Title: The spectroscopy study of focused short-wavelength laser-matter interactions Author: Tomas Burian Department: Department of Surface and Plasma Science Supervisor: Ing. Libor Juha, CSc., Department of Radiation and Chemical Physics, Institute of Physics of the Czech Academy of Sciences, Prague Abstract: This thesis is focused on processes occurring during and immediately after an interaction of intense short-wavelength laser pulses with matter. Extreme states of matter (warm dense matter - WDM and hot dense matter - HDM), induced by EUV/SXR/X-ray lasers of two kinds, i.e., free-electron lasers (FEL) and plasma-based lasers, were investigated by emission spectroscopy over various spectral ranges and mass spectroscopic techniques. Absorption/transmission experiments revealed an effect of saturable absorption of soft X-ray laser radiation in aluminium WDM. Then, an ionisation potential depression (IPD) in dense plasmas was investigated by means of X-ray emission spectroscopy. Results obtained with the X-ray FEL-produced plasma exhibit very good agreement with computer simulations considering the Ecker-Kröll model. Analysis of optical emission spectra (OES) supports the key role played by fast recombination processes in the ablation plume created by focused short-wavelength laser beams on the solid target...

Les impulsions ultra-brèves de rayonnement ultraviolet extrême (UVX) ont un grand champ d’application dans les domaines tels que le diagnostic de plasmas, la spectroscopie ou l’étude de la dynamique ultrarapide dans les atomes et les molécules.Aujourd’hui, il existe trois sources délivrant ce genre d’impulsions. Les harmoniques d’ordre élevé (HHG, en anglais) générés dans les gaz rares ou sur les solides peuvent fournir des impulsions attosecondes. Cependant, leur énergie, le plus souvent de l’ordre du nanojoule, limite les applications. L’amplification des impulsions harmoniques dans les plasmas créés par laser (SXRL, en anglais) a démontré pouvoir fournir des énergies de plusieurs dizaines de microjoules. Des énergies plus élevées peuvent être obtenues avec les lasers à électrons libres (LEL) UVX injectés, mais ce sont des Très Grandes Infrastructures ayant un accès limité.Ces dernières années, des progrès significatifs ont été réalisé avec chacune des ces sources, avec pour objectif la génération d’impulsions plus brèves. Il est devenu nécessaire de développer des nouvelles techniques de métrologie temporelle des impulsions UVX ultra-brèves. De plus, beaucoup d’expériences, comme ceux impliquant des phénomènes non-linéaires, nécessitent de hautes intensités UVX. La focalisation efficace des impulsions de faibles énergies peut significativement augmenter le domaine d’application. De bons fronts d’onde sont nécessaires pour focaliser les impulsions UVX à haute intensité, et les optiques doivent aussi être de bonne qualité et alignées avec précision.Dans cette thèse, les propriétés spatiales des harmoniques d’ordre élevé ont été extensivement étudiées grâce à un senseur de front d’onde UVX. Cet appareil couplé à une source HHG a démontré être utile pour la caractérisation de table et à la longueur d’onde ainsi que pour l’optimisation de systèmes optiques UVX.Le problème de la mise en place de la complète caractérisation temporelle d’impulsions UVX est aussi discuté en détail, et deux nouveaux schémas pour la reconstruction d’impulsions de LEL injectés et de lasers X à plasma sont présentés. Finalement, la première implantation d’un système d’amplification à dérive de fréquence (CPA, en anglais) sur un LEL UVX est présentée et son implantation pour les lasers X à plasmas est aussi discutée. / Ultrashort pulses of extreme-ultraviolet (XUV) radiation have a wide range of applications in fields such as plasma probing, spectroscopy, or the study of ultrafast dynamics in atoms and molecules.Nowadays, there are three main sources of such pulses. High-order harmonic generation (HHG) in rare gases or solid surfaces is able to provide attosecond pulses. However, their limited energy, of the order of nanojoules, limits its number of applications. The amplification of high-harmonic pulses in laser-driven plasmas (SXRL) has been demonstrated to provide energies of tens of microjules. Higher pulse energies can be obtained from seeded XUV free-electron lasers (FELs), large-scale facilities with more limited accessibility.In recent years, significant progress has been made with each of these sources towards the generation of shorter pulses. It is thus necessary to develop new techniques for full temporal metrology of ultrashort XUV pulses. Additionally, many experiments, such as those involving nonlinear phenomena, require high XUV intensities. Efficient focusing of low-energy pulses can significantly increase their range of application. Good wavefronts are required in order to focus XUV pulses to high intensities, and the optics must be of high quality and precisely aligned.In this thesis, the spatial properties of high-harmonic pulses are extensively explored thanks to the use of an XUV Hartmann wavefront sensor. This device is also proven here to be useful for tabletop, at-wavelength characterization and optimization of XUV optical systems with HHG sources.The problem of performing full temporal characterization of XUV pulses is also discussed in detail, and two new schemes for complete pulse reconstruction for seeded XUV FELs and seeded SXRLs are presented. Finally, the first implementation of chirped pulse amplification (CPA) in a seeded XUV FEL is reported, and its implementation in seeded SXRLs is discussed as well.

