We have investigated processes of ionization, energy absorption and subsequent explosion of atomic and molecular clusters under intense laser illumination using numerical as well as analytical methods. In particular, we focused on the response of composite clusters, those consisting of different atomic elements, to intense light pulses. Another major theme is the effect of the molecular structure of clusters on their Coulomb explosion. The action of intense laser pulses on clusters leads to fundamental, irreversible changes: they turn almost instantaneously into nanoplasmas and subsequently disintegrate into separate ions and electrons. Due to this radical transformation, remarkable new features arise. Transient cluster nanoplasmas are capable of absorbing enormous amounts of laser energy. In some cases more than 90 % of incident laser energy is absorbed by a gas of clusters with a density much smaller than that of a solid. After the efficient absorption, the energy is transformed into production of energetic ions, electrons, photons, and even neutrons. Composite clusters show especially interesting behavior when they interact with intense laser pulses. Nanoplasmas formed in composite clusters may absorb even more laser energy, than those formed in homogeneous clusters, as we demonstrate in this work. One of the most important results of this thesis is the identification of a novel type of plasma resonance. This resonance is enabled by an unusual ellipsoidal shape of the nanoplasma created during the ionization process in a helium droplet doped with just a few xenon atoms. In contrast to the conventional plasma resonance, which requires significant ion motion, here, the resonant energy absorption occurs at a remarkably fast rate, within a few laser cycles. Therefore, this resonance is not only the most efficient (like the conventional resonance), but also, perhaps, the fastest way to transfer laser energy to clusters. Recently, dedicated experimental studies of this effect were performed at the Max Planck Institute in Heidelberg. Their preliminary results confirm our prediction of a strong, avalanche-like ionization of the helium droplet with a small xenon cluster inside. A conventional plasma resonance, which relies on the cluster explosion, also exhibits interesting new properties when it occurs in a composite xenon-helium cluster with a core-shell geometry. We have revealed an intriguing double plasma resonance in this system. This was the first theoretical study of the influence of the helium embedding on the laser- driven nanoplasma dynamics. Our results demonstrate the important role of the interaction between xenon and helium parts of the cluster. Understanding this interaction is necessary in order to correctly interpret the experimental results. We have elucidated several important properties of Coulomb explosion in atomic and molecular clusters. Specifically, it was found that the kinetic energy distribution of ions after the Coulomb explosion of an atomic cluster is quite similar to the initial potential energy distribution of ions and is only weakly influenced by ion overtake effects, as was believed before. For the case of molecular hydrogen clusters, we have shown that the alignment of molecules inside the cluster affects its Coulomb explosion. Investigation of the dynamical processes in composite and molecular clusters induced by intense laser pulses is a step towards understanding them in more complex nano-objects, such as biomolecules or viruses. This is of great interest in the context of x-ray diffractive imaging of biomolecules with atomic resolution, which is one of the main goals of new x-ray free electron laser facilities.

Advances in life science require knowledge of active molecules in complex biological systems. These molecules are often only present for a certain time and at limited concentrations. Integrated micro-analytical tools for sampling, separation and mass spectrometric (MS) detection would meet these requests and are therefore continuously gaining interest. An on-line coupling of analytical functions provides shorter analysis time and less manual sample handling. In this thesis, improved compatibility of microdialysis sampling and multidimensional separations coupled to MS detection are developed and discussed. Microdialysis was used in vitro for determination of the non-protein bound fraction of the drug ropivacaine. The sampling unit was coupled on-line to capillary column liquid chromatography (LC) followed by ultraviolet or MS detection. For MS detection, the system was extended with a desalting step and an addition of internal standard. A method for MS screening of microdialysates, collected in vivo, was also developed. The method involved sampling and measurements of the chemical pattern of molecules that generally are ignored in clinical investigations. Chemometric tools were used to extract the relevant information and to compare samples from stimulated and control tissues. Complex samples often require separation in more than one dimension. On-line interfaces for sample transfer between LC and capillary electrophoresis (CE) were developed in soft poly(dimethylsiloxane) (PDMS). MS detection in the LC-CE system was optimised on frequent sampling of the CE peak or on high resolution in mass spectra using time-of-flight (TOF)MS or Fourier transform ion cyclotron resonance (FTICR)MS, respectively. Aspects on electrode positioning in the LC-CE interface led to development of an on-column CE electrode. A successful method for deactivation of the PDMS surface using a polyamine polymer was also developed. The systems were evaluated using peptides and proteins, molecules that are gaining increased attention in bioscience, and consequently also in chemical analysis.

