<p>Dissociation dynamics of the ionized molecules HCl and the deuterated system DCl has been studied in gas-phase using synchrotron based photoelectron spectroscopy (PES).</p><p>The inner-valence "(4σ)^-1" photoionization band for DCl and HCl was recorded using maximum resolution in order to probe an interference pattern between a dissociative and a bound electronic state. For HCl⁺, we clearly observed distorted Fano-type peaks even for modest resolution, whereas for DCl⁺, the pattern was hardly discernible. The observation in HCl⁺ has been explained by a coupling between two adiabatic electronic states, where the bound state was populated through non-adiabatic curve-crossing. The nuclear motion of HCl⁺ is too fast for the Born-Oppenheimer approximation to be fully valid in this case. Whereas for DCl⁺, with larger reduced mass and therefore slower nuclear motion, the non-adiabatic coupling is less pronounced, and the vibrational progression vanishes.</p><p>A comparative study between PES and threshold photoelectron spectra (TPES) of the inner-valence bands of HCl and DCl has been performed, showing differences in intensities and shapes of the vibrational bands. These differences were attributed to the fact that the sudden approximation, which can be assumed to be valid for PES, is violated in the case of TPES.</p><p>A resonant Auger electron spectroscopy study of HCl and DCl has been performed, which shows an interference pattern between atomic and molecular Auger- and photoelectron channels. The atomic features are associated with ultra-fast dissociation of the molecules, on the same time scale as the Auger decay. The observation shows that the excited molecular system has to be regarded as a superposition of fragmented and molecular states.</p><p>A study of the <i>X</i>-state of HCl⁺, populated via a core-excited state, shows a selective population of the final state. The explanation was shown to be that the magnetic orientation of the core-hole is transferred to the final state of the molecule.</p><p>A setup for data acquisition of Photo-Electron Photo-Ion Photo-Ion COincidence (PEPIPICO) measurements using a Time-Of-Flight (TOF) spectrometer has been developed. A Time-to-Digital Converter (TDC) card has been linked together with the data treatment program Igor as a user interface. Furthermore, the PEPIPICO spectrometer has been characterized to provide a solid basis for the analysis of experimental data.</p>

Clusters are aggregates of a finite number of atoms or molecules. In the present work, free clusters out of metallic parent materials have been created and studied by synchrotron radiation-based photoelectron spectroscopy. The clusters have been formed and studied in a beam and the electronic structure of the clusters has been investigated. Conclusions have been drawn about the spatial distribution of atoms of different elements in bi-component clusters, about the development of metallicity in small clusters, and about the excitation of plasmons. Bi-component alloy clusters of sodium and potassium and of copper and silver have been produced. The site-sensitivity of the photoelectron spectroscopy technique has allowed us to probe the geometric distribution of the atoms of the constituent elements by comparing the responses from the bulk and surface of the clusters. In both cases, we have found evidence for a surface-segregated structure, with the element with the largest atoms and lowest cohesive energy (potassium and silver, correspondingly) dominating the surface and with a mixed bulk. Small clusters of tin and lead have been probed to investigate the development of metallicity. The difference in screening efficiency between metals and non-metals has been utilized to determine in what size range an aggregate of atoms of these metallic parent materials stops to be metallic. For tin this has been found to occur below ~40 atoms while for lead it happened somewhere below 20-30 atoms. The excitation of bulk and surface plasmons has been studied in clusters of sodium, potassium, magnesium and aluminium, with radii in the nanometer range. The excitation energies have been found to be close to those of the corresponding macroscopic solids. We have also observed spectral features corresponding to multi-quantum plasmon excitation in clusters of Na and K. Such features have in macroscopic solids been interpreted as due to harmonic plasmon excitation. Our observations of features corresponding to the excitation of one bulk and one surface plasmon however suggest the presence of sequential excitation in clusters.

