The first part of this dissertation (Chapters 1 to 4) describes the use of magnetic resonance techniques for polymeric material characterizations in solutions, with emphasis on methods utilizing magnetic field gradients - magnetic resonance imaging (MRI) and pulsed-field-gradient (PFG) NMR. The second part (Chapter 5) presents enhancements to dynamic nuclear polarization, an intensity enhancement approach for magnetic resonance techniques. In Chapter 2, I illustrate a characterization method to quantify free polymer chain content in a polymer/DNA complex (polyplex) formulation via one-dimensional proton NMR experiments. This assessment of free polymer quantity has critical impacts on in vivo gene transfection efficiency, cellular uptake, as well as toxicity of polycationic gene delivery vectors. Specifically, I investigated the complexation properties of three different polymeric "theranostic" agents, which combine an imaging functionality on the polymer as well as a DNA/RNA complexation component. These agents are under development to allow real time clinical monitoring of drug delivery and efficacy using MRI. Our NMR method provides simple and quantitative assessment of free and DNA-complexed polymers, including the actual polymer amine to DNA phosphate molar ratio (N/P ratio) within polyplexes. The NMR results are in close agreement with the stoichiometric number of polymer/DNA binding obtained by isothermal titration calorimetry. The noninvasive nature of this method allows broad application to a range of polyelectrolyte coacervates, for understanding and optimizing polyelectrolyte complex formation. Chapter 3 demonstrates a time-resolved MRI approach for measuring diffusion of drug-delivery polymeric nanoparticles on mm to cm scales as well as monitoring nanoparticle concentration distribution in bulk biological hydrogels. Our results show that as the particle size and surface charge become larger, collagen gel at tumor relevant concentration (1.0 wt.%) presents a more significant impediment to the diffusive transport of negatively charged nanoparticles. These results agree well with those obtained by fluorescence spectroscopies (neutral or slightly positively charged diffusing particles) as well as the proposed electrostatic bandpass theory of tumor interstitium (negatively charged particles). This study provides fundamental information for the design of polymeric theranostic vectors and carries implications that would benefit the understanding of nanoparticle transport in solid tumors. Furthermore, this work takes a significant step toward developing quantitative and real time in vivo monitoring of clinical drug delivery using MRI. Chapter 4 addresses the application of PFG-NMR for the determination of weight-average molar mass (Mw) for polyanions that have anti-HIV activity through the measurement of polymer diffusion coefficients in solutions. The effective characterization of molecular weights of polyelectrolytes has been a general and growing problem for the polymer industry, with no clear solutions in sight. In this study, we obtained the molar masses (Mw) for two series of sulfonated copolymers using sodium polystyrene sulfonate samples as molecular weight standards. PFG-NMR has notable advantages over conventional techniques for the characterization of charged polymers and shows great promise for becoming an effective alternative to chromatography methods. Chapter 5 is devoted to experimental and theoretical studies of liquid state dynamic nuclear polarization (DNP) via the Overhauser effect. Based on the adventurous work done by previous Dorn group members, we show that for 1H-nuclide-containing systems, the dipolar DNP enhancement can be significantly improved by decreasing the correlation time of the interaction by utilizing a supercritical fluid (SF CO2) which allows for greater dipolar enhancements at higher magnetic fields. For molecules containing the ubiquitous 13C nuclide, we show that previously unreported sp hybridized (H-C) alkyne systems represented by the phenylacetylene-nitroxide system exhibit very large scalar-dominated enhancements. Furthermore, we show for a wide range of molecular systems that the Fermi contact interaction can be computationally predicted via electron-nuclear hyperfine coupling and correlated with experimental 13C DNP enhancements. For biomedical applications, the enhancement of metabolites in SF CO2 followed by rapid dissolution in water or biological fluids is an attractive approach for future hyperpolarized NMR and MRI applications. Moreover, with the aid of density functional theory calculations, solution state DNP provides a unique approach for studying intermolecular weak bonding interaction of solutes in normal liquids and SF fluids. / Ph. D.

