P. A. Posocco – TH10 STATUS OF LINAC BEAM COMMISSIONING FOR THE ITALIAN HADRON THERAPY CENTER CNAO...
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Transcript of P. A. Posocco – TH10 STATUS OF LINAC BEAM COMMISSIONING FOR THE ITALIAN HADRON THERAPY CENTER CNAO...
1P. A. Posocco – TH10P. A. Posocco – TH10
STATUS OF LINAC BEAM STATUS OF LINAC BEAM COMMISSIONING COMMISSIONING
FOR THE ITALIAN HADRON THERAPY FOR THE ITALIAN HADRON THERAPY CENTER CNAOCENTER CNAO
P. A. PosoccoINFN-Laboratori Nazionali di Legnaro
On behalf of the CNAO-GSI-INFNcollaboration
2P. A. Posocco – TH10P. A. Posocco – TH10
Welcome to CNAOWelcome to CNAO(Centro Nazionale Adroterapia Oncologica)(Centro Nazionale Adroterapia Oncologica)
The CNAO has been conceived to perform treatment of deep seated tumours with light ion beams (proton, Carbon ions and others) and to clinical and radiobiological
3P. A. Posocco – TH10P. A. Posocco – TH10
CNAO from outsideCNAO from outside
TechnicalbuildingMain building:
2° floor: auditorium & library
1° floor: offices and laboratories
Ground floor: Reception and med. preparation
Basement: 3 treatment rooms
Accelerator vault
4P. A. Posocco – TH10P. A. Posocco – TH10
The CNAO facilityThe CNAO facility
- 2 w. horizontal beam - 1 w. hor. + vert. beam - scanning mag. (20x20 cm)- ~3000 patients/year - 80% C, 20% protons
- Compact design- 25 m diameter ring - Multi turn injection- Final energy:
Carbon: 2400 MeVProtons: 250 MeV
The accelerator The 3 treatment rooms
5P. A. Posocco – TH10P. A. Posocco – TH10 5
CNAO Injector:CNAO Injector:Sources Specifications
Extraction Voltage 24 kV
Current H3+ > 700 μA
Current C4+ > 150 μA
Transv. norm emitt. (95%) 0.5 mm mrad
LINAC Specifications
Operating frequency 216.816 MHz
Final beam energy 7 MeV/u
Beam pulse length ≤ 300 μs
Beam rep. rate ≤ 5 Hz
Transv. norm emitt. (95%) 0.8 mm mrad
Exit energy spread ± 0.3%
Total injector length ~ 19 m
SourcesC4+ and H3
+
7 MeV/u
400 keV/u
8 keV/u
IH - DTL
RFQ
Stripping foil
SolenoidSpectrometerSwitching magnet
Chopper
Ion source supervised by INFN LNSLow energy beam transport by CNAO Linac by GSI (second version of HICAT) supervised by INFN LNL
6P. A. Posocco – TH10P. A. Posocco – TH10
The InjectorThe Injectoras it was in January 2009as it was in January 2009
Source ISource II
RFQ
75° dipole
Spectrometer
Switchingmagnet Chopper
Solenoid
7P. A. Posocco – TH10P. A. Posocco – TH10 7
Injector commissioning milestonesInjector commissioning milestonesfrom to Section Description
May 08 July 08 Source Beam and LEBT Inst.
September 08 December 08LEBTTB0
Beam
January 09 February 09
RFQTB2
Install.
25th Feb. 09 12th Mar. 09 RF Cond.
13th Mar. 09 3rd April 09 Beam
April 09 May 09IH DTL
TB3
Install.
June 09 now RF Cond.
IH DTL
RFQLEBT
Sources
8P. A. Posocco – TH10P. A. Posocco – TH10
Ion Sources PerformancesIon Sources PerformancesImprovements (in 2007)
• the gas injection system has been modified in order to improve the stability
• extraction gap distance modified to improve beam emittance and stability
• a lead shield 10 mm thick all around the source instead of a 5 mm one for improving radiation safety
• the noise of electronics has been reduced
Performances• 250 μA for C4+ (25% > nominal) • 1100 μA for H3
+ (50% > nominal)
plasma electrode hole diameter reduced to 6 mm allowing to have better emittance
New extraction column
9P. A. Posocco – TH10P. A. Posocco – TH10 9
LEBT CommissioningLEBT Commissioning
TB0
Horizontal Vertical
C4+
Emitt
. RM
S: ~
35 m
m m
rad
10P. A. Posocco – TH10P. A. Posocco – TH10
Commissioning of LEBTCommissioning of LEBTTB0 (GSI & CNAO)TB0 (GSI & CNAO)
CNAOFaraday cup
Farady Cup
ACT (in front of solenoid)
Slit-scannerEmittance chamber (length = 390 mm!)
