ESA HARMONICS Final Presentation (FP), Frascati , May 8, 2012
ACCELERATING A CYCLOTRON 18 MEV PROTON BEAM BY A SCDTL LINAC Luigi Picardi, Concetta Ronsivalle...
1
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 MeV, 150 uA 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 MeV 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. THE SCDTL STRUCTURE 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 Preliminary comparison between T1-T7 triplet and measurement shows a reasonable agreement 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. 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 (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 SPARKLE Radiobiology Line 4 quadrupoles match at best the transverse twiss parameters to the linac acceptance. In between the two doublets there is the chopping system Status-Equipments 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 MG5125 E2V magnetron. The four main Quads have been supplied by RadiaBeam 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. Cyclotron-Linac Coupling Problems PMQ, Demountable (ASTER Inc. ) SCDTL LINAC – Mechanics completed Supports and Collimators Sweeper magnet Beam Dynamics 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 MeV proton beam up to at least 24 MeV, 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. 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. 17 18 19 20 21 22 23 24 0 100 200 300 400 500 D N /5 0 k e V , 1 5 9 5 4 p articles E,M eV E nd ofLIN AC -5 00 0 500 1000 1500 2000 2500 3000 0 100 200 300 400 N um b e r o f p a rticle s in 20 ° phase,deg@ 3 G Hz C ondizionidiriferim ento 16 17 18 19 20 21 22 23 24 25 0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000 5500 6000 N um b e r o fp a rticle s in D E =1 M eV E,M eV N om ina lF ield, O u tpu tP articles= 1597 8 A bove 23 M eV =3470 16 17 18 19 20 21 22 23 24 25 0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000 5500 6000 N um b e r o f p a rticle s in D E =1 M eV E ,M eV F ie ld -1 0 % ,O u tpu tP articles= 1 974 5 A bove 23 M eV = 2802 16 17 18 19 20 21 22 23 24 25 0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000 5500 6000 N um b e r o fp a rticles in D E =1 M eV E,M eV F ie ld + 10 % ,O u tpu tP a rticles= 11 74 6 A bove 23 M eV = 2438 Beam Chopping A sweeping magnet paints the beam vertically. A couple of collimators stop the beam except during the zero crossing Power distribution in the collimators 0 10 20 30 40 50 60 0 100 200 300 400 500 600 700 800 900 1000 z,m m Vert sem i-Aperture, m m Absorbed linearpower, W /cm 2*sigm aY, m m 2*sigm aX , m m 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. 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. During a 4.5 us linac pulse, there are 187 cyclotron micropulses, but not all these particles can be accelerated. Therefore between two linac pulses the powerful cyclotron beam (1.8 kW that is a current of 100 uA at 18 MeV), 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. 1 2 Output spectrum variation with accelerating field: nominal, -10%, +10% Output longitudinal phase space (3 ns beam input) Beam losses through the line Output spectrum Output bunch 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. Out of 100 A CW (average) cyclotron beam, 17 A pulsed (17 nA average) beam exit from linac Only 3 A pulsed (3 nA average) beam is accelerated to 24 MeV +/- 1 MeV The beam should be cleaned with a magnet! A few nA beam average current is sufficient for radiobiology studies Bunch evolution has been computed Quadrupoles (RadiaBeam)
-
Upload
camron-daniels -
Category
Documents
-
view
217 -
download
0
Transcript of ACCELERATING A CYCLOTRON 18 MEV PROTON BEAM BY A SCDTL LINAC Luigi Picardi, Concetta Ronsivalle...
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 MeV, 150 uA 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 MeV 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.
THE SCDTL STRUCTURE
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
Preliminary comparison between T1-T7 triplet and measurement shows a reasonable agreement
SPARKLE FACILITY and SCOPE OF EXPERIMENTThe 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.
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
(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
SPARKLE Radiobiology Line4 quadrupoles match at best the transverse twiss
parameters to the linac acceptance. In between the two doublets there is the chopping system
Status-EquipmentsThe 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 MG5125 E2V magnetron. The four main Quads have been supplied by RadiaBeam 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.
Cyclotron-Linac Coupling Problems
PMQ, Demountable (ASTER Inc. )
SCDTL LINAC – Mechanics completed
Supports and Collimators
Sweeper magnet
Beam Dynamics
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 MeV proton beam up to at least 24 MeV, 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.
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.
17 18 19 20 21 22 23 240
100
200
300
400
500
DN
/50
ke
V, 1
59
54
pa
rtic
les
E, MeV
End of LINAC
-500 0 500 1000 1500 2000 2500 30000
100
200
300
400
Num
ber
of p
artic
les
in 2
0°
phase, deg@3 GHz
Condizioni di riferimento
16 17 18 19 20 21 22 23 24 250
500
1000
1500
2000
2500
3000
3500
4000
4500
5000
5500
6000
Nu
mb
er
of
pa
rtic
les
in D
E=
1 M
eV
E, MeV
Nominal Field, Output Particles=15978Above 23 MeV =3470
16 17 18 19 20 21 22 23 24 250
500
1000
1500
2000
2500
3000
3500
4000
4500
5000
5500
6000
Nu
mb
er
of
pa
rtic
les
in D
E=
1 M
eV
E, MeV
Field -10%, Output Particles=19745Above 23 MeV = 2802
16 17 18 19 20 21 22 23 24 250
500
1000
1500
2000
2500
3000
3500
4000
4500
5000
5500
6000
Nu
mb
er
of
pa
rtic
les
in D
E=
1 M
eV
E, MeV
Field +10%, Output Particles=11746Above 23 MeV = 2438
Beam ChoppingA sweeping magnet paints the
beam vertically. A couple of collimators stop the beam except during the zero crossing
Power distribution in the collimators
0
10
20
30
40
50
60
0 100 200 300 400 500 600 700 800 900 1000z, mm
Vert semi-Aperture, mm
Absorbed linear power, W/cm
2*sigmaY, mm
2*sigmaX, mm
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.
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.
During a 4.5 us linac pulse, there are 187 cyclotron micropulses, but not all these particles can be accelerated.
Therefore between two linac pulses the powerful cyclotron beam (1.8 kW that is a current of 100 uA at 18 MeV), 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.
1
2
Output spectrum variation with accelerating field: nominal, -10%, +10%
Output longitudinal phase space (3 ns
beam input)Beam losses through the line
Output spectrumOutput bunch
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.
Out of 100 A CW (average) cyclotron beam,
17 A pulsed (17 nA average) beam exit from linac
Only 3 A pulsed (3 nA average) beam is accelerated to 24 MeV +/- 1 MeV
The beam should be cleaned with a magnet!
A few nA beam average current is sufficient for radiobiology studies
Bunch evolution has been computed
Quadrupoles (RadiaBeam)