In dieser Arbeit wurde die Methode der breitbandigen fs-zeitaufgelösten Fluoreszenzaufkonversionsspektroskopie (FLUPS) weiterentwickelt und vollständig theoretisch beschrieben, was anhand des Vergleichs von vorhergesagten und experimentell bestimmten photometrischen Korrekturfunktionen gezeigt werden konnte. Die Methode wurde verwendet, um lokale Fluoreszenzspektren von solvatochromen Sonden in der Nähe bestimmter Matrizes in wässrigen Lösungen zu messen. Aus der Dynamik der Stokes-Verschiebung konnte die Solvatations- bzw. Umgebungsdynamik bestimmt werden. Es wurden mittlere Solvatationszeiten τsolv von 0.57±0.06 für reines Wasser, 2.8±0.2 ps für DNA, 480±30 ps für Phospholipid-Kopfgruppen, 0.71±0.03 ps für ein Peptid (α-Helix) und 0.76±0.03 ps für eine t-Butyl-Gruppe erhalten. Hervorzuheben sind dabei die überraschend schnelle Relaxation nahe des Peptids und die sehr langsame Dynamik nahe der Lipid-Kopfgruppen, welche über 5 Größenordnungen der Zeit beobachtet wurde. Um den Einfluss einer hydrophoben Gruppe auf die Solvatationsdynamik erstmals zu aufzuzeigen, wurden präzise Messungen bei verschiedenen Temperaturen vor-genommen. Zuordnungen dieser Dynamiken zu molekularen Prozessen konnten durch Vergleiche zu MD-Simulationen durchgeführt werden. / The method of broadband fs time-resolved fluorescence upconversion spectroscopy (FLUPS) was further developed and completely theoretically described in this work. This was shown by comparing predicted and measured photometric correction functions. This method was used to obtain local fluorescence spectra of solvatochromic dyes near certain matrices in aqueous solution. From the dynamics of the Stokes-Shift the solvation or environmental dynamics respectively were obtained. Average solvation times τsolv of 0.57±0.06 for bulk water, 2.8±0.2 ps for DNA, 480±30 ps for phospholipid head groups, 0.71±0.03 ps for a peptide (α-helix) and 0.76±0.03 ps for a t-butyl group were obtained. Emphasized are the surprisingly fast dynamics near the peptide and the slow dynamics of the lipid head group region. The latter was observed over 5 orders of magnitude in time. To distinguish the influence a hydrophobic group for the first time, precise measurements at different temperatures were performed. Molecular processes were assigned to the obtained dynamics by comparisons to MD studies.

Doctor of Philosophy / Department of Physics / Itzhak Ben-Itzhak / Patrick Richard / This work focuses on the ultrafast dynamics of electrons and phonons in graphitic materials. In particular, we experimentally investigated the factors which influence the transport properties of graphite and carbon nanotubes. In the first part of this dissertation, we used Time-resolved Two Photon photoemission (TR-TPP) spectroscopy to probe the dynamics of optically excited charge carriers above the Fermi energy of double-wall carbon nanotubes (DWNTs). In the second part of this study, time-resolved anti-Stokes Raman (ASR) spectroscopy is applied to investigating in real time the phonon-phonon interactions, and addressing the way the temperature affects the dynamics of single-wall carbon nanotubes (SWNTs) and graphite. With respect to the first part, we aim to deeply understand the dynamics of the charge carriers and electron-phonon interactions, in order to achieve an as complete as possible knowledge of DWNTs. We measured the energy transfer rate from the electronic system to the lattice, and we observed a strong non-linear increase with the temperature of the electrons. In addition, we determined the electron-phonon coupling parameter, and the mean-free path of the electrons. The TR-TPP technique enables us to measure the above quantities without any electrical contacts, with the advantage of reducing the errors introduced by the metallic electrodes. The second investigation uses time-resolved ASR spectroscopy to probe in real time the G-mode non-equilibrium phonon dynamics and the energy relaxation paths towards the lattice by variation of the temperature in SWNTs and graphite. The lifetime range of the optically excited phonons obtained is 1.23 ps to 0.70 ps in the lowest (cryogenic temperatures) and highest temperature limits, respectively. We have also observed an increase in the energy of the G-mode optical phonons in graphite with the transient temperature. The findings of this study are important since the non-equilibrium phonon population has been invoked to explain the negative differential conductance and current saturation in high biased transport phenomena.

