ACCELERATING A CYCLOTRON 18 MEV PROTON BEAM BY

ACCELERATING A CYCLOTRON 18 MEV PROTON BEAM BY A SCDTL LINAC Luigi Picardi, Concetta Ronsivalle (ENEA C. R. Frascati, Frascati (Roma)), Paola Panichelli, Giuseppe Prete, Francesco Romano, Gianluca Valentini (SPARKLE S. r. l. , Casarano (Lecce, IT)) Abstract SPARKLE company is setting up in the south of Italy (Casarano) a new cyclotron facility based on a 18 Me. V, 150 u. A IBA Cyclone 18/9. The aim is to create a multidisciplinary research site for the medical applications of accelerators. The main activity will be the production of standard and new radionuclides, by internal targets and one external beam line. Another opposite beam line has been reserved for low current proton irradiations for radiotherapy studies, and a linac booster between 18 and 24 Me. V was designed and built to this end. The beam line, which focuses and matches the beam to the linac, includes a chopping system to synchronize the beam to the pulsed linac and to collect 99% of the beam not synchronous to the linac. The linac uses a 3 GHz SCDTL structure powered by a magnetron modulator system. In the paper we report an overview of the beam line, component design, and tests. SPARKLE FACILITY and SCOPE OF EXPERIMENT The SPARKLE company in south Italy is pursuing the scope of setting up an advanced center for radiopharmaceutical production and research, and for other proton applications in the field of biology and medicine, like radiobiology, radiotherapy and neutron production for BNCT. The line is opposite to the IBA one to be used for solid target irradiation. To this end an IBA Cyclone 18/9 is installed with several output lines one of which is dedicated to radiobiology experiments. the company proposed in 2008 to ENEA to design and follow the construction of a beam line and a small linac to post-accelerate the 18 Me. V proton beam up to at least 24 Me. V, energy at which the penetration depth in tissue is around 6 mm. The success of this energy boosting experiment could lead also to the future setting up of a proton therapy facility in the area. The cyclotron is a CW machine. The beam is packed in about 2. 4 ns pulses, continuously emitted at a frequency of 41. 7 MHz, that is every 24 ns. 1 Beam Dynamics Bunch evolution has been computed Out of 100 m. A CW (average) cyclotron beam, 17 m. A pulsed (17 n. A average) beam exit from linac Only 3 m. A pulsed (3 n. A average) beam is accelerated to 24 Me. V +/- 1 Me. V Output longitudinal phase space (3 ns beam input) The beam should be cleaned with a magnet! Output spectrum A few n. A beam average current is sufficient for radiobiology studies A sweeping magnet paints the beam vertically. A couple of collimators stop the beam except during the zero crossing Power distribution in the collimators Cyclotron beam has an horizontal emittance of 28 pi mm mrad and a vertical emittance of 17 pi mm mrad, at 90% of the beam. These high values by themselves indicate the coupling difficulty since linacs have corresponding values roughly tenfold lower. Status-Equipments THE SCDTL STRUCTURE Beam loss analysis has been carried mainly through by LINAC code (K. Crandall). It requires emittance values for 100% of the beam, that are as high as ex = 42. 17 mm mrad and ey = 25. 52 mm mrad. Beam losses through the line The linac is, on the contrary a pulsed accelerator, active only for about 4. 5 us at max 200 Hz repetition rate. With this duty cyle (roughly 0. 001), almost all the incoming particles from cyclotron are off the linac working time. Therefore between two linac pulses the powerful cyclotron beam (1. 8 k. W that is a current of 100 u. A at 18 Me. V), if injected, could only damage the linac structure. It is mandatory, therefore, to chop the cyclotron beam, making this a pulsed beam synchronous with the linac accelerating field. 2 (b) avoid the instrumentation (mainly the modulator) and to the linac to suffer a constant irradiation during the cyclotron operation in order to limit gamma and neutron damages 4 quadrupoles match at best the transverse twiss parameters to the linac acceptance. In between the two doublets there is the chopping system During a 4. 5 us linac pulse, there are 187 cyclotron micropulses, but not all these particles can be accelerated. The linac will be positioned in the left shielded vane for the following reasons: (a) have enough space for adequate focusing in order to match the cyclotron beam to the linac Beam Chopping SPARKLE Radiobiology Line Cyclotron-Linac Coupling Problems The project has accumulated about 6 months of delay. Many components are ready. Some others are still under construction. RF Power supply is ready. It has been ordered as a turnkey system to Scandinova. It is based on a MG 5125 E 2 V magnetron. The four main Quads have been supplied by Radia. Beam company (USA). Vacuum components and controls have arrived. The Linac mechanics is almost complete. It has to be tuned and then brazed and welded. The complete assembly can be foreseen within summer, and the tests thereafter. The SCDTL structure consists of short DTL tanks coupled together by side coupling cavities. The DTLs are short tanks, each having 6 cells of βλ length, and the side cavity extends in a space left free on the axis for the accommodation of a very short (3 cm long, 2 cm o. d. , 6 mm i. d. ) PMQ (Permanent Magnet Quadrupole) for transverse focusing. The SPARKLE linac structure is composed of 7 tanks, among which the first and the last are half in length having only three gaps, 6 coupling cavities and 8 PMQs including the first and the last PMQ, Demountable (ASTER Inc. ) Supports and Collimators Sweeper magnet Output bunch Preliminary comparison between T 1 -T 7 triplet and measurement shows a reasonable agreement Output spectrum variation with accelerating field: nominal, -10%, +10% SCDTL LINAC – Mechanics completed Quadrupoles (Radia. Beam)