GSI End Cup
11P. A. Posocco – TH10P. A. Posocco – TH10 11
Emittance in TB0Emittance in TB0
TB0:• AC/DC current• AC/DC profiles• DC emittance exactly at the RFQ matching point!!!
- 4 +4 - 4 +4Horiz. Vert.- 4 +4 - 4 +4
Horiz. Vert.- 4 +4 - 4 +4
- 4 +4Horiz.
- 4 +4Vert.
- 4 +4Horiz.
- 4 +4Vert.
H3+
C4+
> 90% inside 180 mm mrad (yellow ellipse)
12P. A. Posocco – TH10P. A. Posocco – TH10
Sol-002
Sol-002
The 3 solenoids build by SigmaPhi: magnetic field along the axis measurements at INFN Frascati
12
Matching solenoidMatching solenoid
Example of beam steering at TB0 grid as function of the solenoid strength
Results:• Very accurate centroid displacement correction (~1 mm over 3 cm wide beam!!!)• Linear response
mrad
mm
mrad
mm
X i
30.0
10.0
76.2
34.1
Nominal value S. Vitulli & G. Bazzano
(CNAO)
13P. A. Posocco – TH10P. A. Posocco – TH10 13
LEBT Commissioning summaryLEBT Commissioning summaryTB0TB0
• Comparison current measurements (GSI/CNAO & DC/AC)– Consistency
• Comparison of profiles (grid/scanner)– Consistency
• Beam position as function of solenoid field – Steering at RFQ entrance
• Profiles for long and short macro pulses at – Neutralisation, Space
• Different times within pulse (H3+/C4+)
– Charge, verification of DC emittances
• Transmission, Twiss-Parameter and emittances – Matching RFQ– Definition of LEBT operating parameters– Pre-condition for RFQ commissioning
Mandatory for RFQ good performances!!!
14P. A. Posocco – TH10P. A. Posocco – TH10
Commissioning of RFQCommissioning of RFQTB2 (GSI)TB2 (GSI)
Faraday Cup Profile grid (from right)
End Cup
MobEmi Slits and profile grid
Phase probes
ACT
Beam
15P. A. Posocco – TH10P. A. Posocco – TH10
Intertank section with MEBT partly integrated in the RFQ:Intertank section with MEBT partly integrated in the RFQ:compact but reduced flexibilitycompact but reduced flexibility
IH-DTL
RFQ
Quadrupole magnetsSteerer
magnets
Phase probe
205 mm
Buncher gaps
Beam
16P. A. Posocco – TH10P. A. Posocco – TH10 16
Commissioning RFQ Commissioning RFQ –– Results H Results H33+ + at 8 keV/u at 8 keV/u
transmission, steering and energytransmission, steering and energy
Transmission ~57 % at working point 5.1 Volt (195 kW)Moderate steering in both planes with smooth behaviour
Steerer LN-002-ITM offQD1= -11.8 m-1 / QD2= 8.6 m-1
Step 1:Optimisation
Step 2:Perform standardmeasurements
17P. A. Posocco – TH10P. A. Posocco – TH10 17
Commissioning RFQ Commissioning RFQ –– Results H Results H33+ + at 8 keV/uat 8 keV/u
Emittances in TB2Emittances in TB2
4 rms [mm mrad] 4 rms [mm mrad]
18P. A. Posocco – TH10P. A. Posocco – TH10 18
Commissioning RFQ – Results CCommissioning RFQ – Results C4+4+
Transmission, energy und steeringTransmission, energy und steeringVariation of Solenoid
40
45
50
55
60
65
9.4 9.6 9.8 10.0 10.2 10.4
L2-019B-SL1 [1/m]
Tra
nsm
iss
ion
[%]
Transmission RFQ
30
35
40
45
50
55
60
65
4.4 4.5 4.6 4.7 4.8 4.9 5.0 5.1 5.2 5.3
Tank Voltage [V]
Tra
ns
mis
sio
n [
%]
Steering RFQ
-3
-2
-1
0
1
2
3
4.4 4.5 4.6 4.7 4.8 4.9 5.0 5.1 5.2 5.3
Tank Voltage [V]
Ste
eri
ng
[m
m]
x / mm
y / mm
RFQ Beam Energy
390
395
400
405
410
415
420
4.4 4.5 4.6 4.7 4.8 4.9 5.0 5.1 5.2 5.3 5.4
Tank Voltage [V]
Be
am
En
erg
y [
ke
V/u
]
Step 1:Optimization
Step 2:Performstandardmeasurements
Transmission ~62 % at working point 5.1 Volt (195 kW)Moderate steering in both planes with smooth behaviour
19P. A. Posocco – TH10P. A. Posocco – TH10 19
Commissioning RFQ – Results CCommissioning RFQ – Results C4+4+
Emittances in TB2Emittances in TB2
4 rms [mm mrad] 4 rms [mm mrad]
20P. A. Posocco – TH10P. A. Posocco – TH10 20
Probe beam (HProbe beam (H33++))
Slits combined to reduce up to 10% of the full emittance!!!