La matière dense et tiède (WDM pour Warm Dense Matter) est caractérisée par des températures proches de celle de Fermi et des densités proches du solide. Cette thèse présente des études expérimentales de la WDM éventuellement hors équilibre électron-ion, à l'aide de la spectroscopie d'absorption X près des seuils (XANES) résolue en temps. Nous avons développé un dispositif expérimental de XANES résolu en temps, basé sur un spectromètre à deux cristaux de Bragg, qui permet d'obtenir d'une part le signal émis par la source X utilisée, et d'autre part le signal transmis à travers un échantillon fin d'aluminium. La comparaison de ces deux grandeurs permet de mesurer l'absorption absolue de l'échantillon. L'échantillon est excité par un faisceau laser ultra-bref afin d'atteindre les conditions thermodynamiques attendues.Le dépôt laser étant réalisé sur les électrons de l'échantillon, les ions restent froids pendant l'interaction. L'équilibration thermique qui suit a une durée attendue de l'ordre de quelques picosecondes. Lors d'une première expérience, nous avons étudié la dynamique des transitions de phase subies par une feuille d'aluminium de 100 nm d'épaisseur, chauffée par un laser de 120 fs, avec un flux relativement élevé (6 J/cm²). La transition solide-liquide a lieu sur une échelle de temps plus faible que la résolution (environ 3 ps). La transition liquide-vapeur atomique a lieu après une vingtaine de picosecondes, en accord avec des simulations hydrodynamiques. Afin d'observer plus précisément la transition solide-liquide, nous avons réalisé une seconde expérience avec des flux plus faibles (< 1J/cm²). La feuille d'aluminium reste dans un état localement structuré aux temps longs. L'observation de la diminution progressive des modulations XANES, correspondant à une perte partielle d'ordre local, permet de déterminer la dynamique de l'augmentation de la température ionique. La comparaison des résultats expérimentaux avec des simulations hydrodynamiques, et de dynamique moléculaire quantique, a montré que le XANES est un diagnostic pertinent de la température ionique pendant et au delà de la fusion, permettant de suivre l'équilibration thermique électrons-ions. Nous avons constaté un temps caractéristique de l'équilibration significativement plus long qu'attendu, ce qui questionne la détermination du taux de collisions électrons-ions dans le régime dense et tiède. Ce même diagnostic a été exploité lors de deux expériences où nous avons étudié la silice comprimée par un choc laser jusqu'à des densités atteignant plus de deux fois celle du solide. Nous avons ainsi pu suivre l'évolution des structures électronique et ionique de la silice. Pour obtenir une meilleure résolution temporelle, nous avons réalisé deux autres expériences en utilisant une source X bêtatron et un laser X à électrons libres. La faisabilité d'expériences de XANES avec des résolutions femtosecondes a ainsi été démontrée. / Warm Dense Matter (WDM) is characterized by temperatures near the Fermi one and densities close to the solid. Experimental studies of WDM eventually out of electron-ion equilibrium are presented in this thesis with the help of time-resolved X-ray Absorption Near Edge Spectroscopy(XANES).We have developed a time-resolved XANES set-up, based on a two-Bragg-crystals spectrometer, allowing to record in one hand the X-ray source emitted signal, and in the other hand the transmitted one through a thin aluminum sample. The absolute absorption of the sample is measured comparing these two signals. The aluminum sample is heated by an ultrafast laser beam in order to reach the required thermodynamical conditions. Note that the energy is deposited on the electrons, whereas the ions keep cold during the interaction. The thermal equilibration follows with an expected picosecond time scale. We performed a first experiment with the aim of studying the phase transitions undergone by a 100 nm depth aluminum foil, heated with a 120fs laser with a high fluence (6 J/cm²). The solid-liquid transition occurs on a time-scale shorter than the experimental resolution (about 3 ps). Le liquid-vapor transition occurs after about 20 ps, consistent with hydrodynamical simulations. In order to study more precisely the solid-liquid transition, we performed a second experiment with the same set-up but lower laser fluences (< 1 J/cm²). The aluminum foil stays in a locally-structured state even after long delays. The dynamics of the ionic temperature increase can be followed watching the progressive lessening of XANES modulations, corresponding to a partial decrease of the local order. Then one can reach the thermal electron-ion equilibration dynamics. The comparison of experimental data with hydrodynamics and quantum molecular dynamics simulations have revealed the relevance of XANES measurements in order to follow the ionic temperature during and above melting. The precision of the measurements allow to notice a significantly longer equilibration time-scale than expected, questioning the electron-ion collision rate determination in the warm dense regime. The same diagnostic has been operated during two experiments in order to study laser-shock compressed silica up to densities doubling the solid one. We have been able to follow the evolution of the electronic and ionic structures of silica. In order to reach a shorter time resolution, we performed experiments with two other X-ray sources : betatron and a X-ray free electron laser. The feasibility of femtosecond time-resolved XANES experiments have been demonstrated.