This thesis presents experimental studies of gas phasemolecular relaxation after excitation with synchrotron photonsin the 15-35 eV and in the 70-350 eV regions. In the 15-35 eV region, molecular relaxation by neutraldissociation processes and non Franck-Condon effects in N2 and O2 molecules have beenstudied by means of dispersed fluorescence and photoelectronspectroscopy experimental techniques, respectively. From thedispersed fluorescence data, excitation functions for themeasured atomic fluorescence spectra have been obtained. Fromthe recorded photoelectron spectra vibrational branching ratioshave been produced. The results obtained reveal that Rydbergseries and singly and doubly excited valence states of theappropriate symmetry energetically accessible in the studiedregion and interactions between themaccount for most of theobserved effects in these two type of experiments. In the 70-350 eV range, molecular relaxation processesresulting in fragmentation of CD4 and SF6 after absorption ofsynchrotron light have been studied by energy resolved electronion coincidence technique using a multicoincidence experimentalstation developed by our group during the last five years forsuch type of experiments. The coincidence measurements yieldedmass spectra from which information about the kinematics of thedetected fragments has been deduced by means of Monte Carlosimulations of the experimental peak shapes. The obtainedresults show completely different dissociation patternsdepending on the molecular electronic states studied. Thesepatterns reflect the bonding properties of the excited orbitalsand they permit the description and in some cases theidentification of the different molecular relaxation pathwaysobserved. The achievements presented in this thesis exemplifythe potential of the multicoincidence station used in thereported experiments.

Dissociation dynamics of the ionized molecules HCl and the deuterated system DCl has been studied in gas-phase using synchrotron based photoelectron spectroscopy (PES). The inner-valence "(4σ)-1" photoionization band for DCl and HCl was recorded using maximum resolution in order to probe an interference pattern between a dissociative and a bound electronic state. For HCl+, we clearly observed distorted Fano-type peaks even for modest resolution, whereas for DCl+, the pattern was hardly discernible. The observation in HCl+ has been explained by a coupling between two adiabatic electronic states, where the bound state was populated through non-adiabatic curve-crossing. The nuclear motion of HCl+ is too fast for the Born-Oppenheimer approximation to be fully valid in this case. Whereas for DCl+, with larger reduced mass and therefore slower nuclear motion, the non-adiabatic coupling is less pronounced, and the vibrational progression vanishes. A comparative study between PES and threshold photoelectron spectra (TPES) of the inner-valence bands of HCl and DCl has been performed, showing differences in intensities and shapes of the vibrational bands. These differences were attributed to the fact that the sudden approximation, which can be assumed to be valid for PES, is violated in the case of TPES. A resonant Auger electron spectroscopy study of HCl and DCl has been performed, which shows an interference pattern between atomic and molecular Auger- and photoelectron channels. The atomic features are associated with ultra-fast dissociation of the molecules, on the same time scale as the Auger decay. The observation shows that the excited molecular system has to be regarded as a superposition of fragmented and molecular states. A study of the X-state of HCl+, populated via a core-excited state, shows a selective population of the final state. The explanation was shown to be that the magnetic orientation of the core-hole is transferred to the final state of the molecule. A setup for data acquisition of Photo-Electron Photo-Ion Photo-Ion COincidence (PEPIPICO) measurements using a Time-Of-Flight (TOF) spectrometer has been developed. A Time-to-Digital Converter (TDC) card has been linked together with the data treatment program Igor as a user interface. Furthermore, the PEPIPICO spectrometer has been characterized to provide a solid basis for the analysis of experimental data.

