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Synchrocyclotrons

Known as: Synchrocyclotron 
National Institutes of Health

Related topics

Related topics

4 relations

Broader (1)

Cyclotrons
Particle AcceleratorsSynchrotrons

Narrower (1)

Proton synchrotrons

Papers overview

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2017
2017
In Beam PET Acquisition on 75 MeV. $\text {u}^{-1}$ Carbon Beam Using Sampling-Based Read-Out Electronics
Positron Emission Tomography (PET) dedicated to the ion range verification in the context of hadrontherapy treatments, requires a… 
2012
2012
New laser setup for the selective isotope production and investigation in a laser ion source at the IRIS (Investigation of Radioactive Isotopes on Synchrocyclotron) facility.
New laser installation for the resonance ionization spectroscopy in a laser ion source and for rare isotope production has been… 
2010
2010
SYNCHROCYCLOTRON PRELIMINARY DESIGN FOR A DUAL HADRONTHERAPY CENTER
The Italian research foundation TERA has proposed an innovative accelerator solution, called “Cyclinac” [1], dedicated to… 
1991
1991
The narrow proton beam therapy unit at the Svedberg Laboratory in Uppsala
The synchrocyclotron at the The Svedberg Laboratory (TSL) in Uppsala is now reconstructed and can presently operate with fixed… 
Review
1982
Review
1982
In vivo radiobiology of heavy ions.
1971
1971
Status of the Nevis Synchrocyclotron Modification
The Columbia Univ. Nevis Synchrocyclotron Modification should give ∼ 20 μA (time average) of 560 to 570 MeV protons in an… 
1966
1966
Whole-body irradiation of primates with protons of energies to 400 Mev.
The effect of ionizing radiation on man is of vital interest to the space program. To further knowledge of these effects, a study… 
1965
1965
Le faisceau de protons polarisés de 141 MeV du synchrocyclotron d'Orsay. Application à la mesure de la polarisation dans la diffusion élastique p — 12C et p — d
The polarized proton beam from the Orsay synchrocyclotron is described. The protons have an energy of (141 ± 2 MeV) and (61.6 ± 2… 
1962
1962
THE EFFECT OF SHIELDING ON RADIATION PRODUCED BY THE 730-Mev SYNCHROCYCLOTRON AND THE 6.3-Gev PROTON SYNCHROTRON AT THE LAWRENCE RADIATION LABORATORY
Calculation of shielding thickness should be compared with experimental' data obtained with various detectors . Such data are… 
1951
1951
The proton deuteron rf system for the Berkeley Synchrocyclotron.
An rf system is described which allows the acceleration of either 190‐Mev deuterons or 350‐Mev protons in the Berkeley 184‐inch… 
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