In this work, experimental and theoretical approaches are applied to the study of chemical reaction dynamics. In Chapter 2, two applications of transition state theory are presented: (1) Application of microcanonical transition state theory to determine the rate constant of dissociation of C2F3I after π∗ ← π excitation. It was found that this reaction has a very fast rate constant and thus is a promising system for testing the statistical assumption of molecular reaction dynamics. (2) A general rate constant expression for the reaction of atoms and molecules at surfaces was derived within the statistical framework of flexible transition state theory. In Chapter 4, a computationally efficient TDDFT approach was found to produce useful potential energy surface landscapes for application to non-adiabatic predissociative dynamics of the molecule CS2 after excitation from the ground state to the singlet C-state. In Chapter 5, ultrafast experimental results of excitation of CS2 to the predissociative neutral singlet C-state is presented. The bandwidth of the excitation laser was carefully tuned to span a two-component scattering resonance with each component differently evolving electronically with respect to excited state character during the quasi-bound oscillation. Scalar time-resolved photoelectron spectra (TRPES) and vector time-resolved photoelectron angular distribution (TRPAD) observables were recorded during the predissociation. The TRPES yield of photoelectrons was found to oscillate with a quantum beat pattern for the photoelectrons corresponding to ionization to the vibrationless cation ground state; this beat pattern was obscured for photoelectron energies corresponding to ionization from the vibrationally excited CS2 cation. The TRPAD data was recorded for two general molecular ensemble cases: with and without a pre-excitation alignment laser pulse. It was found that in the case of ensemble alignment (Chapter 6), the “molecular frame” TRPAD (i.e. TRMFPAD) was able to image the purely valence electronic dynamics of the evolving CS2 C-state. The unaligned ensemble TRPAD observable suffers from excessive orientational averaging and was unable to observe the quantum beat. Engineering efforts were also undertaken to eliminate scattered light background signal (Chapter 7, Appendix A) and improve laser stability as a function of ambient pressure (Appendix B) for TRMFPAD experiments. / Thesis (Ph.D, Chemistry) -- Queen's University, 2012-09-11 22:18:20.89

The subject of this thesis is the design and development of a unified set up for femtosecond transient absorption and ultrafast Raman loss spectroscopy and demonstrate its potential in capturing the ultrafast photophysical and photochemical processes with excellent time and frequency resolution. Ultrafast spectroscopy has been serving as a powerful tool for understanding the structural dynamical properties of molecules in the condensed and gas phase. The advent of ultrashort pulses with their high peak power enables the laser spectroscopic community to study molecular reaction dynamics and photophysics that happen at extremely short timescales, ranging from picosecond to femtosecond. These processes can be measured with extremely high time resolution, which helps to resolve the under-lying molecular process. But in order to understand the global mechanism of the underlying molecular processes, we have to resolve the nuclear dynamics with the proper frequency resolution. However, achieving both, time and frequency resolutions simultaneously is not possible according to the Heisenberg uncertainty principle. Later, this limitation was overcome by femtosecond stimulated Raman spectroscopy (FSRS), a third order non-linear Raman spectroscopy. In this thesis we introduced the ultrafast Raman loss spectroscopic (URLS) technique which is analogous to FSRS, offering the modern ultrafast community to resolve molecular processes with better signal-to-noise ratio along with proper time and frequency resolution. We demonstrate the experimental procedure including the single shot detection scheme to measure whitelight background, ground state Ra-man, transient absorption and transient Raman in shot-to-shot detection fashion. URLS has been applied to understand the excited state planarization dynamics of 1,4-bis(phenylethynyl)benzene (BPEB) in different solvents. In addition, excitation wavelength dependent conformational reorganization dynamics of different sub-sets of thermally activated ground state population of BPEB are also discussed. Using the same techniques along with femtosecond transient absorption, we demonstrate the ultrafast vibrational energy transfer and the role of coherent oscillations of low frequency vibrations on the solution phase photo-isomerization of trans-stilbene from an optically excited state. The effects of solvents on the coherent nuclear motion are also discussed in the context of reaction rates. 2

