The Quark Gluon Plasma (QGP) is a form of matter in which quarks and gluons are deconfined, and was suggested to be formed in high-energy heavy-ion collisions. Since the discovery of high-pT hadron suppression in central Au+Au collisions at the Relativistic Heavy Ion Collider (RHIC), and the related discovery of the quenching of the away-side jet in these collisions, the role of jets as key probes of the QGP was re-affirmed. The Solenoidal Tracker At RHIC (STAR) detector system, which is suited for jet studies because of its large solid-angle coverage, has produced a number of interesting jet measurements in recent years, including gamma-jet measurements, attempts at full heavy-ion jet reconstruction, and two-dimensional correlations. A long-range correlation in pseudorapidity (the ?Ridge?) was studied (with statistical significance) out to pT^trig. <? 7 GeV /c and was assumed to have an integrated yield independent of pT^trig. Further studies out to higher pT were limited by the minimum biased statistics taken in Run 4 (2004) with STAR. This work presents results of a ridge analysis with (non-reconstructed) pi0s and direct-gamma-rich triggers out to ?13.5 GeV /c in pT^trig. Using triggered data from Run 7 (2007) and Run 10 (2010) Au+Au collisions detected with STAR. Preliminary results seem to indicate that the ridge yield decreases with pT^trig., and that the ridge yield for direct-?-rich triggers is consistent with zero.

Thesis (Ph.D.)--York University, 2007. Graduate Programme in Chemistry. / Typescript. Includes bibliographical references. Also available on the Internet. MODE OF ACCESS via web browser by entering the following URL: http://gateway.proquest.com/openurl?url_ver=Z39.88-2004&res_dat=xri:pqdiss&rft_val_fmt=info:ofi/fmt:kev:mtx:dissertation&rft_dat=xri:pqdiss:NR39012

Inelastic collisions between dipolar molecules, assumed to be trapped in a static electric field at cold (> 10−3K) temperatures, are investigated and compared with elastic collisions. For molecules with a Λ-doublet energy-level structure, a dipole moment arises because of the existence of two nearly degenerate states of opposite parity, and the collision of two such dipoles can be solved entirely analytically in the energy range of interest. Cross sections and rate constants are found to satisfy simple, universal formulas. In contrast, for molecules in a Σ electronic ground state, the static electric field induces a dipole moment in one of three rotational sublevels. Collisions between two rotor dipoles are calculated numerically; the results scale simply with molecule mass, rotational constant, dipole moment, and field strength. It might be expected that any particles interacting only under the influence of the dipole-dipole interaction would show similar behavior; however, the most important and general result of this research is that at cold temperatures inelastic rate constants and cross sections for dipoles depend strongly upon the internal structure of the molecules. The most prominent difference between the Λ-doublet and rotor molecules is variation of the inelastic cross section with applied field strength. For Λ-doublet dipoles, cross sections decrease with increasing field strength. For rotor dipoles, cross sections increase proportionally with the square of field strength. Furthermore, the rate constants of the two types of molecules depend very differently on the angular orientations of the dipoles in the electric field.

Thesis (Ph. D.)--University of Canterbury, 2009. / Typescript (photocopy). Includes bibliographical references (p. 172-183). Also available via the World Wide Web.

Neste trabalho implementamos um programa computacional capaz de descrever passo-a-passo o processo de colisão entre dois átomos confinados numa armadilha magneto-óptica em regime frio. Para isso utilizamos o formalismo de Wigner, que é uma formulação equivalente à mecânica quântica, para encontrar-mos uma aproximação quase-clássica para as equações que descrevem o sistema. Este formalismo permite-nos separar os graus de liberdade externos dos átomos colidentes, que podem ser tratados de maneira quase-clássica, dos graus internos de liberdade, os quais não tem contraparte clássica e, portanto, são tratados quanticamente / In this work we implement a computer program that describes, step by step, the collision process between two atoms confined in a magneto-optical trap in the cold regime. Here we utilize the Wigner-function theory, which is a formulation of quantum mechanics in terms of a phase space, to find a quasi-classical approx¬imation of the dynamical equations that govern the time evolution of the system. This approach allows us to describe the dynamics in terms of external and internal degrees of freedom. The former degrees of freedom are treated quasi-classically, while the latter, because they do not have a classical counterpart, are treated quan¬tum mechanically