The newly emerging technology of X-ray free-electron lasers (XFELs) has the potential to revolutionise molecular imaging. XFELs generate very intense X-ray pulses and predictions suggest that they may be used for structure determination to atomic resolution even for single molecules. XFELs produce femtosecond pulses that outrun processes of radiation damage and permit the study of structures at room temperature and of structural dynamics. While the first demonstrations of flash X-ray diffractive imaging (FXI) on biological particles were encouraging, they also revealed technical challenges. In this work we demonstrated how some of these challenges can be overcome. We exemplified, with heterogeneous cell organelles, how tens of thousands of FXI diffraction patterns can be collected, sorted, and analysed in an automatic data processing pipeline. We improved  image resolution and reduced problems with missing data. We validated, described, and deposited the experimental data in the Coherent X-ray Imaging Data Bank. We demonstrated that aerosol injection can be used to collect FXI data at high hit ratios and with low background. We reduced problems with non-volatile sample contaminants by decreasing aerosol droplet sizes from ~1000 nm to ~150 nm. We achieved this by adapting an electrospray aerosoliser to the Uppsala sample injector. Mie scattering imaging was used as a diagnostic tool to measure positions, sizes, and velocities of individual injected particles. XFEL experiments generate large amounts of data at high rates. Preparation, execution, and data analysis of these experiments benefits from specialised software. In this work we present new open-source software tools that facilitates prediction, online-monitoring, display, and pre-processing of XFEL diffraction data. We hope that this work is a valuable contribution in the quest of transitioning FXI from its first experimental demonstration into a technique that fulfills its potentials.

Mass-selected infrared multiple photon spectroscopy (IRMPD), Fourier transform ion cyclotron resonance (FT-ICR) kinetic experiments, RRKM and electronic structure calculations have been performed in order to propose a complex mechanism involving the formation of the proton-bound dimer of water (H5O2+) from 1,1,3,3-tetrafluorodimethyl ether. It has been found that the reaction is facilitated by a series of sequential exothermic bimolecular ion-molecule reactions. Evidence for the dominant mechanistic pathway involving the reaction of CF2H-O=CHF+, an ion of m/z 99, with water is presented. The primary channel occurs via nucleophilic attack of water on the ion of m/z 99 (CF2H-O=CHF+), to lose formyl fluoride and yield protonated difluoromethanol (m/z 69). Association of a second water molecule with protonated difluoromethanol generates a reactive intermediate which decomposes via a 1,4-elimination to release hydrogen fluoride and yield the proton-bound dimer of water and formyl fluoride (m/z 67). The 1,4-elimination of hydrogen fluoride is found to be strongly supported by the results of both RRKM theory and electronic structure calculations. Lastly, the elimination of formyl fluoride occurs by the association of a third water molecule to produce H5O2+ (m/z 37). The most probable isomeric forms of the ions with m/z 99 and 69 were found using IRMPD spectroscopy and electronic structure theory calculations. Thermochemical information for reactant, transition and product species was obtained using MP2/aug-cc-pVQZ//MP2(full)/6-31G(d) level of theory. Ionic hydrogen bond (IHB) interactions, resulting from the association of ammonia and two of the protonated methylxanthine derivatives, caffeine and theophylline, have been characterized using mass-selected IRMPD and electronic structure calculations at the MP2/aug-cc-pVTZ//B3LYP/6-311+G(d,p) level of theory. It was found that the formation of a proton-bound dimer (PBD) of caffeine and ammonia was elusive under the experimental conditions. The low binding energy of the caffeine and ammonia PBD is responsible for the perceived difficulty in obtaining an IRMPD spectrum. The IRMPD spectrum of the PBD of theophylline and ammonia was obtained and revealed bidentate IHB formation within the complex, which greatly increased the binding energy relative to the most stable isomer of the PBD of caffeine and ammonia. The IRMPD spectra of the protonated forms of caffeine and theophylline have also obtained. The spectrum of protonated caffeine showed the dominant existence of a single isomer, whereas the spectrum of protonated theophylline