Chemical Reactions (CICR)

Studying chemical reactions in an aggregate is an elegant way to investigate the effects of a reaction medium on the dynamics of a chemical reaction. The “Cluster Isolated Chemical Reaction” (CICR) technique is particularly interesting in this field due to its flexibility: this technique allows for the selection of a known number of reactive atoms or molecules and their interaction with a medium, the aggregate, whose structure and temperature are known. The aggregate plays two successive roles: first, it serves to collisionally capture the reactants, and then it mimics the solvent. The motivations for isolating reactions on van der Waals (or helium) aggregates are of several types:

Using the flexibility of the CICR technique to create a study object that is difficult to obtain otherwise, while ensuring spectroscopic information about it.
Determining the exact stoichiometry of a reaction.
Studying how the aggregate disrupts the reaction occurring within it. Two effects exist: i) mechanical by hindering movements, ii) electronic by altering the relative heights of the different potential surfaces involved in the studied chemical reactions, or even modifying the surfaces themselves. The induced dipole/permanent dipole interaction indeed stabilizes the potential surfaces or the regions of potential surfaces corresponding to a charge transfer compared to those for which there is no charge transfer.

Principle of CICR experiments: 1) Aggregates formed by supersonic expansion. Average size: a few thousand monomers. Temperature: 30K for argon aggregates, 0.4K for helium. 2) Reactants are deposited collisionally: the beam of aggregates passes through a cell or jet containing the molecules to be deposited. The deposition of molecules follows a Poisson distribution (on the right). Once the reactants are deposited, they migrate to the surface of the aggregate, collide, and then associate or react. 3) Action of a laser to photoinduce the process to be studied. 4) Analysis of the process by photoionization spectroscopy in a velocity imaging spectrometer.

Attosecond photoionization delays

The time delay of a photoelectron emitted angularly resolved in the molecular reference frame carries the signature of the interaction of the electron ejected from a molecular orbital by the absorption of an XUV photon with the electrostatic potential representing the electronic structure of the molecule. The determination of this observable is generally the objective of complex two-photon (XUV – IR) experiments, temporally resolved on the attosecond scale. We have demonstrated that such photoionization delays can be determined by measuring the molecular emission diagrams of photoelectrons spectrally resolved in the XUV domain using synchrotron radiation (SOLEIL). The reaction illustrating these experimental and theoretical results involves the interference between direct ionization and resonant ionization due to a shape resonance, described by a multichannel Fano model (see figure). The resonant state, responsible for the modulation of the cross-section, increases the ionization delay by retaining the electron before ionization and modifies the emission diagram.

Emission diagrams of photoelectrons as a function of photon energy for the photoionization of the NO molecule along the shape resonance associated with the ionic state NO^+ (state c), for a molecule oriented parallel to the polarization of the XUV radiation. The color represents the value of the photoionization delay (as).

The ionization time delay can also be measured using a time-resolved approach, employing the RABBIT method which involves measuring the time difference taken by an electron escaping from an ion, for different ionization energies. In collaboration with LIDYL, ILM, and LCPMR, and by introducing an angular approach to the measurement, we were able to reconstruct the film of the ionization process in helium.

3D movie of the photoemission of a helium atom following the simultaneous absorption of an extreme ultraviolet (XUV) photon and an infrared (IR) photon. t = 0 is placed at the maximum overlap of the XUV + IR pulses. Each snapshot represents the complex amplitude of the ionization rate (magnitude in polar coordinates, phase given by the color code). At the beginning and end of the interaction, electron emission occurs preferentially in the z direction of the XUV/IR polarization. Remarkably, at the peak of the interaction with light, near time 0, the interference between ionization pathways involving the intermediate states 1s3p and 1s4p strongly affects the symmetry of the emission, which then occurs predominantly perpendicular to the radiation polarization.

Isolated nanoparticle-femtosecond laser interaction

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Ion spectroscopy

The study of photoionization processes in ionic species is essential for the characterization and modeling of many plasmas, whether they are laboratory-based (laser plasmas, tokamaks, etc.) or of astrophysical interest (stars, nebulae, etc.) and planetary (ionospheres). From a fundamental perspective, understanding photon-matter interactions in complex atomic systems poses a real challenge for theoretical models aimed at describing the various competing interactions within the atomic electronic structure. The photoionization process allows, among other things, for tracking the evolution of the relative intensity of electronic correlations in isonuclear series as a function of the variation in the intensity of the central potential.

Experiments on the photoionization of ionic species began in the 1980s using synchrotron radiation provided by the ACO ring and continued at Super ACO, and then on the Pléiades beamline at Soleil, where the current MAIA experimental setup has a permanent installation. Only one setup, located in Germany, competes with it.

Among the numerous results obtained, we can mention the study of the collapse of the 4f orbital in iodine, xenon, or barium depending on the initial charge state of the ion, the study of isonuclear series of ions of astrophysical interest (C, N, O, Fe), or the study of heavy systems whose modeling requires the use of UTA. These studies have extended to more complex systems such as hydrides.

Collaborations:
E.T. Kennedy, J.P. Mosnier  (Dublin College University)
C. Blancard (CEA Bruyères-le-Châtel)
B. Mc Laughlin (Harvard Smithsonian Center for Astrophysics)
T. Gorczyca (Western Michigan University)
S. Cargniato (LCPMR, Paris)

MAIA setup on the PLEIADES beamline at SOLEIL Synchrotron.

Velocity Map Imaging Spectrometers (VMIS)

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Velocity map imaging

Femto and Attosecond XUV pulses

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HHG

Superfluid Helium droplets

MAIA