<div><p><br></p></div><p>This study makes use of a Time-Resolved Raman Spectroscopy (TRRS) system developed in the Purdue Civil Engineering spectroscopy laboratory to advance technology critical to enable field deployment of Raman spectroscopic systems, with a primary focus on developing solutions to overcome two specific barriers to Raman analysis in the natural environment: (1) obtaining Raman spectra of chemical compounds at field-relevant concentrations, and (2) realizing economical spatial monitoring. To inform both streams of activity, this work first explores the role of component choice and apparatus design on Raman system output. A component-level Raman system transfer function is developed in terms of intensity, wavelength, and time which yields detailed insight into system performance that greatly exceeds traditional single “system factor” treatments of apparatus effects. The modelling frame provided by the transfer function is universally applicable in that it is inclusive of the majority of component choices that may be encountered in any open-path or closed-path Raman system, and is likely to be valuable in efforts to assess the performance benefits and limitations of system designs, modify or tailor apparatus layouts, facilitate experiment design, and compare results obtained on different systems. </p><p><br></p><p>The system characterization offered by the transfer function is then employed to develop a multi-photon counting algorithm realized through digital signal processing (DSP) which captures photon arrivals traditionally ignored in conventional counting methods. This approach increases acquired Raman intensity for any given analyte by using detector output voltage or a voltage-time product as an energy proxy – an approach that is likey broadly applicable to any spectroscopic techniques employing detectors that make use of the photoelectric effect. In experiments carried out on analytes (nitrate, isopropanol, and rhodamine 6G) in aqueous solutions, enhanced observations enabled by the multi-photon counting algorithm are shown to increase observed Raman intensities of low Raman-yield solutions 2.0-3.1-fold compared to single-threshold analysis, and also extend the upper observation limit of strong Raman-yield solutions that would traditionally saturate detectors using a binary photon counting scheme. Notably, the improved performance offered by the multi-photon counting algorithm is realized through comparison of multi-photon and conventional counting algorithms applied to the same data in a post-processing exercise, thus eliminating any effects of test-to-test variation on results, and highlighting the ability to employ the developed counting approach without modification of traditional systems.</p><p><br></p><p>Additional insights from the system transfer function are also used to inform exploration of a novel approach to enable spatial environmental monitoring via Raman spectroscopy by combining fiber optics, optical switch technology, and the Raman system prototype. Tests designed to evaluate the system configured as a multiplexed optically switched fiber optic network demonstrate the potential to deliver excitation and collect Raman scattering from different desired monitoring locations with a sole excitation source and a single detector over substantial distances. Using nitrate as an example compound of interest, it is demonstrated that the system has a detection limit of 5 ppm within approximately 1.5 meters, which increases to 15 ppm at 100 m, and 38 ppm at 200 m. Modelling informed using the developed system transfer function highlights that improving the prototype by eliminating fiber connectors and making use of commercially available visible-light optimized fiber can substantially extend the range of the system, offering a 15-ppm nitrate detection limit at 2100 m. As increases in laser power, testing time, and collection optic efficiency are all also straightforward and viable, the prototype demonstrates realistic potential to achieve field relevant detection sensitivity over great distance.</p><p><br></p><p>As a final demonstration of system potential, a set of experiments on aqueous nitrate solutions is performed to understand the influence of turbidity, fluorescence, optics size, and varied raw data integration lengths on Raman observations. Results demonstrate that cumulative advances in the TRRS system establish a new generation of Raman spectroscopic sensing amenable to long-term environmental monitoring over significant spatial extent in complex in-situ conditions. Specific advances made herein include enhanced power delivery and scattered light collection informed by the system transfer function, increases in sensitivity from multi-photon counting, and incorporation of optical multiplexing. Overall, the Time-Resolved Raman Spectroscopic System (TRRS) now offers a set of capabilities that bring in-field deployment within practical reach.</p>