showed a mixture of isomers. The mixture of isomers of protonated theophylline resulted as a consequence of proton-transport catalysis (PTC) occurring within the PBD of theophylline and ammonia. All calculated harmonic spectra have been produced at the B3LYP/6-311+G(d,p) level of theory with fundamental frequencies scaled by 0.9679; calculated anharmonic spectra have also been provided at the same level of theory and were found to greatly improve the match with the IRMPD spectra obtained in all cases. Ionic hydrogen bond (IHB) interactions, resulting from the association of caffeine and theophylline with their protonated counterparts, forming proton-bound homodimers, have been characterized using mass-selected IRMPD and electronic structure calculations at the MP2/6-311+G(2d,2p)//B3LYP/6-311+G(d,p) level of theory. It is found that the IRMPD spectra of the proton-bound homodimers of caffeine and theophylline are complicated resulting from the existence of several pairs of enantiomers separated by a narrow range of relative Gibbs free energies (298 K) of 15.6 and 18.2 kJ mol-1, respectively. The IRMPD spectrum of the proton-bound homodimer of theophylline is dominated by a unique isomer facilitated by formation of a bidentate IHB. Formation of this interaction lowers the relative Gibbs free energy of the ion to 9.75 kJ mol-1 below that of the most favourable pair of enantiomers. The IRMPD spectrum of the PBD of caffeine is complicated by the existence of at least two pairs of enantiomers with the strong likelihood of the spectral contributions of a third pair existing. The most favourable enantiomeric pair involves the formation of a O-H+⋯O IHB. However, verification of a pair of enantiomeric PBDs containing a N-H+⋯O IHB is also observed in the IRMPD spectrum of the PBD of caffeine due to the presence of three free carbonyl stretching modes located at 1731, 1751 and 1785 cm-1. The mass-selected IRMPD spectra of the sodium cation-bound dimers (SCBD) of caffeine and theophylline also have been obtained. Both the mass-selected IRMPD spectra and electronic structure calculations predict the most likely structure of the SCBDs of caffeine and theophylline to form by an efficient O⋯Na+⋯O interaction between C=O functional groups possessed by each monomer. The frequencies of the C=O-Na+ stretch are found to be nearly identical in the IRMPD spectra for both of the SCBDs of caffeine and theophylline at 1644 and 1646 cm-1, respectively. However, the degenerate free C=O symmetric and asymmetric stretches for the SCBDs of caffeine and theophylline found at 1732 and 1758 cm^(-1), respectively, demonstrating a red-shift for caffeine possibly linked to a steric interaction absent in theophylline. Free rotation about the O⋯Na+⋯O bond is found to greatly decrease the complexity of the IRMPD spectra of the SCBDs of caffeine and theophylline and demonstrates excellent agreement between the IRMPD and calculated spectra. Electronic structure calculations have been done at the MP2(full)/aug-cc-pCVTZ/6-311+G(2d,2p)//B3LYP/6-311+G(d,p) level of theory using the aug-cc-pCVTZ basis set for Na+ and all Na+-interacting heterotatoms, and the 6-311+G(2d,2p) basis set for all non-interacting atoms within the SCBDs, in order to provide accurate electronic energies. Currently, installation and implementation of a pulsed electrospray high pressure ion source mated to an existing high pressure mass spectrometer (HPMS) is underway. The new ion source will greatly increase the range of possibilities for the study of ion-molecule reactions in the McMahon laboratory. One of the unique features of the new design is the incorporation of a gas-tight electrospray interface, allowing for more possibilities than only the study of cluster-ion equilibria involving hydration (H2On⋯S+), where S+ is an ion produced by electrospray. Other small prototypical biological molecules such as amines and thiols can be used without concern for the toxicity of these species. Another unique design feature allows electrosprayed ions to associate with neutral solvent species in an electric field free reaction chamber (RC). This ensures that values of equilibrium constants determined are truly representative of ions in states of thermochemical equilibrium. The existing HPMS in the McMahon laboratory is limited to the study of small volatile organic molecules. The new ion source will permit the exploration of systems involving non-volatile species, doubly charged ions and many biologically relevant molecules such as amino acids, peptides, nucleobases and carbohydrates.