Femtosecond time-resolved photoelectron spectroscopy (fsTRPES) experiments have been used to study the photoelectron energy spectra of simple molecules since the 1980’s. Analysis of these spectra provides information about the ultrafast internal conversion dynamics of the parent ions. However, ultraviolet pulses must be used for these pump-probe experiments in order to ionize the molecules. Since current solid state lasers, such as the Ti:sapphire laser, typically produce pulses centered at 800nm, it is necessary to generate UV pulses with nonlinear frequency mixing techniques. I therefore constructed an optical setup to generate the 3rd and 4th harmonics, at 266.7nm and 200nm, respectively, of a Ti:sapphire (Ti:sa) chirped-pulse amplified (CPA) laser system that produces 35fs pulses centered at 800nm. Thin Beta-Barium Borate (β-BaB2O4 or BBO) crystals were chosen to achieve a compromise between short pulse durations and reasonable conversion efficiencies, since ultrashort pulses are quite susceptible to broadening from group velocity dispersion (GVD). Output energies of around 11μJ and 230nJ were measured for the 266.7nm and 200nm pulses, respectively. The transform limits of the 3rd and 4th harmonic pulse lengths were calculated from their measured spectral widths. We found that the 266.7nm bandwidth was large enough to support sub-30fs pulses, and due to cutting at the lower-wavelength end of the 200nm spectrum, we calculated an upper limit of 38fs. The pulses were compressed with pairs of CaF2 prisms to compensate for dispersion introduced by transmissive optics. Two-photon absorption (TPA) intensity autocorrelations revealed fully compressed pulse lengths of 36 ± 2 fs and 42 ± 4 fs for the 3rd and 4th harmonics, respectively.

<p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-bidi-font-weight:bold'>M-DNA is a novel complex formed between DNA and transition metal ions under alkaline conditions.<span style='mso-spacerun:yes'>  </span>The unique properties of M-DNA were manipulated in order to rationally place metal ions at specific regions within a double-stranded DNA helix.<span style='mso-spacerun:yes'>   </span>Investigations using thermal denaturation profiles and the ethidium fluorescence assay illustrate that the pH at which M-DNA formation occurs is influenced heavily by the DNA sequence and base composition.<span style='mso-spacerun:yes'>  </span>For instance, DNA with a sequence consisting of poly[d(TG)d(CA)] is completely converted to M-DNA at pH 7.9 while DNA consisting entirely of poly[d(AT)] remains in the B-DNA conformation until a pH of 8.6 is reached.<span style='mso-spacerun:yes'>  </span>The pH at which M-DNA formation occurs is further decreased by the incorporation of 4-thiothymine (s⁴T).<span style='mso-spacerun:yes'>  </span>DNA oligomers with a mixed sequence composed of </span>half d(AT) and the other half d(TG)d(CA)<span style='mso-bidi-font-weight: bold'> showed that only 50% of the DNA is able to incorporate Zn²⁺ ions at pH 7.9.<span style='mso-spacerun:yes'>  </span>This suggests that only regions corresponding to the tracts of <span class=GramE>d(</span>TG)d(CA) are being transformed.<span style='mso-spacerun:yes'>   </span><o:p></o:p></span></p> <p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-fareast-language:ZH-CN'>Duplex DNA monolayers were self-assembled on gold through <span class=GramE>a</span> Au-S linkage and both B- and M-DNA conformations were studied using X-ray photoelectron spectroscopy (XPS) in order to better elucidate the location of the metal ions.<span style='mso-spacerun:yes'>  </span>The film thickness, density, elemental composition and ratios for samples were analyzed and compared.<span style='mso-spacerun:yes'>  </span>The DNA surface coverage, calculated from both XPS and electrochemical measurements, was <span class=GramE>approximately 1.2 x 10¹³molecules/cm²</span>for B-DNA.<span style='mso-spacerun:yes'>  </span>All samples showed distinct peaks for C 1s, O 1s, N 1s, P 2p and S 2p as expected for a thiol-linked DNA.<span style='mso-spacerun:yes'>  </span></span><span style='mso-bidi-font-weight: bold'>On addition of Zn²⁺ to form M-DNA the C 1s, P 2p and S 2p showed only small changes </span><span style='mso-fareast-language:ZH-CN'>while both the N 1s and O 1s spectra changed considerably.<span style='mso-spacerun:yes'>  </span>This result is consistent with Zn²⁺ interacting with oxygen on the phosphate backbone as well as replacing the imino protons of thymine (T) and guanine (G) in M-DNA.