La spectroscopie d’émission est un outil puissant pour obtenir des informations sur lesprocessus microscopiques dans un plasma de décharge hors-équilibre (décharge couronne)dans des milieux denses tels que le gaz supercritique à haute pression et les liquides. Lesobservations spectroscopiques de la lumière émise à partir d'une zone d'ionisation créée parune décharge entre une pointe fine et un plan sont utilisées pour caractériser l'environnementlocal des atomes ou des molécules émettrices. Les caractéristiques spectrales observablesétant sensibles à l'environnement immédiat de l'espèce émettrice, rend la spectroscopieoptique très utile pour l'étude du plasma hors-équilibre en fonction des paramètres du milieu(pression et température).Dans ce travail, nous avons étudié les caractéristiques courant-tension et lacomposition spectrale d’un cryoplasma initié par une décharge couronne dans l'hélium liquideet gazeux à des températures cryogéniques. Ces expériences ont été effectuées pour un certainnombre de températures fixes de 300 K à 4,2 K dans une plage de pression de 0,1 à 10 MPa.Ces conditions couvrent une large région des états thermodynamiques de la matière avec unedensité d'environ 1019 cm-3 pour le gaz à une densité de 2*1022 cm-3 pour le liquide. / Fluorescence spectroscopy is a powerful tool to obtain information on microscopicprocesses in non-equilibrium discharge plasma (corona) in dense media such as high pressuresupercritical gas and even liquids. Spectroscopic observations of the light emitted from anionization zone near a tip electrode can be used to determine structural information of thelocal environment of the emitting atoms or molecules. The spectral features observable aresensitive to the immediate surroundings of the emitting species, which makes emissionspectroscopy very useful for study of the cold nonequilibrium plasma varying the pressureand the temperature.In this work, we have studied the current-voltage characteristics and spectralcomposition of helium cryoplasma initiated with a corona discharge in gaseous and liquidhelium. A cryoplasma has been realized in laboratory conditions using corona discharge ingaseous and liquid Helium at cryogenic temperatures of the matter. Experiments were carriedout at a number of fixed temperatures from 300 K down to 4.2 K within the pressure range0.1÷10 MPa. The conditions covered a wide region of thermodynamic states of the mattersuch as from a gas with density of ~1019 cm-3 up to liquid Helium with density of 2*1022cm-3.

Les BTEX est une famille de polluants très répandue en air intérieur. Ils présentent des effets nocifs sur la santé humaine à des faibles concentrations ce qui a emmené le législateur à fixer des seuils afin de limiter l'exposition des gens. L'objectif de ce travail de recherche est de développer et de mettre en place une méthode analytique sensible, précise et rapide basée sur un dispositif de mesure. Le dispositif ainsi mis en place est un chromatographe en phase gazeuse miniaturisé équipé d'un mini détecteur à photo ionisation dédié à la détection des BTEX en temps quasi-réel. Le système analytique est très portable ayant une consommation gazeuse très faible assurant une autonomie élevée sur de longues durées. Son mode de fonctionnement se base sur l'échantillonnage de l'air dans une boucle connecté à une vanne six voies. L'injection de l'échantillon sur une colonne analytique placée dans un four pour la séparation est assurée par le changement de la position de la vanne avant la détection par photo ionisation. Le nouveau dispositif miniaturisé a été déployé lors de deux campagnes intensives menées dans un collège énergétiquement performant. Cette étude a porté sur la surveillance temporelle de la concentration des polluants présents en air intérieur, y compris les BTEX. Les résultats ainsi obtenus pour les BTEX avec notre dispositif ont été comparés à ceux fournis par d'autres techniques dites techniques de référence. Ces campagnes de terrain ont permis donc de valider les performances analytiques, la robustesse et l'autonomie de cette nouvelle méthodologie. / BTEX are very widespread indoor air pollutants. Their harmful effects on human health had led the legislator to set thresholds in order to limit the population exposure. The aim of this thesis is to develop a sensitive, accurate and fast analytical method based on a measurement device. Therefore, the device implemented is a miniaturized gas chromatography (GC) equipped with a mini photo ionization detector dedicated to BTEX detection in indoor air in near-real time. The miniaturized GC is very portable with a very low gas consumption which enhances its autonomy over a long period. Its operation mode is based on air sampling inside a sample loop which is connected to a six port valve. The injection over a heated analytical column is ensured by switching the valve position before detection by a photo ionization detector. This novel device was used in real conditions during two field campaigns conducted in an energy efficient college. This study focused on the temporal monitoring of indoor air pollutant concentrations including BTEX. The results obtained with our miniaturized device for BTEX were compared to those given by other techniques known as reference techniques. These field campaigns have therefore enabled us to validate the analytical performances, the robustness and the autonomy of this novel analytical method.