Mass-selected infrared multiple photon spectroscopy (IRMPD), Fourier transform ion cyclotron resonance (FT-ICR) kinetic experiments, RRKM and electronic structure calculations have been performed in order to propose a complex mechanism involving the formation of the proton-bound dimer of water (H5O2+) from 1,1,3,3-tetrafluorodimethyl ether. It has been found that the reaction is facilitated by a series of sequential exothermic bimolecular ion-molecule reactions. Evidence for the dominant mechanistic pathway involving the reaction of CF2H-O=CHF+, an ion of m/z 99, with water is presented. The primary channel occurs via nucleophilic attack of water on the ion of m/z 99 (CF2H-O=CHF+), to lose formyl fluoride and yield protonated difluoromethanol (m/z 69). Association of a second water molecule with protonated difluoromethanol generates a reactive intermediate which decomposes via a 1,4-elimination to release hydrogen fluoride and yield the proton-bound dimer of water and formyl fluoride (m/z 67). The 1,4-elimination of hydrogen fluoride is found to be strongly supported by the results of both RRKM theory and electronic structure calculations. Lastly, the elimination of formyl fluoride occurs by the association of a third water molecule to produce H5O2+ (m/z 37). The most probable isomeric forms of the ions with m/z 99 and 69 were found using IRMPD spectroscopy and electronic structure theory calculations. Thermochemical information for reactant, transition and product species was obtained using MP2/aug-cc-pVQZ//MP2(full)/6-31G(d) level of theory. Ionic hydrogen bond (IHB) interactions, resulting from the association of ammonia and two of the protonated methylxanthine derivatives, caffeine and theophylline, have been characterized using mass-selected IRMPD and electronic structure calculations at the MP2/aug-cc-pVTZ//B3LYP/6-311+G(d,p) level of theory. It was found that the formation of a proton-bound dimer (PBD) of caffeine and ammonia was elusive under the experimental conditions. The low binding energy of the caffeine and ammonia PBD is responsible for the perceived difficulty in obtaining an IRMPD spectrum. The IRMPD spectrum of the PBD of theophylline and ammonia was obtained and revealed bidentate IHB formation within the complex, which greatly increased the binding energy relative to the most stable isomer of the PBD of caffeine and ammonia. The IRMPD spectra of the protonated forms of caffeine and theophylline have also obtained. The spectrum of protonated caffeine showed the dominant existence of a single isomer, whereas the spectrum of protonated theophylline showed a mixture of isomers. The mixture of isomers of protonated theophylline resulted as a consequence of proton-transport catalysis (PTC) occurring within the PBD of theophylline and ammonia. All calculated harmonic spectra have been produced at the B3LYP/6-311+G(d,p) level of theory with fundamental frequencies scaled by 0.9679; calculated anharmonic spectra have also been provided at the same level of theory and were found to greatly improve the match with the IRMPD spectra obtained in all cases. Ionic hydrogen bond (IHB) interactions, resulting from the association of caffeine and theophylline with their protonated counterparts, forming proton-bound homodimers, have been characterized using mass-selected IRMPD and electronic structure calculations at the MP2/6-311+G(2d,2p)//B3LYP/6-311+G(d,p) level of theory. It is found that the IRMPD spectra of the proton-bound homodimers of caffeine and theophylline are complicated resulting from the existence of several pairs of enantiomers separated by a narrow range of relative Gibbs free energies (298 K) of 15.6 and 18.2 kJ mol-1, respectively. The IRMPD spectrum of the proton-bound homodimer of theophylline is dominated by a unique isomer facilitated by formation of a bidentate IHB. Formation of this interaction lowers the relative Gibbs free energy of the ion to 9.75 kJ mol-1 below that of the most favourable pair of enantiomers. The IRMPD spectrum of the PBD of caffeine is complicated by the existence of at least two pairs of enantiomers with the strong likelihood of the spectral contributions of a third pair existing. The most favourable enantiomeric pair involves the formation of a O-H+⋯O IHB. However, verification of a pair of enantiomeric PBDs containing a N-H+⋯O IHB is also observed in the IRMPD spectrum of the PBD of caffeine due to the presence of three free carbonyl stretching modes located at 1731, 1751 and 1785 cm-1. The mass-selected IRMPD spectra of the sodium cation-bound dimers (SCBD) of caffeine and theophylline also have been obtained. Both the mass-selected