Abstract: A facility for producing radioisotopes. The facility includes at least one target holder. The target holder is configured to receive a target that includes a compound to be irradiated with an accelerated particle beam. The facility includes a cyclotron for producing the accelerated particle beam. The cyclotron includes at least one accelerating cavity within which the beam is subjected to a radiofrequency electric field in order to be accelerated and to a magnetic field enabling it to travel through the cavity several times, describing orbits about an axis of the cyclotron. The magnetic field is produced by at least one coil. The at least one target holder is inside the at least one coil as observed along the axis of the cyclotron. The at least one coil does not have symmetry of revolution about the axis.

Abstract: A synchrocyclotron for extracting charged particles accelerated to an extraction energy includes a magnetic unit comprising N valley sectors and N hill sectors, and configured for creating z-component of a main magnetic characterized by a radial tune of the successive orbits. The synchrocyclotron includes a first instability coil unit and a second instability coil unit configured for creating a field bump of amplitude increasing radially. The amplitude of the field bump may be varied to reach the value of the offset amplitude at the average instability onset radius. The offset amplitude may be the minimal amplitude of the field bump at the average instability onset radius required for sufficiently offsetting the center of the orbit of average instability onset radius to generate a resonance instability to extract the beam of charged particle at the average instability onset radius.

Abstract: A synchrocyclotron for extracting charged particles accelerated to an extraction energy includes a magnetic unit comprising N valley sectors and N hill sectors, and configured for creating z-component of a main magnetic characterized by a radial tune of the successive orbits. The synchrocyclotron includes a first instability coil unit and a second instability coil unit configured for creating a field bump of amplitude increasing radially. The amplitude of the field bump may be varied to reach the value of the offset amplitude at the average instability onset radius. The offset amplitude may be the minimal amplitude of the field bump at the average instability onset radius required for sufficiently offsetting the center of the orbit of average instability onset radius to generate a resonance instability to extract the beam of charged particle at the average instability onset radius.

Abstract: A facility for producing radioisotopes, including:—at least one target capable of receiving a compound to be irradiated with a beam of accelerated particles,—a cyclotron for producing the beam of accelerated particles, including at least one accelerating chamber within which the beam is subjected to a radiofrequency electric field in order to be accelerated and to a magnetic field enabling the beam to cross the chamber several times by describing orbits around an axis (Z) of the cyclotron, this magnetic field being produced by at least one coil, and a facility in which the target is inside the coil when same is viewed along the axis (Z) of the cyclotron, the coil not having rotational symmetry about this axis (Z).