La microfabrication 3D par laser dans les matériaux à faible bande interdite néces- sitera l’utilisation d’impulsions intenses dans l’infrarouge proche et moyen. Cette étude expérimentale se concentre sur les spécificités de la physique d’ionisation nonlinéaire dans la gamme de longueur d’onde de 1300-2200nm. Contrairement aux semiconducteurs, l’ab- sorption nonlinéaire mesurée dans les diélectriques est indépendante de la longueur d’onde révélant ainsi l’importance accrue de l’ionisation par effet tunnel avec ces longueurs d’onde. Nous étudions également les rendements et les seuils d’ionisation multiphotonique et ava- lanche dans le silicium intrinsèque et dopé N. Les résultats couplés à l’observation des ma- tériaux irradiés montrent que les propriétés intrinsèques des semiconducteurs empêchent un dépôt d’énergie suffisamment confiné pour viser directement des applications de modifica- tion locale. Ce travail illustre les possibilités de micro-usinage laser 3D dans les diélectriques et les défis de l’extension de cette technique aux semiconducteurs. / 3D laser microfabrication inside narrow gap solids like silicon will require the use of long wavelength intense pulses. This experimental study concentrates on the specificity of the nonlinear ionization physics with tightly focused femtosecond laser beams over a wa- velength range of 1300-2200nm. The measured nonlinear absorption is independent of the wavelength in dielectrics revealing the increased importance of tunnel ionization with long wavelength. This can open up an alternative to pulse shortening toward ultraprecision op- tical breakdown in dielectrics. Using n-doped silicon, we study the multiphoton-avalanche absorption yields and thresholds inside semiconductors. Also observations of the irradia- ted materials reveal that the intrinsic properties of semiconductors prevent efficient direct energy deposition in the bulk for applications. This work illustrates opportunities for 3D laser micromachining in dielectrics and challenges for its extension to semiconductors.