IRMPD spectra and electronic structure calculations predict the most likely structure of the SCBDs of caffeine and theophylline to form by an efficient O⋯Na+⋯O interaction between C=O functional groups possessed by each monomer. The frequencies of the C=O-Na+ stretch are found to be nearly identical in the IRMPD spectra for both of the SCBDs of caffeine and theophylline at 1644 and 1646 cm-1, respectively. However, the degenerate free C=O symmetric and asymmetric stretches for the SCBDs of caffeine and theophylline found at 1732 and 1758 cm^(-1), respectively, demonstrating a red-shift for caffeine possibly linked to a steric interaction absent in theophylline. Free rotation about the O⋯Na+⋯O bond is found to greatly decrease the complexity of the IRMPD spectra of the SCBDs of caffeine and theophylline and demonstrates excellent agreement between the IRMPD and calculated spectra. Electronic structure calculations have been done at the MP2(full)/aug-cc-pCVTZ/6-311+G(2d,2p)//B3LYP/6-311+G(d,p) level of theory using the aug-cc-pCVTZ basis set for Na+ and all Na+-interacting heterotatoms, and the 6-311+G(2d,2p) basis set for all non-interacting atoms within the SCBDs, in order to provide accurate electronic energies. Currently, installation and implementation of a pulsed electrospray high pressure ion source mated to an existing high pressure mass spectrometer (HPMS) is underway. The new ion source will greatly increase the range of possibilities for the study of ion-molecule reactions in the McMahon laboratory. One of the unique features of the new design is the incorporation of a gas-tight electrospray interface, allowing for more possibilities than only the study of cluster-ion equilibria involving hydration (H2On⋯S+), where S+ is an ion produced by electrospray. Other small prototypical biological molecules such as amines and thiols can be used without concern for the toxicity of these species. Another unique design feature allows electrosprayed ions to associate with neutral solvent species in an electric field free reaction chamber (RC). This ensures that values of equilibrium constants determined are truly representative of ions in states of thermochemical equilibrium. The existing HPMS in the McMahon laboratory is limited to the study of small volatile organic molecules. The new ion source will permit the exploration of systems involving non-volatile species, doubly charged ions and many biologically relevant molecules such as amino acids, peptides, nucleobases and carbohydrates.

This thesis investigates the use of high-power lasers for synchrotron radiation sources with high brilliance, from the EUV to the hard X-ray spectral range. Hereby lasers accelerate electrons by laser-wakefield acceleration (LWFA), act as optical undulators, or both. Experimental evidence shows for the first time that LWFA electron bunches are shorter than the driving laser and have a length scale comparable to the plasma wavelength. Furthermore, a first proof of principle experiment demonstrates that LWFA electrons can be exploited to generate undulator radiation. Building upon these experimental findings, as well as extensive numerical simulations of Thomson scattering, the theoretical foundations of a novel interaction geometry for laser-matter interaction are developed. This new method is very general and when tailored towards relativistically moving targets not being limited by the focusability (Rayleigh length) of the laser, while it does not require a waveguide. In a theoretical investigation of Thomson scattering, the optical analogue of undulator radiation, the limits of Thomson sources in scaling towards higher peak brilliances are highlighted. This leads to a novel method for generating brilliant, highly tunable X-ray sources, which is highly energy efficient by circumventing the laser Rayleigh limit through a novel traveling-wave Thomson scattering (TWTS) geometry. This new method suggests increases in X-ray photon yields of 2-3 orders of magnitudes using existing lasers and a way towards efficient, optical undulators to drive a free-electron laser. The results presented here extend far beyond the scope of this work. The possibility to use lasers as particle accelerators, as well as optical undulators, leads to very compact and energy efficient synchrotron sources. The resulting monoenergetic radiation of high brilliance in a range from extreme ultraviolet (EUV) to hard X-ray radiation is of fundamental importance for basic research, medical applications, material and life sciences and is going to significantly contribute to a new generation of radiation sources and free-electron lasers (FELs).

