THIAGO CARLUCCIO
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Resumo IPEN-doc 15426 The utilization of MCNP code to simulate the yalina booster facility using the ADS library2006 - CARLUCCIO, T.; MAIORINO, J.R.; SANTOS, A. dosArtigo IPEN-doc 10648 A review of models and codes for neutron source (spallation) calculation for ADS application2005 - MAIORINO, J.R.; MONGELLI, S.T.; SANTOS, A.; ANEFALOS, S.; DEPPMAN, A.; CARLUCCIO, T.Artigo IPEN-doc 18829 The calculation of the YALINA BOOSTER zero power sub critical assembly driven by external neutron sources: Brazilian contribution2010 - CARLUCCIO, THIAGO; ROSSI, PEDRO C.R.; MAIORINO, JOSE R.Artigo IPEN-doc 12170 Reactor physics calculations for a sub critical core of the IPEN-MB-01 driven by an external neutron source2007 - ANTUNES, A.; CARLUCCIO, THIAGO; MENDONCA, A.G.; SANTOS, ADIMIR dos; MAIORINO, JOSE R.Artigo IPEN-doc 15473 The utilization of a compact neutron generator to drive a sub critical core of the IPEN-MB-01 facility for reactor physics experiments2006 - MAIORINO, J.R.; LEUNG, K.; SANTOS, A.; BITELLI, U.; FILHO, T.M.; CARLUCCIO, T.Artigo IPEN-doc 12092 The participation of IPEN in the IAEA coordinated research projects on accelerator driven systems2007 - MAIORINO, JOSE R.; SANTOS, A.; CARLUCCIO, T.; ROSSI, P.C.R.; ANTUNES, A.; OLIVEIRA, F. de; LEE, S.M.Artigo IPEN-doc 10932 Spallation physics and the ADS target design2005 - MONGELLI, S.T.; MAIORINO, J.R.; ANEFALOS, S.; DEPPMAN, A.; CARLUCCIO, T.This 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.