<span style='mso-spacerun:yes'>   </span>Analysis of the Zn 2p spectra also demonstrated that the concentration of Zn²⁺ present under M-DNA conditions is consistent with Zn²⁺ binding to both the phosphate backbone as well as replacing the imino protons of T or G in each base pair.<span style='mso-spacerun:yes'>  </span>After the M-DNA monolayer is washed with a buffer containing only Na⁺ the Zn²⁺ bound to the phosphate backbone is removed while the Zn²⁺ bound internally still remains. </span><span style='mso-bidi-font-weight:bold'>Variable angle x-ray photoelectron spectroscopy (VAXPS) was also used to examine monolayers consisting of mixed sequence oligomers.<span style='mso-spacerun:yes'>  </span>Preliminary results suggest that under M-DNA conditions, the zinc to phosphate ratio changes relative to the position of the <span class=GramE>d(</span>TG)d(CA) tract being at the top or bottom of the monolayer.<span style='mso-spacerun:yes'>  </span><span style='mso-spacerun:yes'> </span><o:p></o:p></span></p> <p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-bidi-font-weight:bold'>Electrochemistry was also used to investigate the properties of M-DNA monolayers on gold and examine how the localization of metal ions affects the resistance through the DNA monolayer.<span style='mso-spacerun:yes'>  </span>T</span>he effectiveness of using the IrCl₆^2-/3-redox couple to investigate DNA monolayers and the potential advantages of this system over the standard Fe(CN)₆^3-/4- redox couple are demonstrated.<span style='mso-spacerun:yes'>  </span>B-DNA monolayers were converted to M-DNA by incubation in buffer containing 0.4 mM Zn²⁺ at pH 8.6 and studied by cyclic voltammetry (CV), electrochemical impedance spectroscopy (EIS) and chronoamperometry (CA) with IrCl₆^2-/3-.<span style='mso-spacerun:yes'>  </span>^{<span style='mso-spacerun:yes'> </span>}Compared to B-DNA, M-DNA showed significant changes in CV, EIS and CA spectra.<span style='mso-spacerun:yes'>  </span>However, only small changes were observed when the monolayers were incubated in Mg²⁺at pH 8.6 or in Zn²⁺ at pH 6.0.<span style='mso-spacerun:yes'>  </span>The heterogeneous electron-transfer rate (<i style='mso-bidi-font-style:normal'>k</i>_ET) between the redox probe and the surface of a bare gold electrode was determined to be 5.7 x 10^-3 cm/s.<span style='mso-spacerun:yes'>  </span>For a B-DNA modified electrode, the <i style='mso-bidi-font-style:normal'>k</i>_ET through the monolayer was too slow to be measured.<span style='mso-spacerun:yes'>  </span>However, under M-DNA conditions, a <i style='mso-bidi-font-style:normal'>k</i>_ET of 1.5 x 10^-3 cm/s was reached.<span style='mso-spacerun:yes'>  </span>As well, the percent change in resistance to charge transfer (R_CT), measured by EIS, <span class=GramE>was</span> used to illustrate the dependence of M-DNA formation on pH.<span style='mso-spacerun:yes'>  </span>This result is consistent with Zn²⁺ ions replacing the imino protons on thymine and guanine residues.<span style='mso-spacerun:yes'>  </span>Also, at low pH values, the percent change in R_CT seems to be greater for <span class=GramE><span style='mso-bidi-font-weight:bold'>d(</span></span><span style='mso-bidi-font-weight: bold'>TG)₁₅d(CA)₁₅ compared to oligomers with mixed d(AT) and d(TG)d(CA) tracts.<span style='mso-spacerun:yes'>  </span></span>The IrCl₆^2-/3-redox couple was also effective in differentiating between single-stranded and double-stranded DNA during dehybridization and rehybridization experiments.<span style='mso-spacerun:yes'>  </span><span style='mso-bidi-font-weight:bold'><o:p></o:p></span></p>

Femtosecond time-resolved photoelectron spectroscopy (fsTRPES) experiments have been used to study the photoelectron energy spectra of simple molecules since the 1980’s. Analysis of these spectra provides information about the ultrafast internal conversion dynamics of the parent ions. However, ultraviolet pulses must be used for these pump-probe experiments in order to ionize the molecules. Since current solid state lasers, such as the Ti:sapphire laser, typically produce pulses centered at 800nm, it is necessary to generate UV pulses with nonlinear frequency mixing techniques. I therefore constructed an optical setup to generate the 3rd and 4th harmonics, at 266.7nm and 200nm, respectively, of a Ti:sapphire (Ti:sa) chirped-pulse amplified (CPA) laser system that produces 35fs pulses centered at 800nm. Thin Beta-Barium Borate (β-BaB2O4 or BBO) crystals were chosen to achieve a compromise between short pulse durations and reasonable conversion efficiencies, since ultrashort pulses are quite susceptible to broadening from group velocity dispersion (GVD). Output energies of around 11μJ and 230nJ were measured for the 266.7nm and 200nm pulses, respectively. The transform limits of the 3rd and 4th harmonic pulse lengths were calculated from their measured spectral widths. We found that the 266.7nm bandwidth was large enough to support sub-30fs pulses, and due to cutting at the lower-wavelength end of the 200nm spectrum, we calculated an upper limit of 38fs. The pulses were compressed with pairs of CaF2 prisms to compensate for dispersion introduced by transmissive optics. Two-photon absorption (TPA) intensity autocorrelations revealed fully compressed pulse lengths of 36 ± 2 fs and 42 ± 4 fs for the 3rd and 4th harmonics, respectively.

<p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-bidi-font-weight:bold'>M-DNA is a novel complex formed between DNA and transition metal ions under alkaline conditions.<span style='mso-spacerun:yes'>  </span>The unique properties of M-DNA were manipulated in order to rationally place metal ions at specific regions within a double-stranded DNA helix.<span style='mso-spacerun:yes'>   </span>Investigations using thermal denaturation profiles and the ethidium fluorescence assay illustrate that the pH at which M-DNA formation occurs is influenced heavily by the DNA sequence and base composition.<span style='mso-spacerun:yes'>  </span>For instance, DNA with a sequence consisting of poly[d(TG)d(CA)] is completely converted to M-DNA at pH 7.9 while DNA consisting entirely of poly[d(AT)] remains in the B-DNA conformation until a pH of 8.6 is reached.<span style='mso-spacerun:yes'>  </span>The pH at which M-DNA formation occurs is further decreased by the incorporation of 4-thiothymine (s⁴T).<span style='mso-spacerun:yes'>  </span>DNA oligomers with a mixed sequence composed of </span>half d(AT) and the other half d(TG)d(CA)<span style='mso-bidi-font-weight: bold'> showed that only 50% of the DNA is able to incorporate Zn²⁺ ions at pH 7.9.<span style='mso-spacerun:yes'>  </span>This suggests that only regions corresponding to the tracts of <span class=GramE>d(</span>TG)d(CA) are being transformed.<span style='mso-spacerun:yes'>   </span><o:p></o:p></span></p> <p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-fareast-language:ZH-CN'>Duplex DNA monolayers were self-assembled on gold through <span class=GramE>a</span> Au-S linkage and both B- and M-DNA conformations were studied using X-ray photoelectron spectroscopy (XPS) in order to better elucidate the location of the metal ions.<span style='mso-spacerun:yes'>  </span>The film thickness, density, elemental composition and ratios for samples were analyzed and compared.<span style='mso-spacerun:yes'>  </span>The DNA surface coverage, calculated from both XPS and electrochemical measurements, was <span class=GramE>approximately 1.2 x 10¹³molecules/cm²</span>for B-DNA.<span style='mso-spacerun:yes'>  </span>All samples showed distinct peaks for C 1s, O 1s, N 1s, P 2p and S 2p as expected for a thiol-linked DNA.<span style='mso-spacerun:yes'>  </span></span><span style='mso-bidi-font-weight: bold'>On addition of Zn²⁺ to form M-DNA the C 1s, P 2p and S 2p showed only small changes </span><span style='mso-fareast-language:ZH-CN'>while both the N 1s and O 1s spectra changed considerably.<span style='mso-spacerun:yes'>  </span>This result is consistent with Zn²⁺ interacting with oxygen on the phosphate backbone as well as replacing the imino protons of thymine (T) and guanine (G) in M-DNA.<span style='mso-spacerun:yes'>   </span>Analysis of the Zn 2p spectra also demonstrated that the concentration of Zn²⁺ present under M-DNA conditions is consistent with Zn²⁺ binding to both the phosphate backbone as well as replacing the imino protons of T or G in each base pair.<span style='mso-spacerun:yes'>  </span>After the M-DNA monolayer is washed with a buffer containing only Na⁺ the Zn²⁺ bound to the phosphate backbone is removed while the Zn²⁺ bound internally still remains. </span><span style='mso-bidi-font-weight:bold'>Variable angle x-ray photoelectron spectroscopy (VAXPS) was also used to examine monolayers consisting of mixed sequence oligomers.