This thesis presents HELIOS, an in-house laboratory for time-resolved pump-probe spectroscopy with extreme-ultraviolet (XUV) probe radiation. A wide span of pump wavelengths can be generated using commercial laser equipment while XUV probe radiation is generated via a high harmonic generation process in a noble gas delivering probe photons with energies between 20 eV and 72 eV. The XUV beam path features a time-preserving monochromator and was constructed and built in-house. HELIOS features an overall time resolution of about 50 fs when using 800 nm pump and 41 eV probe photons. An energy resolution of 110 meV at 41 eV photon energy can be achieved. HELIOS features two beamlines. One µ-focus beamline with an XUV focal size of about 20 µm can be used with experiments that require such a small XUV focal size as well as with different end stations. The other beamline features a semi-permanently mounted end station for angle-resolved photoelectron spectroscopy under ultra-high vacuum conditions. Experiments demonstrating the usability of HELIOS and the two beamlines are presented. A pump-probe measurement on graphene demonstrates the capability of determining a large part of the k-space in only one measurement due to the use of an ARTOF angle-resolved time-of-flight electron spectrometer. A non-angle-resolved pump-probe measurement on the conducting polymer PCPDTBT demonstrates the high signal-to-noise ratio achievable at this beamline in non-angle-resolved photoelectron-spectroscopy pump-probe measurements. The usability of the µ-focus beamline is demonstrated with time-resolved measurements on magnetic samples employing an in-house-designed spectrometer. These experiments allow the retrieval of element-specific information on the magnetization within a sample employing the transversal magneto-optical Kerr effect (T-MOKE). Additionally, a Fourier transform spectrometer for the XUV is presented, the concept was tested at a synchrotron and it was used to determine the longitudinal coherence of the XUV radiation at HELIOS.

This thesis is concerned with the influence of nanoscale boundaries and interfaces upon the electronic processes that occur within both organic and inorganic semiconductors. Photoluminescent polymers, highly conducting polymers and nanoscale inorganic semiconductors have been investigated using state-of-the-art ultrafast optical techniques, to provide information on the sub-picosecond photoexcitation dynamics in these systems. The influence of dimensionality on the excitation transfer dynamics in a conjugated polymer blend is studied. Using time-resolved photoluminescence spectroscopy, the transfer transients both for a three-dimensional blend film, and for quasi-two-dimensional monolayers formed through intercalation of the polymer blend between the crystal planes of a SnS2 matrix have been measured. A comparison of the experimental data with a simple, dimensionality-dependent model is presented, based on point dipole electronic coupling between electronic transition moments. Within this approximation, the energy transfer dynamics are found to adopt a three-dimensional character in the solid film, and a two-dimensional nature in the monolayers present in the SnS2 -polymer nanocomposite. The time-resolved conductivity of isolated GaAs nanowires has been investigated by optical-pump terahertz-probe time-domain spectroscopy. The electronic response exhibits a pronounced surface plasmon mode that forms within 300 fs, before decaying within 10 ps as a result of charge trapping at the nanowire surface. The mobility has been extracted using the Drude model for a plasmon and is found to be remarkably high, being roughly one third of that typical for bulk GaAs at room-temperature and indicating the high quality and low bulk defect density in the nanowires studied. Finally, the time-resolved conductivity dynamics of photoexcited polymer-fullerene bulk heterojunction blends for two model polymers, P3HT and MDMO-PPV, blended with PCBM are presented. The observed terahertz-frequency conductivity is characteristic of dispersive charge transport for photoexcitation both at the π−π* absorption peak (560 nm for P3HT), and significantly below it (800 nm). The photoconductivity at 800 nm is unexpectedly high, which is attributed to the presence of a charge transfer complex. In addition, the excitation-fluence dependence of the photoconductivity is studied over more than four orders of magnitude. The time-averaged photoconductivity of the P3HT:PCBM blend is over 20 times larger than that of P3HT, indicating that long-lived positive polarons are responsible for the high photovoltaic efficiency of polymer:fullerene blends. At early times (~ ps) the linear dependence of photoconductivity upon fluence indicates that interfacial charge transfer dominates as an exciton decay pathway, generating charges with mobility of at least ~0.1cm2 V−1 s−1. At later times, a sub-linear relationship shows that carrier-carrier recombination effects influence the conductivity on a longer timescale (> 1 μs).

