Insight into the relationship between the Ionization Energy (IE) offsets between donor and acceptor materials and the performance of the organic solar cells (OSC) could improve the charge generation efficiency. Charge generation can proceed through two different paths in Bulk Heterojunction (BHJ) based OSCs which are electron transfer from donor to acceptor and hole transfer from acceptor to donor. Electron transfer can be controlled by electron affinities and hole transfer can be controlled by ionization energies. In this work, large IE offsets were investigated in poly(3-hexylthiophene-2,5-diyl)(P3HT):Non Fullerene Acceptor (NFA) based OSCs by fabricating and characterizing devices, also conducting several experiments to optimize the processing conditions for the devices. These results provide an overview of the charge transfer and IE offsets dependence, also a general picture of the photophysics in P3HT:NFAs based OSCs. Moreover, using wide bandgap polymer donor which has shallow IE such as P3HT with low-bandgap NFAs may provide sufficient IE offsets between donor and acceptors enabled us to reach the inverted Marcus regime. In this regime, the electron transfer rate decreases upon decreasing the charge transfer (CT) state energy compared to the exciton energy. The decrease of the internal quantum efficiency (IQE) upon increasing the IE offset suggests that we are in that regime.

SuperB is a high luminosity e+e- collider experiment that is currently being designed to explore the flavour sector of particle physics. The detector at SuperB will contain a drift chamber, a gas filled device used to measure the momentum and identity of particles produced in the collisions. Particle identification in a drift chamber uses the measured amount of ionization deposited by the particle in the cells of the chamber, which provides a measurement of the particle speed. The ionization loss is traditionally measured by integrating the total charge released by the ionization after a gas amplification avalanche process. Since such a measurement has potentially large uncertainties associated with fluctuations in the gas amplification and other processes, it is possible that measuring the number of primary clusters of ionization caused by the particle could provide an improvement in the measurement of the ionization loss. The results of experiments performed at the University of Victoria and the TRIUMF laboratory M11 test beam using a SuperB drift chamber prototype to test the feasibility of counting clusters are presented here. The ability to separate muons and pions at the momenta explored in the TRIUMF testbeam was similar to the ability to separate pions and kaons at the higher momenta of SuperB. It was found that counting the clusters provides a significant improvement to particle identification when combined with the traditional measurement of the integrated charge. / Graduate

No description available.

Group 3 metal clusters are synthesized by laser vaporization in a pulsed cluster beam source and identified with laser ionization time-of-flight mass spectrometry. The adiabatic ionization energies and vibrational frequencies of these clusters are measured using mass-analyzed threshold ionization (MATI) spectroscopy. Their structures and electronic states are determined by combining the MATI spectra with quantum chemical calculations and spectral simulations. This dissertation focuses on the study of several small molecules, which include LaO2, La2, M2O2, M3O4, M3C2, and La3C2O, where M = Sc, Y, and La. Except for La2, these molecules exhibit strong ionic characters between the metal and oxygen or carbon atoms and can be described as [O-][La2+][O-], [M2+]2[O2-]2, [M8/3+]3[O2-]4, [M2+]3[C3-]2, and [La8/3+]3[C3-]2[O2-]. The interactions between the metal atoms form covalent bonds, which can be described by a triple bond in La2, a two-center two electron bond in M2O2, a three-center one electron bond in M3O4, and a three-center three electron bond in M3C2. In addition, the electron in the non-bonding highest occupied molecular orbital (HOMO) is localized in the La 6s orbital in LaO2 and La3C2O. The ground states of these molecules are all in low electron-spin states with the spin multiplicities of 1 or 2. Although the ground electronic state of LaO2 is a linear structure, the excited quartet state of the molecule is determined to be a bent structure. M2O2 and M3O4 have the planar rhombic and cage-like structures, respectively; whereas M3C2 has a trigonal bipyramid structure. La3C2O is formed by oxygen binding with two La atoms of La3C2. Ionization removes a metal-based (n+1)s electron in all neutral molecules, and the resultant ions have similar geometries to those of the corresponding neutral states. In the case of La2, additional ionization of a La 5d electron is also observed.