Les systèmes composés d'atomes et d'ions ultrafroids ont étés un sujet d'intérêt pour les physiciens atomiques et, plus récemment, pour la communauté des ions froids (simulation et calcul quantique avec des ions piégés). Ils sont considéré la possibilité d'utiliser un gaz d'atomes ultrafroids pour refroidir sympathiquement les ions car la modulation intrinsèque du mouvement, le micromouvement, représente une source de décohérence dans les applications des ions froids. L'intérêt envers ce système mixte est aussi motivé par l'étude de la physique d'impuretés et par une meilleure compréhension des réactions entre espèces ioniques et neutre ayant pour but la création d'ions moléculaires. Cette thèse a pour objectif d'étudier les effets du micromouvement dans les collisions atome-ion. Nous traitons au préalable les collisions à 1D d'une particule dans un piège harmonique (un ion) et d'un particule libre (une atome) en utilisant différentes approches numériques. Ce système est intéressant en soi en raison de la dimensionnalité mixte 0D-1D. Le potentiel atome-ion est modélisé par une interaction à portée nulle tout au cours de ce travail. Par la suite, nous traitons un problème similaire mais dans le cas d'une particule dans un piège harmonique décrivant un piège de Paul. Enfin, nous généralisons l'étude du micromouvement à un système modèle 3D avec un ion dans un piège de Paul sphérique 3D et un atome lourd au centre du piège. Nous discutons de l'influence du micromouvement en vue d'applications potentielles de ce système telle que la porte logique de phase. / Ultracold atom-ion systems have been a topic of interest for atomic physicists studying chemical reactions and since recently, the cold ion community (ion trap quantum computation and simulation). They have been looking at the possibility of using an ultracold atom gas to sympathetically cool ions since intrinsic motional modulation i.e micromotion is an inherent cause of decoherence in coherent applications of cold ions. Interest is also piqued by the possibility of using this hybrid system for studying impurity physics and to better understand ion-neutral reactions aimed at creation of molecular ions. In this thesis, we aim to study the effect of ion micromotion in atom-ion collision. As a prelude, we treat the 1D collision of a particle in a harmonic trap (ion) and a free particle (atom) using different numerical schemes. This system is of interest in its own right due to the mixed 0D-1D dimensionality. Atom-ion potential is simplified to a zero range potential all through out the work. Next we deal with a similar problem but with the trapped particle in a time dependent harmonic trap identical to an ion Paul trap. Finally we extend the study of micromotion to a model system in 3D with an ion in a 3D spherical Paul trap and a heavy atom at the trap centre. We discuss the effect micromotion has on potential applications of such a system, like a quantum phase gate.

In this thesis a production of J/ψ meson in pp and heavy-ion collisions was investigated. A comparison between Monte Carlo generator and data by ATLAS experiment at CERN was done. PYTHIA version 8.2 was chosen for the Monte Carlo generator. In the first part, comparisons of several configurations of PYTHIA were used to establish the best matching of the Monte Carlo to the data using collisions with centre-of-mass energy of 7 TeV. Choice of parton distribution functions was found not to be important, while presence or absence of initial and final state radiation were proven to have an important impact on the result. In the second part, correlation of J/ψ meson and the jet production was quantified. Anti-kt algorithm with R = 0.4 was used to reconstruct jets. Pairs of muons were used to identify J/ψ meson candidates. Only less than 10% of J/ψ mesons were found to be associated with jets. 1