Die vorliegende Arbeit beschäftigt sich in Experiment und Theorie mit Laser-Plasma beschleunigten Elektronen und optischen Undulatoren zur Erzeugung von brillianter Synchrotronstrahlung. Zum ersten Mal wird experimentell nachgewießen, dass laserbeschleunigte Elektronenpulse kürzer als 30 fs sind. Ferner werden solche Elektronenpulse erstmalig in einem Demonstrationsexperiment durch einen magnetischen Undulator als Synchrotronstrahlenquelle genutzt. Aufbauend auf diesen experimentellen Erkenntnissen, sowie umfangreichen numerischen Simulationen zur Thomsonstreuung, werden die theoretischen Grundlagen einer neuartigen Interaktionsgeometrie für Laser-Materie Wechselwirkungen entwickelt. Diese neue, in der Anwendbarkeit sehr allgemeine Methode basiert auf raum-zeitlicher Laserpulsformung durch nichtlineare Winkeldispersion wie diese durch VLS- (varied-line spacing) Gitter erzeugt werden kann und hat den Vorteil nicht durch die Fokussierbarkeit des Lasers (Rayleighlänge) begrenzt zu sein. Zusammen mit laserbeschleunigten Elektronen ermöglicht dieser traveling-wave Thomson scattering (TWTS) benannte Ansatz neuartige, nur auf optischer Technologie basierende Synchrotronstrahlenquellen mit Zentimeter bis Meter langen optische Undulatoren. Die hierbei mit existierenden Lasern erzielbaren Brillianzen übersteigen diese bestehender Thomsonquellen-Designs um 2-3 Größenordnungen. Die hier vorgestellten Ergebnisse weisen weit über die Grenzen der vorliegenden Arbeit hinaus. Die Möglichkeit Laser als Teilchenbeschleuniger und auch optischen Undulator zu verwenden führt zu bauartbedingt sehr kompakten und energieeffizienten Synchrotronstrahlungsquellen. Die hieraus resultierende monochromatische Strahlung hoher Brillianz in einem Wellenlängenbereich von extremen ultraviolett (EUV) zu harten Röntgenstrahlen ist für die Grundlagenforschung, medizinische Anwendungen, Material- und Lebenswissenschaften von fundamentaler Bedeutung und wird maßgeblich zu einer neuen Generation ultrakurzer Strahlungsquellen und freien Elektronenlasern (FELs) beitragen. / This thesis investigates the use of high-power lasers for synchrotron radiation sources with high brilliance, from the EUV to the hard X-ray spectral range. Hereby lasers accelerate electrons by laser-wakefield acceleration (LWFA), act as optical undulators, or both. Experimental evidence shows for the first time that LWFA electron bunches are shorter than the driving laser and have a length scale comparable to the plasma wavelength. Furthermore, a first proof of principle experiment demonstrates that LWFA electrons can be exploited to generate undulator radiation. Building upon these experimental findings, as well as extensive numerical simulations of Thomson scattering, the theoretical foundations of a novel interaction geometry for laser-matter interaction are developed. This new method is very general and when tailored towards relativistically moving targets not being limited by the focusability (Rayleigh length) of the laser, while it does not require a waveguide. In a theoretical investigation of Thomson scattering, the optical analogue of undulator radiation, the limits of Thomson sources in scaling towards higher peak brilliances are highlighted. This leads to a novel method for generating brilliant, highly tunable X-ray sources, which is highly energy efficient by circumventing the laser Rayleigh limit through a novel traveling-wave Thomson scattering (TWTS) geometry. This new method suggests increases in X-ray photon yields of 2-3 orders of magnitudes using existing lasers and a way towards efficient, optical undulators to drive a free-electron laser. The results presented here extend far beyond the scope of this work. The possibility to use lasers as particle accelerators, as well as optical undulators, leads to very compact and energy efficient synchrotron sources. The resulting monoenergetic radiation of high brilliance in a range from extreme ultraviolet (EUV) to hard X-ray radiation is of fundamental importance for basic research, medical applications, material and life sciences and is going to significantly contribute to a new generation of radiation sources and free-electron lasers (FELs).