This thesis discusses methods for the comparatively mild covalent functionalization of graphene. Several graphene models were investigated: polycyclic aromatic hydrocarbons (PAHs), chemical vapor deposition (CVD)-graphene on SiO2/Si substrate, graphite foil, graphite flakes, kish graphite and highly oriented pyrolytic graphite. The PAHs were viewed as graphene edge analogs with the following molecules representing different edge motifs: pyrene, perylene, benzo[a]pyrene, benzo[e]pyrene, triphenylene, acenapthylene, and anthracene. Ozone was used in combination with different solvents to functionalize PAHs, graphite, and CVD-graphene on SiO2/Si. Ozonation in water or methanol resulted in trapping of the carbonyl oxide intermediate that was formed in the reaction, producing a variety of functional groups. Ozonation in hydrogen peroxide solution with sonication promoted radical formation, possibly resulting in edge-oxidation of graphite. The regioselectivity for addition reactions (ozonolysis) and electrophilic aromatic substitution reactions with graphene edges is discussed. To achieve functionalization of the basal plane of graphite or graphene, white light irradiation was used in combination with several transfer hydrogenation reagents. Formic acid treatment under irradiation resulted in the expected hydrogenation, whereas iso-propanol treatment resulted in iso-propanol attachment to the graphene. The developed methods provide opportunities for graphene functionalization without the need for metal based reagents or harsh conditions.

Metal-cyclic hydrocarbon complexes were prepared in a laser-vaporization molecular beam source and studied by single-photon zero electron kinetic energy (ZEKE) and IR-UV resonant two-photon ionization (R2PI) spectroscopy. The ionization energies and vibrational frequencies of the metal complexes were measured from the ZEKE spectra. Metal-ligand bonding and low-lying electronic states of the neutral and ionized complexes were analyzed by combining the ZEKE measurements with density functional theory (DFT) calculations. In addition, C-H stretching frequencies were measured from the R2PI spectra. In this dissertation, metal complexes of 1, 3, 5, 7-cyclo-octatetraene (COT), toluene, p-xylene, mesitylene, hexamethylbenzene, biphenyl, naphthalene, pyrene, perylene, and coronene were studied. For each metal-ligand complex, different effects from the metal coordination have been identified. Although free COT is a nonaromatic molecule with a tub-shaped structure, the group III transition metal atoms (Sc, Y, and La) donate two electrons to a partially filled π orbital of COT, making the ligand a dianion. As a result, metal coordination converts COT into a planar, aromatic structure and the resulting complex exhibits a half-sandwich structure. For the Sc(methylbenzene) complexes, the benzene rings of the ligands are bent and the π electrons are localized in a 1, 4-diene fashion due to differential Sc binding with the carbon atoms of the rings. Due to differential metal binding, the degenerate d orbitals split and the Sc-methylbenzene complexes prefer the low-spin ground electronic states. In addition, as the number of methyl group substituents in the ligand increases, the ionization energies (IEs) of the Sc-methylbenzene complexes decrease. However, Ti, V, or Co coordination does not disrupt the delocalized π electron network within the carbon skeleton in the high-spin ground states of the metal complexes. For group VI metal (Cr, Mo, and W)-bis(toluene) complexes, methyl substitution on the benzene ring yields complexes with four rotational conformers of 0°, 60°, 120°, and 180° conformation angles between two methyl groups. In addition, variable-temperature ZEKE spectroscopy using He, Ar, or their mixtures has determined the totally eclipsed 0° rotamer to be the most stable. When there are two equivalent benzene rings, the metal (Ti, Zr or Hf) binds to both the benzene rings of biphenyl, or the metal (Li) binds to one of the benzene rings of naphthalene. On the other hand, the metal (Li) favors the ring-over binding site of the benzene ring with a higher π electron content and aromaticity in pyrene, perylene, and coronene.