<span style='mso-spacerun:yes'>  </span>Preliminary results suggest that under M-DNA conditions, the zinc to phosphate ratio changes relative to the position of the <span class=GramE>d(</span>TG)d(CA) tract being at the top or bottom of the monolayer.<span style='mso-spacerun:yes'>  </span><span style='mso-spacerun:yes'> </span><o:p></o:p></span></p> <p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-bidi-font-weight:bold'>Electrochemistry was also used to investigate the properties of M-DNA monolayers on gold and examine how the localization of metal ions affects the resistance through the DNA monolayer.<span style='mso-spacerun:yes'>  </span>T</span>he effectiveness of using the IrCl₆^2-/3-redox couple to investigate DNA monolayers and the potential advantages of this system over the standard Fe(CN)₆^3-/4- redox couple are demonstrated.<span style='mso-spacerun:yes'>  </span>B-DNA monolayers were converted to M-DNA by incubation in buffer containing 0.4 mM Zn²⁺ at pH 8.6 and studied by cyclic voltammetry (CV), electrochemical impedance spectroscopy (EIS) and chronoamperometry (CA) with IrCl₆^2-/3-.<span style='mso-spacerun:yes'>  </span>^{<span style='mso-spacerun:yes'> </span>}Compared to B-DNA, M-DNA showed significant changes in CV, EIS and CA spectra.<span style='mso-spacerun:yes'>  </span>However, only small changes were observed when the monolayers were incubated in Mg²⁺at pH 8.6 or in Zn²⁺ at pH 6.0.<span style='mso-spacerun:yes'>  </span>The heterogeneous electron-transfer rate (<i style='mso-bidi-font-style:normal'>k</i>_ET) between the redox probe and the surface of a bare gold electrode was determined to be 5.7 x 10^-3 cm/s.<span style='mso-spacerun:yes'>  </span>For a B-DNA modified electrode, the <i style='mso-bidi-font-style:normal'>k</i>_ET through the monolayer was too slow to be measured.<span style='mso-spacerun:yes'>  </span>However, under M-DNA conditions, a <i style='mso-bidi-font-style:normal'>k</i>_ET of 1.5 x 10^-3 cm/s was reached.<span style='mso-spacerun:yes'>  </span>As well, the percent change in resistance to charge transfer (R_CT), measured by EIS, <span class=GramE>was</span> used to illustrate the dependence of M-DNA formation on pH.<span style='mso-spacerun:yes'>  </span>This result is consistent with Zn²⁺ ions replacing the imino protons on thymine and guanine residues.<span style='mso-spacerun:yes'>  </span>Also, at low pH values, the percent change in R_CT seems to be greater for <span class=GramE><span style='mso-bidi-font-weight:bold'>d(</span></span><span style='mso-bidi-font-weight: bold'>TG)₁₅d(CA)₁₅ compared to oligomers with mixed d(AT) and d(TG)d(CA) tracts.<span style='mso-spacerun:yes'>  </span></span>The IrCl₆^2-/3-redox couple was also effective in differentiating between single-stranded and double-stranded DNA during dehybridization and rehybridization experiments.<span style='mso-spacerun:yes'>  </span><span style='mso-bidi-font-weight:bold'><o:p></o:p></span></p>

In order to gain insights into the electronic interactions between metallic gold and self-assembled monolayers composed of π-conjugated thiols, a series of thiol-containing molecules based on a stilbene backbone were synthesized and assembled on gold surface. The resulted monolayers were characterized with a variety of surface-sensitive techniques and the electronic properties of the obtained surfaces were studied with the use of ultraviolet photoelectron spectroscopy. Work-function changes and alignment of the molecular energy levels with respect to the Fermi level of the metal were investigated and important insights regarding the electronic properties of the metal / organic interfaces were obtained. Another aspect of interactions between organic dyes and metallic gold was studied in the context of spectroscopic properties of systems incorporating gold nanoparticles with organic fluorophores covalently attached to the nanoparticle surface. Ultrafast dynamics of the excited-state deactivation of the organic fluorophores attached to the surface of gold nanoparticles were studied with the use of a fs transient absorption technique. It was found that the close proximity of a gold nanoparticle had a profound impact on the excited-state lifetime of the studied organic fluorophore. The influence of the structure of the studied systems on the excited-state deactivation dynamics of the organic fluorophores was described.