Laboratory based temperature-dependent kinetics and product yields for alkene ozonolysis and the reaction of CH3O2 with ClO and BrO have been measured via chamber studies and a turbulent flow tube coupled to CIMS (Chemical Ionisation Mass Spectrometry). In order to gain a better understanding of the fate of the products formed during hydrocarbon oxidation and their subsequent impact on the ozone budget (and so the oxidising capacity of the atmosphere) it is imperative to know the rate at which these reactions proceed and to identify their product yields. As tropospheric temperature varies, Arrhenius parameters were determined during the ozonolysis of selected alkenes. The temperature dependent kinetic database was extended and the activation energies for the ozonolysis of selected alkenes were correlated with an existing SAR (Structure Activity Relationship). Given the myriad organic species in the atmosphere, SARs are useful tools for the prediction of rate coefficients. Inclusion of Arrhenius parameters into the SAR allows for prediction over a range of temperatures, improving the conditions reflected in models. Achieving mass balance for alkene ozonolysis has proven to be a difficult challenge considering the numerous pathways of the Criegee Intermediate (CI). The product yield of formic acid – an organic acid with significant atmospheric implications which is under predicted by models – was determined as a function of relative humidity during ethene ozonolysis. This reaction exhibited a strong water dependence which lead to the prediction of the reaction rate of the CI with water which ranges between 1 × 10-12 – 1 × 10-15 cm3 molecule-1 s-1 and will therefore dominate its loss with respect to bimolecular processes in the atmosphere. Peroxy radicals, strongly influence the total oxidising capacity of the troposphere. The reaction of peroxy radicals with halogen oxides is recognised to be responsible for considerable ozone depletion in the atmosphere, exacerbated by reactive halogens (X, XO) taking part in catalytic cycles. Arrhenius parameters were determined for ClO + CH3O2 and BrO + CH3O2. Temperature is an important parameter affecting rate, exemplified here as the reaction involving ClO exhibited a positive temperature dependence whereas for BrO a negative temperature dependence was evident. As a consequence, the impact of ClO + CH3O2 with respect to ozone loss is diminished. Global modelling predicts a reduction in ozone loss by a factor of around 1.5 and implicates regions such as clean marine environments rather than the polar stratosphere. Conversely, a more pronounced temperature dependence for the reaction of BrO with CH3O2 placed particular importance on lower stratospheric chemistry where the modelled CH3O2 oxidation is doubled. The main products for this reaction were identified to be HOBr and CH2O2. The decomposition of CH2O2 could enhance HOx in the lower and middle stratosphere and contribute to a significant source of HOx in the upper troposphere. Bimolecular reaction of CH2O2 with water could also provide a none negligible source HC(O)OH in the upper troposphere. Alkenes and peroxy radicals undergo chemical processing in the atmosphere whilst acting as a source and sink of ozone and thus can impose detrimental effects on the biosphere, climate and air quality of the Earth.

Depuis la fin des années 80 et l'avènement de la femto-chimie nous pouvons sonder la dynamique nucléaire à l’œuvre au cours de réactions chimiques à l'échelle de la femtoseconde. Plus récemment, la production d'impulsions lasers attosecondes isolées permet d'atteindre une résolution temporelle plus grande encore. Par elle, il devient possible de sonder la dynamique d'origine purement électronique induite par photo-excitation, et notamment photo-ionisation. Dans ce contexte, avec le développement des techniques de spectroscopie résolue en temps, il est important de disposer d'approches théoriques fiables aidant à l'appréhension de résultats toujours plus nombreux dans ce domaine. La tâche et néanmoins rendue difficile par le caractère profondément multi-électronique des processus en jeu. Traiter de tels effets précisément requiert une grande puissance de calcul, ce qui a limité les études disponibles aujourd'hui à de petits systèmes. Au cours de cette thèse, j'ai tenté d'expliquer les résultats d'une expérience de type "pompe-sonde" (UVX-IR) sur molécule de Caféine menée par une équipe de collaborateurs à l'Institut lumière matière. J'ai utilisé pour cela une méthode basée sur la théorie de la fonctionnelle de la densité dépendante du temps, la TD-DFTB dont le coût numérique réduit par rapport à cette dernière permet des calculs sur de gros systèmes en temps raisonnable. J'y présente une étude du paysage énergétique de la Caféine ainsi que le résultat de 2 approches distinctes pour simuler l'ionisation de ce composé. La première, l'approximation de l'ionisation soudaine cosiste à retirer "à la main" un électron à l'une des orbitales Kohn-Sham occupées du système neutre et ne tient pas compte du champ laser. La seconde à recours à un potentiel imaginaire (ou CAP - Complex Absorbing Potential) pour simuler la perte d'electrons, et tiens explicitement compte du champ laser / Since the advent of femtochemistry, at the end of 1980's, we are able to probe the nuclear dynamics underlying chemical reactions down to the scale of a femtosecond. More recently, the production of isolated attosecond pulses allows to reach an even bigger temporal resolution. It is now possible to probe the ultrafast electronic dynamics following a photo-excitation. In this context, with the developpement of time-resolved spectroscopy techniques, it is important to have reliable theorectical approaches in order to apprehend the increasing number of results in this field. This task is made difficult by the intrinsic multi-electronic nature processes at play. The precise treatment of such effects requires a considerable computing power, and have thus limited the availables studies to relatively small systems. In this thesis, I tried to explain the outcome of a "pump-probe" (XUV-IR) experiment on Caffeine molecule realized by our collaborators at the Insitut Lumière Matière. To do so, I used a method based on density functional theory, the TD-DFTB, which lower numerical cost with respect to TD-DFT allows calculation on bigger compounds. I present in the document a study of the energetical landscape of Caffeine, and 2 approaches to simulate ionization. The first one, the so called sudden-ionization approximation consist to retrieve "by hand" an electron from the occupied Kohn-Sham orbitals of the neutral system without taking the laser field into account. The other one is based on the introduction of a complex absorbing potential (CAP) to account for electron loss and take explicitely the laser field into account.

