65 research outputs found

    Stopping of energetic sulfur and bromine ions in dense hydrogen plasma

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    The concepts of communicative space, media sphere and public sphere are sometimes used like synonyms one of the other. However, according to us, they are three different concepts: public sphere and media sphere are two distinct spaces symbolic systems which, both, are anchored in communicative spac

    INVESTIGATION OF THE TRANSMISSION AND STOPPING OF LIGHT IONS PASSING THROUGH A PLASMA TARGET

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    Transmission and energy losses of 2 MeV/u Carbon and Sulphur beams passing through a plasma target, have been extensively investigated. A hydrogen plasma ignited by an electrical discharge was coupled to the Orsay Tandem beam accelerator. Fluctuations in beam transmission have been observed and attributed to a magnetic focusing effect generated during the plasma evolution. Energy loss measurements were performed on the basis of time of flight techniques and indicate an enhanced stopping power of the plasma relative to its cold matter equivalent

    Determination of the parameters of a plasma JET generated by a capillary discharge

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    A pulsed capillary discharge has been the subject of various experimental and theoretical studies. A jet of copperhydrogen plasma with a cylindrical symmetry has been developed as a light source for spectroscopic measurements. The electron density of the plasma was obtained by using the HÎČ spectral line of the hydrogen component plasma. The electron temperature was determined by means of the Boltzmann method applied to the copper profiles emitted by the plasma jet. The copper and hydrogen lines were broadened principally by the Stark effect. The electron density of the plasma was found to be about 2×1017 cm–3 and the electron temperature about 20000K

    PLASMA DIAGNOSTICS IN THE HEAVY ION BEAM-DENSE PLASMA INTERACTION EXPERIMENT AT ORSAY

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    On décrit la source plasma utilisée lors d'expériences d'interaction entre un faisceau d'ions lourds (C4+ ou S7+) à une énergie de 2 Mev par nucléon et un plasma. Le but était de mesurer la perte d'énergie des ions dans le plasma. Les méthodes de diagnostic du plasma par spectroscopie d'émission, par interférométrie laser et par absorption laser à deux longueurs d'ondes sont présentées ainsi que les résultats.We describe the plasma source used for interaction experiments between heavy ion beams (C4+ S7+) at energies of 2 Mev per nucleon and a plasma. The purpose of these experiments was to measure the ion energy loss in the plasma. The plasma diagnostics methods by emission spectroscopy, by laser interferometry and two-wavelength laser absorption are presented as well as the results

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    Abstract A pulsed capillary discharge has been the subject of various experimental and theoretical studies. A jet of copperhydrogen plasma with a cylindrical symmetry has been developed as a light source for spectroscopic measurements. The electron density of the plasma was obtained by using the H ÎČ spectral line of the hydrogen component plasma. The electron temperature was determined by means of the Boltzmann method applied to the copper profiles emitted by the plasma jet. The copper and hydrogen lines were broadened principally by the Stark effect. The electron density of the plasma was found to be about 2×10 17 cm -3 and the electron temperature about 20000K

    Energy loss of heavy ions in a plasma target

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    The public: definitions and perceptions The public is a difficult concept to grasp. It exhibits contradictory meanings: a collective abstract entity that is based on a “togetherness” founded on the exercise of reason; a cumulative heterogeneous phenomenon formed into an audience by certain kinds of specialised proceedings; or, another possibility, the driving force of action aimed at modifying something of the individuals that one wishes to reach. In all these cases, it is not a self-defined social collective. However, we constantly speak of the public's point of view. Can we really contemplate a situation in which the public could be thought of as a potential enunciator of a point of view? Or at least as an interlocutor in communication with the institutions of which it is the public? This article describes the division between the status of the members of the public engaged in interpersonal communications with representatives of the institution and the status of the public as a collective abstract entity engaged in a “communication” with the institution

    Caractérisation du seuil d'ablation des parois dans les sources de rayonnement EUV par décharge capillaire

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    Les sources de rayonnement ExtrĂȘme Ultraviolet (EUV) par dĂ©charge capillaire connaissent un intĂ©rĂȘt de plus en plus considĂ©rable pour de nombreuses applications scientifiques et technologiques. Au GREMI, nous Ă©tudions le fonctionnement des sources de rayonnement EUV Ă©mettant Ă  13.5 nm pouvant rĂ©pondre Ă  certaines applications liĂ©es Ă  la nouvelle gĂ©nĂ©ration de la lithographie. Ces sources pulsĂ©es, nommĂ©es CAPELLA, ATλ\lambda AS et PROXIMA, sont basĂ©es sur une dĂ©charge capillaire en flux de gaz. Ce type de dĂ©charge produit un plasma chaud, dense et fortement ionisĂ© Ă©mettant dans la gamme spectrale de l'EUV. En effet, les tempĂ©ratures Ă©lectroniques peuvent atteindre des dizaines d'Ă©lectronvolts et les densitĂ©s Ă©lectroniques sont de l'ordre de 101710^{17} cm-3^{\hbox{-}3}. Les Ă©changes thermiques entre le plasma ainsi crĂ©Ă© et les parois du capillaire peuvent ĂȘtre suffisamment important pour que les parois du capillaire soient ablatĂ©es. Cette ablation peut ĂȘtre plus ou moins importante selon la densitĂ© d'Ă©nergie injectĂ©e dans le capillaire. Des mesures spectroscopiques du plasma Ă©metteur dans les gammes spectrales de l'UV et l'EUV ont montrĂ© la prĂ©sence d'un seuil d'ablation situĂ© autour de Ă  350 J.cm-3^{\hbox{-}3}. Nous utilisons un modĂšle thermique prĂ©sentĂ© [1] pour modĂ©liser l'Ă©volution temporelle de la tempĂ©rature des parois du capillaire. Le seuil peut ĂȘtre ainsi estimĂ©. Les rĂ©sultats expĂ©rimentaux obtenus Ă  partir de nos mesures spectroscopiques sont comparĂ©s ensuite aux rĂ©sultats numĂ©riques
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