Spallation Physics And The Ads Target Design

dc.creatorMongelli S.T.
dc.creatorMaiorino J.R.
dc.creatorAnefalos S.
dc.creatorDeppman A.
dc.creatorCarluccio T.
dc.date2005
dc.date2015-06-26T14:06:55Z
dc.date2015-11-26T15:40:46Z
dc.date2015-06-26T14:06:55Z
dc.date2015-11-26T15:40:46Z
dc.date.accessioned2018-03-28T22:49:14Z
dc.date.available2018-03-28T22:49:14Z
dc.identifier
dc.identifierBrazilian Journal Of Physics. , v. 35, n. 3 B, p. 894 - 897, 2005.
dc.identifier1039733
dc.identifier
dc.identifierhttp://www.scopus.com/inward/record.url?eid=2-s2.0-31444444633&partnerID=40&md5=997cca11cf3c2914f2627451bfb18a7f
dc.identifierhttp://www.repositorio.unicamp.br/handle/REPOSIP/93243
dc.identifierhttp://repositorio.unicamp.br/jspui/handle/REPOSIP/93243
dc.identifier2-s2.0-31444444633
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1264452
dc.descriptionThis paper reviews the physics of the spallation which is a nuclear reaction in which a particle (e.g. proton) interacts with a nucleus. Given to the high energy of the incident proton, in a first stage it interacts with the individual nucleons in an intranuclear cascade which leads to the emission of secondary particles (neutrons, protons, mesons, etc.). In a secondary stage the nucleus is left in an excited state and can de-excite by evaporation and/or fission. Given to the high number of secondary neutrons produced (∼30 n/p for proton energy of 1 GeV), this reaction can be used as a source of neutrons, for example for ADS systems as external source to drive the sub critical reactor. The main codes used in the ADS target design and an example on the utilization of one of these codes (the LAHET code) for typical ADS target are given.
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dc.languageen
dc.publisher
dc.relationBrazilian Journal of Physics
dc.rightsfechado
dc.sourceScopus
dc.titleSpallation Physics And The Ads Target Design
dc.typeActas de congresos


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