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<dc:title xml:lang="fr">Collisions assistées par laser pour la formation d'antimatière</dc:title>
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<dc:subject xml:lang="fr">GBAR</dc:subject>
<dc:subject xml:lang="fr">Collision assistée par laser</dc:subject>
<dc:subject xml:lang="fr">Antihydrogène</dc:subject>
<dc:subject xml:lang="fr">Positronium</dc:subject>
<dc:subject xml:lang="fr">Section efficace</dc:subject>
<dc:subject xml:lang="fr">Approximation de Born</dc:subject>
<dc:subject xml:lang="fr">États de Volkov</dc:subject>
<dc:subject xml:lang="fr">Théorie des perturbations dépendantes du temps</dc:subject>
<dc:subject xml:lang="en">GBAR</dc:subject>
<dc:subject xml:lang="en">Laser assisted collision</dc:subject>
<dc:subject xml:lang="en">Antihydrogen</dc:subject>
<dc:subject xml:lang="en">Positronium</dc:subject>
<dc:subject xml:lang="en">Cross section</dc:subject>
<dc:subject xml:lang="en">Born approximation</dc:subject>
<dc:subject xml:lang="en">Volkov states</dc:subject>
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<tef:elementdEntree autoriteExterne="027373053" autoriteSource="Sudoc">Antimatière</tef:elementdEntree>
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<dcterms:abstract xml:lang="fr">L’expérience GBAR vise à mesurer la chute libre d’atomes d’antihydrogène ultra-froids (neV). Cela implique de produire des ions d’antihydrogène, obtenus à l’issue de deux réactions d’échange de charge faisant intervenir des antiprotons et des atomes de positronium. Le but de ce travail est d’étudier la possibilité d’augmenter les taux de production d’atomes et d’ions antihydrogène produits, en assistant les deux réactions par laser. Les sections efficaces sont obtenues aux énergies d’antiproton de GBAR (1 - 10keV), en utilisant une approche semi-perturbative proposée par Byron et Joachain. Celle-ci permet de décrire simultanément l’interaction électron-atome (Coulomb Born Approximation ou Continuum Distorted Waves - Final State), l’interaction électron-laser (états de Volkov),et les interactions laser-atomes (premier ordre de la théorie des perturbations dépendantes du temps). L’excitation depuis l’état 1s du positronium par le processus de transition virtuel à un photon est étudiée, en considérant des lasers dont les longueurs d’onde sont proches de 243 nm (raie Lyman-α). Une adaptation de ces lasers est ensuite proposée afin d’exciter les états 3s et 3d (Paschen-β). Les décalages Doppler résultants de la distribution de vitesse du nuage de positronium sont également pris en compte, aux énergies de confinement de 25 meV et 48 meV. Finalement, le nombre d’antiatomes produits est estimé. Comparativement à la situation où les collisions ne sont pas assistées par un laser, les pertes induites par les processus de photo-ionisation et de photo-détachement sont évaluées.</dcterms:abstract>
<dcterms:abstract xml:lang="en">The GBAR experiment aims at measuring the free fall of ultra-cold antihydrogens (neV).This implies the production of antihydrogen ions, which are obtained by two charge exchange reactions involving antiprotons and positronium atoms. The goal of this study is to analyse the possibility to increase the production rates of the antihydrogens and the antihydrogen ions produced, by assisting the two reactions with a laser. The cross sections are obtained in the antiproton energy range of the GBAR experiment (1 - 10 keV), by using a semi-perturbative approach proposed by Byron and Joachain. This method,simultaneously, allows the description of electron-atom interaction (Coulomb Born Approximation or Continuum Distorted Waves - Final State), the electron-laser interaction (Volkov states), and the laser-atom interactions (first order time dependent perturbation theory). The positronium excitation from the 1s state by one-photon virtual transition process is studied, by considering lasers whose wavelengths are around 243 nm (Lyman-αline). It is then proposed to adapt these laser sources in order to excitate 3s and 3d states (Paschen-β). The Doppler shifts resulting from the positronium cloud velocity distribution are taken into account as well, at the confinement energies of 25 meV and 48 meV. Finally,the number of antiparticules produced is estimated. Compared to the case of non-assisted collisions, the losses induced by the photo-ionization and photo-detachment processes are evaluated.</dcterms:abstract>
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