Cette thèse porte sur différents aspects des dynamiques ultra-rapides d’atomes et de molécules soumises à des impulsions laser infrarouges courtes et intenses. Nous étudions des processus fortement non linéaires tels que l’ionisation tunnel, la génération d’harmoniques d’ordre élevé ou l’ionisation au-dessus du seuil. Deux approches différentes sont utilisées. D’un côté nous mettons au point des modèles analytiques approchés qui nous permettent de construire des interprétations physiques de ces processus. D’autre part nous appuyons les interprétations données par ces modèles avec les résultats obtenus par des simulations numériques qui résolvent explicitement l’équation de Schrödinger dépendante du temps en dimension réduite. Nous étudions également une méthode numérique basée sur l’interaction de configuration dépendante du temps afin de pouvoir des décrire des systèmes à plusieurs électrons plus gros et plus complexes. / In this thesis we study different aspects of the ultrafast dynamics of atoms and molecules triggered by intense and short infrared laser pulses. Highly non-linear processes like tunnel ionization, high order harmonic generation and above threshold ionization are investigated. Two different and complementary approaches are used. On the one hand we construct approximate analytical models to get physical insight on these processes. On the other hand, these models are supported by the results of accurate numerical simulations that explicitly solve the time dependent Schrödinger equation for simple benchmark models in reduced dimensions. A numerical method based on time dependent configuration interaction is investigated to describe larger and more more complex systems with several electrons

The non-adiabatic quantum molecular dynamics (NA-QMD) method couples self-consistently classical nuclear motion with time-dependent density functional theory (TDDFT) in basis expansion for the electron dynamics. It has become a versatile approach to study the dynamics of atoms, molecules and clusters in a wide range of scenarios. This work presents applications of the NA-QMD method to important benchmark systems and its systematic extension to include quantum effects in the nuclear motion. Regarding the first objective, a complete study of the strong-field ionization and dissociation dynamics of nature’s simplest molecule H2+ is performed. By including all electronic and nuclear degrees of freedom and all reaction channels, molecular rotation is shown to play an important role in the ionization process. In addition, strong orientation effects in the energy deposition process of the Buckminster fullerene C60 in short intense laser pulses are surprisingly found in full dimensional calculations. Their consequences on the subsequent nuclear relaxation dynamics shed new light on available experimental data and future experiments are proposed to confirm the detailed predictions. Regarding the second objective, the NA-QMD formalism is basically extended to take electron-nuclear correlations into account. This extension is achieved by means of a trajectory surface hopping scheme in the adiabatic Kohn-Sham framework. First studied examples from collision physics and photochemistry illustrate the relevance and importance of quantum effects in the nuclear dynamics.

