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1

Sang, Robert Thomas, i n/a. "Superelastic Electron Scattering from Laser Excited States of Sodium". Griffith University. School of Science, 1995. http://www4.gu.edu.au:8080/adt-root/public/adt-QGU20050921.120911.

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This thesis presents the results of a series of experiments in which electrons are superelastically scattered from various laser excited states of sodium. The atoms, once in the optically prepared state, are forced to relax via the superelastic collision with an electron. The rate of detection of superelastically scattered electrons was measured as a function of the laser polarisation which enabled pseudo Stokes parameters to be determined. These pseudo Stokes parameters are functions of both optical pumping parameters and atomic collision parameters. The optical pumping parameters describe the laser-atom interaction and the atomic collision parameters describe the electron-atom collision process. Three different laser excitation mechanisms were used to optically pump the atoms into various excited states. The first of these used a single laser tuned to the 32S 112(F'=2 hyperfine state)-~32P312 transition. The excited atoms underwent a superelastic collision with an electron leaving the atom in the ground state and pseudo Stokes parameters were measured as a function of both scattering angle and incident electron energy. The second superelastic experiment, utilised a folded step excitation mechanism which employed two lasers tuned from the two hypethne states of the 32S112 ground state respectively to the 32P312 excited state. Power broadening effects in the single laser experiment cause the atoms to be optically pumped into the F= 1 hyperfine ground state. The laser powers used were not great enough to power broaden the hyperfine ground states and as such the F'= 1 sublevel effectively acted as a sink. The folded step excitation method enabled the excited state population to be increased so that data at larger scattering angles could be obtained. Stokes parameters from both of these experiments which had an incident energy range of 10eV to 30eV and an angular range of 5°-25° were compared to three current electron-atom scattering theories and previous experimental data. Overall, fair to good agreement was found between theory and experiments for the individual Stokes parameters. Losses of coherence was observed at small scattering angles (50.200) at 20eV and 25eV incident electron energies which were poorly modelled by the three different theories. The third superelastic experiment involved the use of two lasers of specified polarisation to stepwise excite the atoms to the 32D512 excited state. Superelastic collisions with incident electron energies of 20eV from the 32D512-*32P312~312 collision were studied at three different scattering angles and pseudo Stokes parameters for the case where the polarisations of the radiation from the lasers were parallel were measured. The single step and folded step laser-atom interactions for it excitation were modelled using a full quantum electrodynamical treatment so that the optical pumping parameters from the single and folded step experiments could be investigated. Equations of motion were derived in the Heisenberg picture and it is shown that for the single laser case 59 equations of motion are required to fully model the interaction and for the folded step ease 78 equations of motion are required. The results of calculations demonstrated that the optical pumping parameters were sensitive to laser intensity, laser detuning and the Doppler width of the atomic beam. The theoretical quantum electrodynamical calculation results were in good agreement with the experimental results.
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2

Arndt, Phillip Todd. "PROBING THE EXCITED ROVIBRATIONAL STATES OF SODIUM DIMERS". Miami University / OhioLINK, 2015. http://rave.ohiolink.edu/etdc/view?acc_num=miami1438641133.

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3

Scielzo, Nicholas David. "Measurement of the beta-neutrino correlation in laser trapped {sup 21}Na". Berkeley, Calif. : Oak Ridge, Tenn. : Lawrence Berkeley National Laboratory ; distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy, 2003. http://www.osti.gov/servlets/purl/821455-YDxgQ2/native/.

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Thesis (Ph.D.); Submitted to Univ. of California, Berkeley, CA (US); 1 Jun 2003.
Published through the Information Bridge: DOE Scientific and Technical Information. "LBNL--54350" Scielzo, Nicholas David. USDOE Director. Office of Science. Nuclear Physics (US) 06/01/2003. Report is also available in paper and microfiche from NTIS.
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4

Thomson, Robin Graham Crawford. "Laser spectroscopy of excited states in indium-mercury vapour mixtures". Thesis, Queen's University Belfast, 1991. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.334682.

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5

Weragoda, Geethika K. "Excited state intramolecular proton transfer (ESIPT) and trans-cis isomerization on the triplet excited states". University of Cincinnati / OhioLINK, 2015. http://rave.ohiolink.edu/etdc/view?acc_num=ucin1439296134.

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6

Chawla, Gunjit. "Study of long range potentials in excited states of diatomic sodium using modulated gain spectroscopy". Thesis, Massachusetts Institute of Technology, 1985. http://hdl.handle.net/1721.1/15297.

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Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Chemistry, 1985.
MICROFICHE COPY AVAILABLE IN ARCHIVES AND SCIENCE.
Includes bibliographical references.
by Gunjit Chawla.
Ph.D.
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7

Bohl, Elvira. "Investigating excited electronic states in fullerenes and polycyclic aromatic hydrocarbons using Femtosecond Laser Photoelectron spectrometry". Thesis, University of Edinburgh, 2016. http://hdl.handle.net/1842/25979.