OBJECTIVES: To compare morbidity and mortality between pediatric victims of motor vehicle collisions (MVC) who were unrestrained to those restrained and to describe compliance with child restraint usage in our population. MATERIALS AND METHODS: A retrospective consecutive chart review study was performed on MVC victims 14 years old and younger who presented to our academic, level 1 trauma emergency department in 2003. Each patient's emergency department and hospital course was reviewed and data were collected. Odds ratios (ORs) were calculated for unrestrained children with respect to restrained children for fractures; intraabdominal injuries, intrathoracic injuries, intracranial injuries, admission, surgery, blood transfusion, intubation; and deaths. Hospital charges and length of hospital stay were compared between those unrestrained and restrained. Percentage of children unrestrained was determined. RESULTS: Of 336 patients, 81 (24%) were unrestrained. Mean hospital stay for unrestrained children was longer, 1.94 days (95% confidence interval [CI] 0.75-3.12) versus 0.098 days (95% CI 0.02-0.21). Unrestrained victims had higher mean charges, $14,754 (95% CI $7676-$21,831) versus $1996 (95% CI $1207-$2786). Admissions (OR = 14.48, 95% CI 5.91-38.63), fractures (OR = 5.85, 95% CI 2.13-16.89), intraabdominal injuries (OR = 20.16, 95% CI 2.36-930.68), and intrathoracic injuries (OR = 13.09, 95% CI 1.26-647.05) were all more likely in unrestrained patients. No restrained child had intracranial injury, whereas 9/81 (11.11%) of unrestrained did. Odds were higher in unrestrained for surgery [OR = 13.09, 95% CI 3.30-74.33] and transfusion [OR = 27.61, 95% CI 3.56-229.85]. Ten out of 81 (12.35%) of unrestrained children required intubation versus none for restrained. The only 2 mortalities were unrestrained patients. CONCLUSION: Critical injuries and cost of care are higher in unrestrained than restrained children. Improved compliance with child safety restraint in southern Arizona should decrease childhood morbidity and mortality from MVCs.

Les collisions d’ions lourds à haute énergieproduisentunnouvelétatdelamatièreappelé le plasma de quarks et de gluons. Un parton traversant le plasma perds de l’énergie, en atténuant les gerbeshadroniques:c’estl’effetde"jetquenching". La dépendance du jet quenching dans la saveur du parton fournit des contraintes sur les modèles de perte d’énergie. Le déséquilibre d’une paire de jets issus de quarks b est une observable appropriée pour étudier ce phénomène. Cette thèse présente lamesure du déséquilibre en impulsion transverse des jets de b et des jets inclusifs (non-identifiés), dans des collisions PbPb a √sNN = 5.02 TeV, réalisée avecledétecteurCMSauLHCpouruneluminosité intégrée de 404 µb−1. Aucune différence n’est observée dans le jet quenching entre les jets issus de partons légers et lourds. Une analyse des résultats à l’aide d’un modèle simple de perte d’énergie est présentée. / The collisions of heavy ions at high energy produce the new state of matter called the quark gluon plasma. A parton traversing the plasma loses its energy which results in the jet quenching phenomenon. The dependence of the jet quenchingonthepartonflavorprovidesconstraints the models describing energy loss. The imbalance of b-jets is a very suitable observable to study this phenomena. This dissertation presents the measurement of the transverse momentum imbalance of b-jets and inclusive (non-identified) jets in PbPb collisions at √sNN = 5.02 TeV which is performed with the CMS detector at the LHC with total integral luminosity of 404 µb−1. No significant difference in jet quenching between light and heavy flavor jets is observed. The interpretation of results with a simple model of energy loss is performed.

In the course of experiments using uniaxial double alignment channeling to investigate radiation damage in single crystals, an anomalously large ion-scattering yield from the near surface of disordered or simulated disordered solid targets was observed. The chronology of the discovery of this new ion-solid effect and its explanation are presented along with experiments detailing the dependence of the new effect upon ion type and energy, as well as target atomic number and density. Targets included a spectrum of polycrystalline elemental targets in a range Z = 29 to Z = 82. Also, the influence of the effect upon scattering yields from an aligned Au(110) single crystal is demonstrated.