Metal-hydrocarbon complexes were prepared in a laser-vaporization molecular beam source and studied by single-photon zero electron kinetic energy (ZEKE) and mass-analyzed threshold ionization (MATI) spectroscopy. The ionization energies and vibrational frequencies of the metal complexes were measured from the ZEKE and MATI spectra. Metal-ligand bonding and low-lying electronic states of the neutral and ionized complexes were analyzed by combining the spectroscopic measurements with quantum chemical calculations and spectral simulations. In this dissertation, the metal complexes of mesitylene, aniline, cyclooctatetraene, benzene, ethene, and propene were studied. For each complex, different effects from metal coordination have been identified. Although metal-bis(mesitylene) sandwich complexes may adopt eclipsed and staggered conformations, the group VI metal-bis(mesitylene) complexes are determined to be in the eclipsed form. In this form, rotational conformers with the methyl group dihedral angles of 0 and 60° are identified for the Cr complex, whereas the 0° rotamer is observed for the Mo and W species. The unsuccessful observation of the 60° rotamer for the Mo and W complexes is the result of its complete conversion to the 0° rotamer in both He and He/Ar carriers. For group III metal aniline complexes, the ZEKE spectrum of each complex exhibits a strong origin band, a short M+-aniline stretching progression, and several low-frequency ligand based vibrational modes. The intensities of most of the transitions can be explained by the Franck-Condon (FC) principle within the harmonic approximation. However, the intensity of the low frequency out-of-plane ring deformation mode is greatly overestimated by the FC calculations and may be caused by the anharmonic nature of the mode. Although aniline offers two possible binding modes for the metal atoms, a п binding mode is identified with the metal atom over the phenyl ring. For Ce, Pr, and Nd(cyclooctatetraene) complexes multiple band systems are observed. This is assigned to the ionization of several low-lying electronic states of the neutral complex. This observation is different from the Gd(cyclooctatetraene) complex, for which a single band system is observed. The presence of the multiple low-energy electronic states is caused by the splitting of the partially filled lanthanide 4f orbitals in the ligand field. The ZEKE spectrum of the Gd(benzene) complex exhibits a strong origin band, whereas the spectrum of Lu(benzene) displays a weak one. The benzene ring is planar in the Gd complex, but bent in the Lu complex. Dehydrogenation and C-C coupling products are observed in the reaction of La atom and ethene/propene. For the La and ethene reaction, La(C2H2) and La(C4H6) complexes are identified. With propene, C-H bond activation leads to the formation of the La(C3H4) and H-La(C3H5) complexes, whereas the C-C coupling yields the La(trimethylenemethane) complex. In addition, the La(CHCCH3) and La(CHCHCH2) isomers of La(C3H4) are observed, which are produced by the 1,2- and 1,3-hydrogen elimination of propene.