In spite of the failures to find an ultimate theory of unconventional superconductivity, after many years of research the scientific community possesses a considerable store of theoretical knowledge about the problem. Over time, the focus is gradually shifted from finding a theoretical description of an experimentally observed phenomenon to distinguishing between multiple models that offer comparably reasonable descriptions. From the point of view of an experimentalist, this means that any qualitative under-standing of an experimental observation would no longer suffice. Instead, the empha-sis in the experimental research should be shifted to accurate quantification of obser-vations, which becomes possible only if the results available from all the available ex-perimental methods are connected together by the theoretical glue. Among the meth-ods that are to be unified, ARPES plays a central role. The reason for this is that it gives access to the single-particle excitation spectrum of the material as a function of both momentum and energy with very high resolution. Other experimental techniques, such as inelastic neutron scattering (INS), Raman spectroscopy, or the newly estab-lished Fourier-transform scanning tunneling spectroscopy (FT-STS) probe more com-plicated two-particle spectra of the electrons and up to now can not achieve the mo-mentum resolution comparable with that of ARPES. Such reasoning serves as the mo-tivation for the present work, in which some steps are done towards understanding the anomalous effects observed in the single-particle excitation spectra of cuprates and relating the ARPES technique to other experimental methods. First, the electronic properties of BSCCO are considered — the superconducting cuprate most studied by surface-sensitive methods. The recent progress in un-derstanding the electronic structure of this material is reported, focusing mainly on the many-body effects (renormalization) and their manifestation in the ARPES spectra. The main result of this part of the work is a model of the Green’s function that is later used for calculating the two-particle excitation spectrum. Then, the matrix element effects in the photoemission spectra of cuprates are discussed. After a general introduction to the problem, the thesis focuses on the recently discovered anomalous behavior of the ARPES spectra that partially originates from the momentum-dependent photoemission matrix element. The momentum- and excitation energy dependence of the anomalous high-energy dispersion, termed “waterfalls”, is covered in full detail. Understanding the role of the matrix element effects in this phenomenon proves crucial, as they obstruct the view of the underlying excitation spectrum that is of indisputable interest. Finally, the work describes the relation of ARPES with other experimental methods, with the special focus on the INS spectroscopy. For the optimally doped bilayer Bi-based cuprate, the renormalized two-particle correlation function in the superconducting state is calculated from ARPES data within an itinerant model based on the random phase approximation (RPA). The results are compared with the experimental INS data on BSCCO and YBCO. The calculation is based on numerical models for the normal and anomalous Green’s functions fitted to the experimental single-particle spectra. The renormalization is taken into account both in the single-particle Green’s function by means of the self-energy, and in the two-particle correlation function by RPA. Additionally, two other applications of the same approach are briefly sketched: the relation of ARPES to FT-STS, and the nesting properties of Fermi surfaces in two-dimensional charge density wave systems.