We have investigated processes of ionization, energy absorption and subsequent explosion of atomic and molecular clusters under intense laser illumination using numerical as well as analytical methods. In particular, we focused on the response of composite clusters, those consisting of different atomic elements, to intense light pulses. Another major theme is the effect of the molecular structure of clusters on their Coulomb explosion. The action of intense laser pulses on clusters leads to fundamental, irreversible changes: they turn almost instantaneously into nanoplasmas and subsequently disintegrate into separate ions and electrons. Due to this radical transformation, remarkable new features arise. Transient cluster nanoplasmas are capable of absorbing enormous amounts of laser energy. In some cases more than 90 % of incident laser energy is absorbed by a gas of clusters with a density much smaller than that of a solid. After the efficient absorption, the energy is transformed into production of energetic ions, electrons, photons, and even neutrons. Composite clusters show especially interesting behavior when they interact with intense laser pulses. Nanoplasmas formed in composite clusters may absorb even more laser energy, than those formed in homogeneous clusters, as we demonstrate in this work. One of the most important results of this thesis is the identification of a novel type of plasma resonance. This resonance is enabled by an unusual ellipsoidal shape of the nanoplasma created during the ionization process in a helium droplet doped with just a few xenon atoms. In contrast to the conventional plasma resonance, which requires significant ion motion, here, the resonant energy absorption occurs at a remarkably fast rate, within a few laser cycles. Therefore, this resonance is not only the most efficient (like the conventional resonance), but also, perhaps, the fastest way to transfer laser energy to clusters. Recently, dedicated experimental studies of this effect were performed at the Max Planck Institute in Heidelberg. Their preliminary results confirm our prediction of a strong, avalanche-like ionization of the helium droplet with a small xenon cluster inside. A conventional plasma resonance, which relies on the cluster explosion, also exhibits interesting new properties when it occurs in a composite xenon-helium cluster with a core-shell geometry. We have revealed an intriguing double plasma resonance in this system. This was the first theoretical study of the influence of the helium embedding on the laser- driven nanoplasma dynamics. Our results demonstrate the important role of the interaction between xenon and helium parts of the cluster. Understanding this interaction is necessary in order to correctly interpret the experimental results. We have elucidated several important properties of Coulomb explosion in atomic and molecular clusters. Specifically, it was found that the kinetic energy distribution of ions after the Coulomb explosion of an atomic cluster is quite similar to the initial potential energy distribution of ions and is only weakly influenced by ion overtake effects, as was believed before. For the case of molecular hydrogen clusters, we have shown that the alignment of molecules inside the cluster affects its Coulomb explosion. Investigation of the dynamical processes in composite and molecular clusters induced by intense laser pulses is a step towards understanding them in more complex nano-objects, such as biomolecules or viruses. This is of great interest in the context of x-ray diffractive imaging of biomolecules with atomic resolution, which is one of the main goals of new x-ray free electron laser facilities.:1. Introduction 1 2. Interaction of clusters with intense laser pulses 5 2.1. Cluster formation and structure . . . . . . . . . . . . . . . . . . 5 2.1.1. Cluster formation . . . . . . . . . . . . . . . . . . . . . . 5 2.1.2. Cluster structure . . . . . . . . . . . . . . . . . . . . . . 6 2.1.3. Composite clusters . . . . . . . . . . . . . . . . . . . . . 7 2.2. Matter in intense light fields . . . . . . . . . . . . . . . . . . . . 9 2.2.1. Laser sources . . . . . . . . . . . . . . . . . . . . . . . . 9 2.2.2. Atoms . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10 2.3. Clusters under intense laser pulses . . . . . . . . . . . . . . . . . 