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Fullerenes have highly excited electronic states with interesting properties for possible wide ranging applications including in electronics. These highly excited, Rydberg-like states, so-called superatom molecular orbitals (SAMOs), are diffuse low-angular momenta states with molecular orbitals centred on the hollow fullerene core. The SAMOs can be detected by femtosecond photoelectron spectroscopy (PES) and characterised by photoelectron angular distributions (PADs) combined with time-dependent density functional theory (TD-DFT) calculations. The photoelectron spectra of C60 and C70 show a peak structure below kinetic energies corresponding to the photon energy, superimposed on a thermal electron background. This peak structure was assigned to one-photon ionisation of the SAMO states based on PAD and TD-DFT. In this thesis, studies of the fullerene species C82 and Sc3N@C80 revealed PES and PAD with similar features to C60 and C70. The SAMO peaks became less prominent compared to the thermal electron background for increasing molecular size and decreasing symmetry, and were almost absent for the endohedral species. To provide more information about the influence of encapsulated atoms in the fullerene cage on the SAMO states, experiments on Li@C60 have been carried out. A lower thermal electron emission temperature and a splitting of the SAMO peaks has been observed for Li@C60 compared to C60. Nevertheless the binding energies are remarkably similar in all investigated fullerenes, which is important for any applications. Since the binding energies are about the same, but the ionisation potentials of the fullerenes are different, the excitation energy to the SAMOs scales with the ionisation energy. The reasons for the well-pronounced peak structure of the SAMO states in the PES of C60 could be explained by the similarity of the SAMOs to Rydberg states along with the higher photoionisation probabilities compared to valence states which were modelled by Benoît Mignolet and Françoise Remacle. As the SAMOs are highly excited electronic states, like Rydberg states, the potential energy surface of the neutral molecule and the ionised molecule are similar. Therefore the vibrational energy is conserved in the molecule during the photoionisation on the femtosecond time scale. The TD-DFT calculations on C60, carried out by Benoît Mignolet and Françoise Remacle, revealed the photoionisation probabilities of the SAMOs to be at least three orders of magnitude higher than for non-SAMOs for the applied experimental conditions. To test the prediction of the model, the relative photoionisation probabilities of the s-SAMO to p-SAMO and the s-SAMO to d-SAMO were obtained experimentally from the PES at various photon energies (2-3.5 eV) within this work. The analysis indicates remarkable agreement between the experiment and the theoretical values. Further quantum chemical calculations on a series of polycyclic aromatic hydrocarbons (PAHs) were carried out within this thesis, which revealed similar Rydberg-like molecular orbitals in analogy to the SAMOs in fullerenes. The first series included benzene, naphthalene, anthracene, tetracene, pentacene and hexacene. The second series consisted of phenanthrene, pyrene and coronene. Finally, the third series covered cubane, adamantane and dodecahedral C20. All modelled molecules showed diffuse, excited electronic states similar to the SAMOs. Within each series the binding energies of these states decrease with increasing molecular size as well as the ionisation energies, except for the 3rd series. A comparison between all series shows that the binding energies of the states for the 3rd series (the 3-D series) are slightly higher than for the 1st and 2nd series in relation to similar molecular size. The results of the coronene calculations are compared to experimental photoelectron spectra and are shown to be in good agreement with the experiments.
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8

Dickson, Nicole Marie. "Exploration of the Excited States of Organic Molecules and Metal Complexes Using Ultrafast Laser Spectroscopy". The Ohio State University, 2011. http://rave.ohiolink.edu/etdc/view?acc_num=osu1306872674.

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9

Zhang, Yunlong. "Ultrafast Time Resolved and Computational Studies of Diazo and Diazirine Excited States, and of Carbenes". The Ohio State University, 2010. http://rave.ohiolink.edu/etdc/view?acc_num=osu1267479070.

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10

Pant, Lok Raj. "The Radiative Lifetime Measurement on 61Σ+g (v = 9, 10, 11, J = 31) Excited States of Molecular Sodium Using Time Resolved High Resolution Doubled Resonance Spectroscopy". Miami University / OhioLINK, 2021. http://rave.ohiolink.edu/etdc/view?acc_num=miami1626966676896514.

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11

Wang, Jin. "Ultrafast studies of reactive intermediates". Columbus, Ohio : Ohio State University, 2007. http://rave.ohiolink.edu/etdc/view?acc%5Fnum=osu1196155202.

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12

JAGOSICH, FABIO H. "Estudos dos processos de transferência de energia dos íons de Ersup(3+) e Hosup(3+) para os íons de Ndsup(3+), Tbsup(3+) e Eusup(3+) no cristal de LiYFsub(4) e no vidro ZBLAN para a otimização de meios laser ativos que operam na região de 3 microns". reponame:Repositório Institucional do IPEN, 2006. http://repositorio.ipen.br:8080/xmlui/handle/123456789/11432.