Investigations of soft matter using ultrashort high intensity pulses have been made possible through the advent of X-ray free-electrons lasers. The last decade has seen the development of a new type of protein crystallography where femtosecond dynamics can be studied, and single particle imaging with atomic resolution is on the horizon. The pulses are so intense that any sample quickly turns into a plasma. This thesis studies the ultrafast transition from soft matter to warm dense matter, and the implications for structural determination of proteins.                    We use non-thermal plasma simulations to predict ultrafast structural and electron dynamics. Changes in atomic form factors due to the electronic state, and displacement as a function of temperature, are used to predict Bragg signal intensity in protein nanocrystals. The damage processes started by the pulse will gate the diffracted signal within the pulse duration, suggesting that long pulses are useful to study protein structure. This illustrates diffraction-before-destruction in crystallography. The effect from a varying temporal photon distribution within a pulse is also investigated. A well-defined initial front determines the quality of the diffracted signal. At lower intensities, the temporal shape of the X-ray pulse will affect the overall signal strength; at high intensities the signal level will be strongly dependent on the resolution. Water is routinely used to deliver biological samples into the X-ray beam. Structural dynamics in water exposed to intense X-rays were investigated with simulations and experiments. Using pulses of different duration, we found that non-thermal heating will affect the water structure on a time scale longer than 25 fs but shorter than 75 fs. Modeling suggests that a loss of long-range coordination of the solvation shells accounts for the observed decrease in scattering signal. The feasibility of using X-ray emission from plasma as an indicator for hits in serial diffraction experiments is studied. Specific line emission from sulfur at high X-ray energies is suitable for distinguishing spectral features from proteins, compared to emission from delivery liquids. We find that plasma emission continues long after the femtosecond pulse has ended, suggesting that spectrum-during-destruction could reveal information complementary to diffraction.

This thesis investigates the use of high-power lasers for synchrotron radiation sources with high brilliance, from the EUV to the hard X-ray spectral range. Hereby lasers accelerate electrons by laser-wakefield acceleration (LWFA), act as optical undulators, or both. Experimental evidence shows for the first time that LWFA electron bunches are shorter than the driving laser and have a length scale comparable to the plasma wavelength. Furthermore, a first proof of principle experiment demonstrates that LWFA electrons can be exploited to generate undulator radiation. Building upon these experimental findings, as well as extensive numerical simulations of Thomson scattering, the theoretical foundations of a novel interaction geometry for laser-matter interaction are developed. This new method is very general and when tailored towards relativistically moving targets not being limited by the focusability (Rayleigh length) of the laser, while it does not require a waveguide. In a theoretical investigation of Thomson scattering, the optical analogue of undulator radiation, the limits of Thomson sources in scaling towards higher peak brilliances are highlighted. This leads to a novel method for generating brilliant, highly tunable X-ray sources, which is highly energy efficient by circumventing the laser Rayleigh limit through a novel traveling-wave Thomson scattering (TWTS) geometry. This new method suggests increases in X-ray photon yields of 2-3 orders of magnitudes using existing lasers and a way towards efficient, optical undulators to drive a free-electron laser. The results presented here extend far beyond the scope of this work. The possibility to use lasers as particle accelerators, as well as optical undulators, leads to very compact and energy efficient synchrotron sources. The resulting monoenergetic radiation of high brilliance in a range from extreme ultraviolet (EUV) to hard X-ray radiation is of fundamental importance for basic research, medical applications, material and life sciences and is going to significantly contribute to a new generation of radiation sources and free-electron lasers (FELs).

