Dr
Alessandro Ruggiero
(Brookhaven National Laboratory)
16/04/2007 09:00
Proton acceleration for ADS
Oral presentation
As an alternative to the use of a Superconducting Linac, we
have explored at Brookhaven National Laboratory a
complex made of a pair of Non-Scaling FFAGs for the
acceleration of Ions of Uranium-238 for the production of
Radio-Isotopes and esotic nuclear fragments. The beam power
requirement is 400 kWatt at an energy of 400 MeV/
u. The design of the FFAG accelerators is straightfoward...
Dr
Dejan Trbojevic
(Brookhaven National Laboratory)
16/04/2007 09:30
Proton acceleration for ADS
Oral presentation
A major cost of the Radioactive Ion accelerator is in the
superconducting linac
the present design assumes three superconducting linacs with
stripping foils
between two stages of heavy ion acceleration. The heavy ion
maximum kinetic
energy is assumed to be 400 MeV/u with a total of 400 kW
power for uranium
ion beams. To reduce the cost for the long superconducting
linacs...
Dr
Grahame Rees
(CCLRC)
16/04/2007 10:00
Proton acceleration for ADS
Oral presentation
M.
franck lemuet
(doctoral student)
16/04/2007 11:00
Proton acceleration for ADS
Oral presentation
This paper describes the setting up of ray-tracing tools and
preliminary
beam dynamics studies concerning the electron model
3-5.4463~MeV of
a non-linear, non-scaling proton driver FFAG 3-10~GeV.
Prof.
Stephan TZENOV
(CCLRC Daresbury Laboratory)
16/04/2007 11:30
Afternoon working group session - 4th day
Oral presentation
Based on the synchro-betatron formalism the theory of
accelerated orbits in FFAG
accelerators is developed. Traditional notions like
dispersion, momentum compaction
and slip phase have been introduced with due account of the
reference and accelerated
orbit. Further, some preliminary features of the
longitudinal dynamics have been
pointed out.
Dr
Alessandro Ruggiero
(Brookhaven National Laboratory)
16/04/2007 12:00
Proton acceleration for ADS
Oral presentation
The use of a Non-Scaling FFAG accelerator is here described
for the acceleration of Protons to 1 GeV or more for an
average beam power of 10 MWatt or more. Several modes of
operation are descibed: at the repetition rate of 1 kHz,
10 kHz, and in Continuou Mode. The use of Harmonic Number
Jump method for acceleration is also assumed.
Possible applications for the Proton Driver...