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Made available in DSpace on 2014-10-09T12:51:51Z (GMT). No. of bitstreams: 0
Made available in DSpace on 2014-10-09T14:06:32Z (GMT). No. of bitstreams: 0
Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)
Tese (Doutoramento)
IPEN/T
Instituto de Pesquisas Energeticas e Nucleares - IPEN/CNEN-SP
FAPESP:00/11446-0
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13

Eliah, Dawod Ibrahim. "Structural integrity of highly ionized peptides". Thesis, Uppsala universitet, Molekyl- och kondenserade materiens fysik, 2019. http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-387886.

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In order to understand the behaviour and function of proteins, their three dimensional structure needs to be known. Determination of macro-molecules’ structures is done using X-ray diffraction or electron microscopy, where the resulting diffraction pattern is used for molecular reconstruction. These methods are however limited by radiation damage.The aim of this work is to study radiation damage of peptides in proteins using computer simulations. Increased understanding of the atomic and molecular dynamics can contribute to an improvement of the method ofimaging biological molecules. To be able to describe the processes that take place as accurately as possible, the problem must treated quantum mechanically.Thus, the simulations are performed with molecular dynamics based on first principles. In order to capture the dynamics of the excited states of the molecule when exposed to X-rays, time-dependent density functional theory with delta self-consistent field is used. These simulations are compared to ground state simulations. The results of the thesis conclude that the excited and ground state simulations result in differences in the dynamics, which are most pronounced for lager molecules.
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14

Garnier, Nicolas. "Spectroscopie dans l'état excité des ions terres-rares Nd3+ et Tm3+ et fonctionnement laser multilongueur d'onde du YAG : Nd3+". Saint-Etienne, 1997. http://www.theses.fr/1997STET4020.

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L'ensemble des travaux présentés dans cette thèse a été réalisé dans le cadre du Groupement de recherche matériaux lasers (GDR CNRS n°1148, thème : critère de qualité). Il est issu d'une collaboration entre le Laboratoire Traitement du signal et instrumentation, le Laboratoire Physico-chimie des matériaux luminescents et les entreprises CRISMATEC et BM industrie. Ces travaux ont conduit à la mise en oeuvre de différentes techniques expérimentales permettant la compréhension de divers processus se manifestant par une limitation de l'effet laser dans les cristaux de YAG : Nd3+ (Y3al 5o 1 2 : Nd3+) et YLF : Nd3+ (YLIF4 : Nd3+). Le premier aspect de ces processus est lié à l'ion dopant, ce sont des processus intrinsèques tels que l'absorption dans l'état excité et l'addition de photon par transfert d'énergie conduisant à un dépeuplement du niveau métastable émetteur dans l'infrarouge. Nous avons mis au point différentes expériences à deux faisceaux laser synchronisés (pompe, sonde) permettant l'étude des transitions dans l'état excité tant du point de vue spectral que des sections efficaces. Dans le cas du YLF : Nd3+, ces techniques ont permis la mise en évidence d'un double processus d'addition de photons par transfert d'énergie conduisant à des émissions visibles et ultraviolettes faisant suite à un pompage infrarouge ainsi qu'une double absorption dans l'état excité autour de la longueur d'onde laser (1. 05 m). Nous avons par ailleurs appliqué ces techniques à l'étude de transitions d'absorption dans l'état excité intervenant dans le processus d'avalanche de photons dans l'ion thulium pour différentes matrices (Y3al 5o 1 2, YALO3 et Y2O3). Le second aspect de ces travaux, appliqué au YAG : Nd3+, nous a conduit à envisager l'intervention d'un processus extrinsèque à l'ion dopant lié à la formation de centres colorés après pompage optique. On observe ainsi, après pompage, la diminution d'une bande d'absorption autour de 250 nm n'appartenant pas à l'ion Nd3+, l'apparition d'une bande d'absorption s'étendant depuis le visible jusqu'à l'infrarouge conduisant ainsi à l'augmentation de l'absorption résiduelle à la longueur d'onde laser (1. 064 m), cette absorption résiduelle étant mesurée par une technique interférométrique spécialement développée à cet effet. Le processus envisagé est le changement de Valence d'une impureté (probablement du fer) par piégeage d'un électron libéré dans la matrice YAG sous l'effet du rayonnement ultraviolet des flashes de pompage, processus partiellement réversible, avec la création de centres absorbants sous forte intensité de pompage (phénomène à deux photons) et annihilation (blanchiment) de ces centres sous faible intensité de pompage (phénomène à un photon). L'hypothèse actuelle, quant à la nature de ces centres, serait liée au processus d'oxydo-réduction : Fe3+ + e- Fe2+. Nous avons observé que ces centres colorés avaient une influence sur l'énergie extraite et sur la thermique des barreaux en fonctionnement laser
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15

Chien-YuKuo i 郭健裕. "Laser Spectroscopic Studies of the A1Σ+ and 21II States on Higher Excited Levels in Gaseous Sodium Deuteride". Thesis, 2018. http://ndltd.ncl.edu.tw/handle/95ke6n.

