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Träfflista för sökning "WFRF:(Broggi F) srt2:(2007-2009)"

Sökning: WFRF:(Broggi F) > (2007-2009)

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1.
  • Battistoni, G., et al. (författare)
  • The FLUKA code and its use in hadron therapy
  • 2008
  • Ingår i: Nuovo Cimento della Societa Italiana di Fisica C. - Italian Physical Society. - 1124-1896. ; 31:1, s. 69-75
  • Tidskriftsartikel (refereegranskat)abstract
    • FLUKA is a multipurpose Monte Carto code describing transport and interaction with matter of a, large variety of particles over a wide energy range ill complex geometries. FLUKA is successfully applied ill several fields, including, but not only particle physics, cosmic-ray physics, dosimetry, radioprotection, hadron therapy. space radiation, accelerator design and neutronics. Here we briefly review recent model developments and provide examples of applications to hadron therapy, including calculation of physical and biological dose for comparison with analytical treatment planning engines as well as beta(+)-activation for therapy monitoring by means of positron emission tomography.
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2.
  • Hoa, C., et al. (författare)
  • Parametric study of heat deposition from collision debris into the insertion superconducting magnets for the LHC luminosity upgrade
  • 2007
  • Ingår i: IEEE Particle Accelerator Conference, PAC07. - 9781424409167 ; , s. 323-325
  • Konferensbidrag (refereegranskat)abstract
    • With a new geometry in a higher luminosity environment, the power deposition in the superconducting magnets becomes a critical aspect to analyze and to integrate in the insertion design. In this paper, we quantify the power deposited in magnets insertion at variable positions from the interaction point (IP). A fine characterization of the debris due to the proton-proton collisions at 7 TeV, shows that the energetic particles in the very forward direction give rise to non intuitive dependences of the impacting energy on the magnet front face and inner surface. The power deposition does not vary significantly with the distance to the interaction point, because of counterbalancing effects of different contributions to power deposition. We have found out that peak power density in the magnet insertion does not vary significantly with or without the Target Absorber Secondaries (TAS) protection.
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