Parallèlement à l’impression jet d’encre et au bioplotting, l’impression d'éléments biologiques assistée par laser (Laser Assisted Bioprinting : LAB) qui utilise le transfert vers l’avant induit par laser (Laser Induced Forward Transfer : LIFT) a émergé comme une méthode alternative dans l’assemblage et la micro–structuration de biomatériaux et de cellules. Le LAB est une technique d’écriture directe qui offre la possibilité d’imprimer des motifs avec une haute résolution spatiale à partir d'une large gamme de matériaux solides ou liquides, tels que des diélectriques, des biomolécules et des cellules vivantes en solution.Dans nos travaux de recherche, nous avons considéré une approche expérimentale et numérique pour étudier les mécanismes physiques mis en jeu lors de la microimpression d’éléments biologiques assistée par laser. Dans un premier temps nous avons défini les paramètres rhéologiques des bioencres et les conditions de transfert (composition, épaisseur et viscosité de la bioencre et énergie laser). Puis nous avons mené une analyse statistique du volume des gouttelettes déposées pour quatre viscosités de bioencre, cinq épaisseurs de bioencre et cinq énergies laser. Ensuite nous avons conçu et mis en place un système d’imagerie résolue en temps pour étudier les effets de la viscosité sur la dynamique de l’éjection. Nous avons ainsi différencié trois régimes d'éjection en fonction de l'énergie laser déposée dans la couche absorbante, de la viscosité et de l'épaisseur de la bioencre. Parallèlement, un modèle numérique a été mis en place pour comprendre et prédire la dynamique de l’éjection en fonction de paramètres multiples : choix et épaisseur de la couche absorbante, épaisseur de la couche de bioencre, énergie laser déposée. Enfin, au regard de ces études, nous proposons un mécanisme d'éjection des microgouttelettes intervenant au cours du procédé de microimpression assistée par laser. / Over this decade, cell printing strategy has emerged as one of the promising approaches to organize cells in two and three dimensional engineered tissues. In parallel with ink-jet printing and bioplotting, Laser Assisted Bioprinting (LAB) using Laser-Induced Forward Transfer (LIFT) has emerged as an alternative method in the assembly and micropatterning of biomaterials and cells. LAB is a laser direct-write technique that offers the possibility of printing micropatterns with high spatial resolution from a wide range of solid or liquid materials, such as dielectrics, biomolecules and living cells in solution. In our research works, we considered an experimental and numerical approach to study the physical mechanisms involved in the biological elements microprinting laser assisted.First we defined the rheological parameters of bioinks and the transfer conditions (composition, thickness and viscosity of the bioink and laser energy). Then we led a statistical analysis of the volume of the transfer droplets for four viscosities of bioink, five thicknesses of bioink and five laser energies. Then we designed and implemented a system for time resolved imaging to study the effects of viscosity on the dynamics of the ejection. Thus we have differentiated three ejection regimes in function of the laser energy released in the absorbing layer, the visocsity and the thickness of the bioink. In parallel, a numerical model was developed to understand and predict the dynamics of the ejection parameters according to multiple choice and thickness of the absorbing layer, thickness of the layer bioencre, energy deposited. Finally, with regard to these studies, we propose a mechanism for ejecting droplets involved in the process of laser-assisted microprinting.