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16

Miles, Randall D. "Theoretical studies of highly excited triplet states of NaK /". Diss., 2005. http://gateway.proquest.com/openurl?url_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:dissertation&res_dat=xri:pqdiss&rft_dat=xri:pqdiss:3188499.

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17

Wilkins, Angela D. "Theoretical studies of highly excited triplet states of sodium-potassium". 2007. http://gateway.proquest.com/openurl?url_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:dissertation&res_dat=xri:pqdiss&rft_dat=xri:pqdiss:3285756.

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18

Li, Yufei. "Electron scattering from atoms in the ground state or laser-excited states". 1996. http://hdl.handle.net/1993/19242.

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19

Chen, Hsien-Tsun, i 陳羨尊. "Influence of excited states and temperature effects on quantum-dot laser properties–modeling and analysis". Thesis, 2004. http://ndltd.ncl.edu.tw/handle/94670281180424140038.

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碩士
國立臺灣大學
電子工程學研究所
92
A set of coupled rate equations is applied to analyze quantum-dot laser properties. Except for the inhomogeneous broadening effect due to the quantum-dot size fluctuation, and the homogeneous broadening effect, the influences of excited states and temperature effects are also taken into account. At room temperature, the threshold current density and lasing wavelength as a function of loss are calculated. The conditions for a smooth or step-like change in the lasing wavelength are described and are provided for the optimum design of laser cavity lengths. These would help us to avoid lasing via the excited-state due to short laser cavities. Furthermore, three different mechanisms of temperature effects on quantum-dot laser threshold, i.e. homogeneous broadening effect, carrier capture time and carrier thermal escape from quantum dots, are investigated in details to show their individual influence on laser threshold behavior. The unique negative characteristic temperature phenomenon of quantum-dot lasers is therefore clarified. Not only the thermal equilibrium distribution of carriers among quantum dots, but also the interplay of carrier capture time and homogeneous broadening will cause the negative characteristic temperature phenomenon.
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20

Philippson, Jeffrey. "Experimental and Theoretical Studies of Highly-Excited Molecules at a Wide Range of Internuclear Distances". Thesis, 2012. http://hdl.handle.net/1974/6990.

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Experimental and theoretical investigations of highly-excited molecules are presented that advance the current state of knowledge of intramolecular interactions in highly-excited molecular states. A quantitative analysis of intramolecular interactions in excited hydrogen fluoride is presented, in which the rotational levels of the B singlet-Sigma+, v = 29 vibronic level are shown to mix with the corresponding e-parity components of the C singlet-Pi, v = 0 level. Extrapolating the experimentally-derived mixing parameter to the unperturbed limit reveals an unperturbed value of the aF hyperfine parameter of 4132(25) MHz. Coupling energies between the ion-pair curve and long-range asymptotes of covalent states are calculated for a large number of alkali–alkali collision channels, revealing the dependence on the internuclear distance at which the crossing takes place and forming a foundational step for the calculation of cross-sections and rate coefficients for different charge-exchange and other processes. To advance the experimental investigation of these systems, optical instrumentation and associated control systems have been designed and constructed for cooling and trapping lithium in preparation for experimental studies of cold-collisions that will be informed by, and ultimately a test of, some of these calculated ionic–covalent coupling energies. A novel scheme for systematic optimization of peak-locking has been developed and implemented, providing a rigorous assessment of the optimal experimental parameters. A side-of-filter offset-locking scheme was implemented, characterizing and correcting for a previously unexplained offset in the error-signal. A novel calibrated polarimetry scheme is demonstrated, correcting for the primary sources of uncertainty relating to manufacturing tolerances and experimental errors. The calibrated set of polarization measurements is used to examine the purity of the optical polarization state in the light sources to be used for trapping lithium.
Thesis (Ph.D, Physics, Engineering Physics and Astronomy) -- Queen's University, 2012-01-31 11:30:22.479
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21

Breitbach, Thomas H. [Verfasser]. "Laser magnetic resonance applied to excited states of iodine and to the fine structure transition in the electronic groundstate of iodine monoxide / von Thomas H. Breitbach". 2002. http://d-nb.info/967214106/34.

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22

Clarkin, OWEN. "Chemical Reaction Dynamics at the Statistical Ensemble and Molecular Frame Limits". Thesis, 2012. http://hdl.handle.net/1974/7456.

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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
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