Die vorliegende Arbeit beschäftigt sich in Experiment und Theorie mit Laser-Plasma beschleunigten Elektronen und optischen Undulatoren zur Erzeugung von brillianter Synchrotronstrahlung. Zum ersten Mal wird experimentell nachgewießen, dass laserbeschleunigte Elektronenpulse kürzer als 30 fs sind. Ferner werden solche Elektronenpulse erstmalig in einem Demonstrationsexperiment durch einen magnetischen Undulator als Synchrotronstrahlenquelle genutzt. Aufbauend auf diesen experimentellen Erkenntnissen, sowie umfangreichen numerischen Simulationen zur Thomsonstreuung, werden die theoretischen Grundlagen einer neuartigen Interaktionsgeometrie für Laser-Materie Wechselwirkungen entwickelt. Diese neue, in der Anwendbarkeit sehr allgemeine Methode basiert auf raum-zeitlicher Laserpulsformung durch nichtlineare Winkeldispersion wie diese durch VLS- (varied-line spacing) Gitter erzeugt werden kann und hat den Vorteil nicht durch die Fokussierbarkeit des Lasers (Rayleighlänge) begrenzt zu sein. Zusammen mit laserbeschleunigten Elektronen ermöglicht dieser traveling-wave Thomson scattering (TWTS) benannte Ansatz neuartige, nur auf optischer Technologie basierende Synchrotronstrahlenquellen mit Zentimeter bis Meter langen optische Undulatoren. Die hierbei mit existierenden Lasern erzielbaren Brillianzen übersteigen diese bestehender Thomsonquellen-Designs um 2-3 Größenordnungen. Die hier vorgestellten Ergebnisse weisen weit über die Grenzen der vorliegenden Arbeit hinaus. Die Möglichkeit Laser als Teilchenbeschleuniger und auch optischen Undulator zu verwenden führt zu bauartbedingt sehr kompakten und energieeffizienten Synchrotronstrahlungsquellen. Die hieraus resultierende monochromatische Strahlung hoher Brillianz in einem Wellenlängenbereich von extremen ultraviolett (EUV) zu harten Röntgenstrahlen ist für die Grundlagenforschung, medizinische Anwendungen, Material- und Lebenswissenschaften von fundamentaler Bedeutung und wird maßgeblich zu einer neuen Generation ultrakurzer Strahlungsquellen und freien Elektronenlasern (FELs) beitragen. / This thesis investigates the use of high-power lasers for synchrotron radiation sources with high brilliance, from the EUV to the hard X-ray spectral range. Hereby lasers accelerate electrons by laser-wakefield acceleration (LWFA), act as optical undulators, or both. Experimental evidence shows for the first time that LWFA electron bunches are shorter than the driving laser and have a length scale comparable to the plasma wavelength. Furthermore, a first proof of principle experiment demonstrates that LWFA electrons can be exploited to generate undulator radiation. Building upon these experimental findings, as well as extensive numerical simulations of Thomson scattering, the theoretical foundations of a novel interaction geometry for laser-matter interaction are developed. This new method is very general and when tailored towards relativistically moving targets not being limited by the focusability (Rayleigh length) of the laser, while it does not require a waveguide. In a theoretical investigation of Thomson scattering, the optical analogue of undulator radiation, the limits of Thomson sources in scaling towards higher peak brilliances are highlighted. This leads to a novel method for generating brilliant, highly tunable X-ray sources, which is highly energy efficient by circumventing the laser Rayleigh limit through a novel traveling-wave Thomson scattering (TWTS) geometry. This new method suggests increases in X-ray photon yields of 2-3 orders of magnitudes using existing lasers and a way towards efficient, optical undulators to drive a free-electron laser. The results presented here extend far beyond the scope of this work. The possibility to use lasers as particle accelerators, as well as optical undulators, leads to very compact and energy efficient synchrotron sources. The resulting monoenergetic radiation of high brilliance in a range from extreme ultraviolet (EUV) to hard X-ray radiation is of fundamental importance for basic research, medical applications, material and life sciences and is going to significantly contribute to a new generation of radiation sources and free-electron lasers (FELs).