11 2.3.1. Three stages of intense laser-cluster interaction . . . . . 12 2.3.2. Pathways of cluster ionization and energy absorption . . 13 2.3.3. Composite clusters in intense laser fields . . . . . . . . . 14 2.4. Scenarios of cluster explosion . . . . . . . . . . . . . . . . . . . 15 2.4.1. Coulomb explosion vs. quasi-neutral expansion . . . . . 15 2.4.2. Anisotropic explosion . . . . . . . . . . . . . . . . . . . . 17 2.5. Comparison between experiment and theory . . . . . . . . . . . 18 3. Theoretical methods for intense laser-cluster interaction 21 3.1. The Hamiltonian . . . . . . . . . . . . . . . . . . . . . . . . . . 21 3.2. Survey of simulation methods . . . . . . . . . . . . . . . . . . . 22 3.2.1. Quantum methods . . . . . . . . . . . . . . . . . . . . . 22 3.2.2. Classical methods . . . . . . . . . . . . . . . . . . . . . . 23 3.3. Our method: classical microscopic molecular dynamics . . . . . 24 3.3.1. Initial configuration . . . . . . . . . . . . . . . . . . . . . 24 3.3.2. Integrating the equations of motion . . . . . . . . . . . . 26 3.3.3. Observables . . . . . . . . . . . . . . . . . . . . . . . . . 28 3.4. The role of quantum effects . . . . . . . . . . . . . . . . . . . . 31 4. Cluster nanoplasma: a statistical approach 33 4.1. Vlasov-Poisson formalism . . . . . . . . . . . . . . . . . . . . . . 33 4.2. Nanoplasma electrons at quasi-equilibrium . . . . . . . . . . . . 34 4.2.1. Self-consistent potential and electron density . . . . . . . 34 4.2.2. Energy distribution of nanoplasma electrons . . . . . . . 36 4.3. Harmonic oscillator model . . . . . . . . . . . . . . . . . . . . . 41 4.3.1. Derivation from kinetic equations . . . . . . . . . . . . . 42 4.3.2. Comparison with the molecular dynamics results . . . . 44 4.4. Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 46 5. Ionization and energy absorption in helium droplets doped with xenon clusters 47 5.1. Local ignition and anisotropic nanoplasma growth . . . . . . . . 48 5.1.1. Cluster size dependence . . . . . . . . . . . . . . . . . . 50 5.1.2. Nanoplasma resonance during its anisotropic growth . . 51 5.1.3. Range of laser frequencies and intensities . . . . . . . . . 55 5.1.4. Plasma resonance for circular polarization . . . . . . . . 56 5.1.5. Summary and future work . . . . . . . . . . . . . . . . . 57 5.2. Electron migration and its influence on the cluster expansion . . 59 5.2.1. Charging dynamics . . . . . . . . . . . . . . . . . . . . . 59 5.2.2. Explosion dynamics . . . . . . . . . . . . . . . . . . . . . 61 5.3. Interplay between nanoplasma expansion and its electronic response 63 5.3.1. Single pulse: time-dependence . . . . . . . . . . . . . . . 64 5.3.2. Two pulses: a pump-probe study . . . . . . . . . . . . . 67 5.4. Conclusions and outlook . . . . . . . . . . . . . . . . . . . . . . 71 6. Coulomb explosions of atomic and molecular clusters 75 6.1. Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 75 6.2. Analytical treatment of the Coulomb explosion . . . . . . . . . . 76 6.2.1. Steplike density profile . . . . . . . . . . . . . . . . . . . 76 6.2.2. Kinetic approach . . . . . . . . . . . . . . . . . . . . . . 79 6.2.3. Gradually decreasing initial density . . . . . . . . . . . . 83 6.3. Coulomb explosions of atomic and molecular hydrogen clusters: a molecular dynamics study . . . . . . . . . . . . . . . . . . . . 84 6.3.1. Kinetic energy distributions of ions (KEDI) . . . . . . . 85 6.3.2. Information loss during the explosion . . . . . . . . . . . 87 6.3.3. Ion overtake processes . . . . . . . . . . . . . . . . . . . 90 6.3.4. Non-radial motion of ions . . . . . . . . . . . . . . . . . 91 6.3.5. Three-body effects in Coulomb explosion . . . . . . . . . 93 6.4. Conclusions and outlook . . . . . . . . . . . . . . . . . . . . . . 96 7. Conclusions and outlook 97 7.1. Physical conclusions . . . . . . . . . . . . . . . . . . . . . . . . 97 7.2. Methodological conclusions . . . . . . . . . . . . . . . . . . . . . 99 7.3. Research perspectives . . . . . . . . . . . . . . . . . . . . . . . . 100 A. Suppression of the cluster barrier 101 B. Structure determination for Xen@Hem clusters 103 C. Calculation of the time-dependent phase shift 107 D. Potential of a uniformly charged spheroid 109 E. On the possibility of molecular alignment inside hydrogen clusters 111 Bibliography