Kvantkemiska studier av reaktiviteten hos guldnanopartiklar Au3-Au11 och Au13 mot O- centrerade molekylradikaler OH , OOH , OCH3   och H2O undersöks. Olika molekylära ytegenskaper tas med i beräkningen, elektrostatiska ytpotentialen, den genomsnittliga lokala joniseringsenergin, electron attachment energy och spinndensiteten (VS(r), IS(r), TS(r), ES(r) och S(r)). De erhållna resultaten gäller slutna och öppna skalsystem. Där system med slutna skal bildas från växelverkan mellan en guldklusterradikal och en fri radikal, och system med öppna skal bildas från växelverkan mellan ett jämnt antal guldatomer med en fri radikal. För system med slutna skal Aux-R (där x = 3, 5, 7, 9 eller 11 och R är en O-centrerad radikal) finns det en övergripande trend av bindningsenergin gentemot ES(r), vilket återspeglar elektrofilictiten hos guldnanopartiklar. Multivariata modeller visar vidare hur de olika parametrarna korrelerar gentemot varandra för system med slutna skal.För strukturerna Aux-R (där x=3-11) medl ägst bindningsenergi, dvs. inklusive både slutna och öppna skalsystem, är den tydligaste trenden bindningsenergi vs minimum i ES(r) och parametern TS(r). Vid jämförelse av resultaten av interaktionerna med de fria radikalerna med H2O är trenden alltid tydligast för H2O. I linje med tidigare studier finns det även en korrelation av bindningsenergierna med VS,max och ES,min för H2O. Slutligen sträcker sig trenden med bindningsenergi vs ES,min vidare till systemet som innehåller den icke-plana Au13-strukturen. Denna studie visar kopplingen mellan reaktiviteten hos guldnanopartiklar mot fria radikaler till den lokala ES(r), samtidigt som bidraget från andra ytegenskaper visas. Detta kan vara av betydelse för fortsatta studier kring naturen av interaktioner av guldnanopartiklar. / The nature of gold nanoparticle interactions towards molecular radicals are investigated. Quantum chemical studies of the reactivity of gold nanoparticles Au3-Au11 and Au13 towards O-centered molecular radicals OH , OOH , OCH3   and H2O are performed. Different molecular surface properties are taken into account; the surface electrostatic potential, average local ionization energy, electron attachment energy and spin density (VS(r), IS(r), TS(r), ES(r) and S(r)). The obtained results concern closed and open shell systems. Where closed shell systems are formed from the interaction of a radical gold cluster and a free radical, and open shell systems are formed from the interaction of an even number of gold atoms with a free radical. For closed shell systems Aux-R (where x = 3, 5, 7, 9 or 11 and R is an O-centered radical) there is an overall trend of the binding energy vs the local electron attachment energy, reflecting the electrophilicity of the gold nanoparticles. Multivariate plots further show how the different parameters correlate together for closed shell systems. Looking at the lowest energy structures Aux-R (where x = 3-11), i.e. including closed and open shell systems, the clearest trend is of binding energy vs minima in the local electron attachment energy ES,min and the TS(r) parameter. When comparing the results of the interactions with the free radicals with H2O, the trend is always clearest for H2O. Concurring with previous trends, there is a correlation of the binding energies with VS,max and ES,min for H2O. Lastly, the trend of Binding energy vs ES,min further extends to systems containing the non-planar Au13 structure. This study extends the reactivity of gold nanoparticles towards free radicals to the local electron attachment energy, while showing the contribution of other surface properties. This might be of importance for further studies concerning the nature of gold nanoparticle interactions.

V této práci je prezentována studie fragmentačního procesu zvolené molekuly a jeho vztah ke složení fragmentačních produktů. Práce je zaměřená na výpočet fragmentační energie molekuly pomocí ab initio kvantově chemických metod, metodou „density functional theory (DFT)“ a také srovnáním s experimentem. Je prezentován vliv výpočetní metody, bázového setu, a geometrie molekuly na simulaci. Byla porovnána fragmentace methylfenylsilanu (MPS), dimethylfenylsilanu (DMPS), a trimetylfenylsilanu (TMPS). Fragmentace byla iniciována monochromatickým elektronovým svazkem (EII). Hmotnostní spektrometrie byla využita ke studiu složení fragmentačních produktů MPS a TMPS. Fragmentační produkty MPS a TMPS měřené v rámci této práce byly doplněny o experimentální studii DMPS, která byla prezentována v literatuře. Takto byla získána řada molekul, které jsou strukturně podobné, ale mají výrazně rozdílné chování během fragmentace. Pomocí měření účinného průřezu byly měřeny disociační energie vazeb a tyto disociační energie byly vypočteny pomocí metody DFT. Kombinací teoretického výpočtu metodou DFT a experimentálního měření jsme poukázali na společné rysy a na rozdíly ve fragmentačním schématu všech tří molekul. Navrhli jsme odštěpení dvou vodíkových atomů během plazmově indukovaného fragmentačního procesu. Vodíky mohou být odštěpeny pomocí dvou mechanismů: i. odštěpení dvou vodíků jeden po druhém a ii. odštěpení molekuly H2 v jednom kroku. Z profilů energie dokážeme určit, který mechanismus bude v tom konkrétním případě pravděpodobnější. Předpokládaný mechanismus je v korelaci s experimentálními výsledky fragmentace zjištěnými z hmotnostních spekter.

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