Horizontal Vertical
profile in L2(~10 mm width)
H3+
Emit. RMS:~5 π mm mrad
M. Pullia (CNAO)
21P. A. Posocco – TH10P. A. Posocco – TH10 21
Transmission ~70 % at working point 5.1 Volt (195 kW)
Moderate steering in both planes with smooth behaviour
Steerer LN-002-ITM ausQD1= -11.8 / QD2= 8.6
RFQ Beam Energy (new drift lenght)
390
395
400
405
410
415
420
425
4,4 4,5 4,6 4,7 4,8 4,9 5,0 5,1 5,2 5,3 5,4
Tank Voltage [V]
Beam
Energ
y [keV
/u]
Transmission RFQ
40
45
50
55
60
65
70
75
80
4,40 4,60 4,80 5,00 5,20
Tank Voltage [V]
Tra
nsm
issi
on [%
]
Steering RFQ
-3
-2
-1
0
1
2
3
4,4 4,5 4,6 4,7 4,8 4,9 5,0 5,1 5,2 5,3
Tank Voltage [V]
Ste
erin
g [m
m]
x / mm
y / mm
RFQ: Results HRFQ: Results H33+ + “probe beam”“probe beam” at 8 keV/uat 8 keV/u
Steering, energy and transmissionSteering, energy and transmission
22P. A. Posocco – TH10P. A. Posocco – TH10 22
RFQ commissioning resultsRFQ commissioning resultsIon H3
+ C4+
Energy (keV/u) 7.5 8.0 8.5 8.0
Workingpoint (V) 5.15 5.10 5.15 5.10
Max. transm.full beam 4.6% 58% 59% 62%
Max. transm.probe beam 3.4% 71% 69% -
x rms emit.(4 rms [mm mrad]) - 18.7 21.6 17.9
y rms emit.(4 rms [mm mrad]) - 14.2 13.7 12.3
23P. A. Posocco – TH10P. A. Posocco – TH10 23
Effect of the bend electrodes on RFQ acc.Effect of the bend electrodes on RFQ acc.
(total)
Full beam
cm
HITCNAO
By S. Yaramyshev
150 17512530
Probe beam
Measured at CNAO~15%
24P. A. Posocco – TH10P. A. Posocco – TH10 24
xc= -1.4 mm
x’c= 3 mrad
yc= -0.1 mm
y’c= -10 mrad
± 15 mrad!!
By S. Yaramyshev
Probe beam displaced in position and angle with L2 steerers
Exp. RFQ acceptance at 8 keV/uExp. RFQ acceptance at 8 keV/u
M. Pullia (CNAO) et al.
25P. A. Posocco – TH10P. A. Posocco – TH10 25
Commissioning RFQCommissioning RFQSummary resultsSummary results
• Working point: – Energy of 400 keV/u reached at 195 kW power
• Steering RFQ and quadrupole doublet: – Size acceptable and smooth behavior – during operation only small correction with steerers – very small beam losses in inter-tank section!
• Currents: – ~500 µA (H3
+) – ~75 µA (C4+) – transmissions up to 60 %
• Transverse emittances:– H3
+ : Hor - Ver(90%) = 19 / 14 π mm mrad– C4+: Hor - Ver(90%) = 18 / 12 π mm mrad– within acceptance of IH-DTL (~50 mm mrad)
• RFQ operating parameters: – Established for H3
+ and C4+ beams
26P. A. Posocco – TH10P. A. Posocco – TH10 26
Commissioning RFQCommissioning RFQSummary of further measurementsSummary of further measurements
• Variation of LEBT energy: Measurements with 7.5, 8.0 and 8.5 keV/u– At 7.5 keV/u no useful results– At 8.5 keV/u results are similar to 8.0 keV/u case but at higher RFQ power level
• Stability of energy over 1.5 h: – variation in 2 keV/u region
• Measurement (Hor. and Vert.) of RFQ acceptance at 8.0 and 8.5 keV/u:– both measurements consistent
• Optimization of LEBT settings with respect to centers of measured acceptance– higher transmission– reduced steering and emittance after RFQ
• WHY ONLY 70% TRASMISSION AT MAX, with pencil beam ?– Probably longitudinal losses, the RFQ is not able to capture and accelerate more than
70% of particles even for on axis particles!
27P. A. Posocco – TH10P. A. Posocco – TH10 27
Now: IH – DTL!Now: IH – DTL!TB3 (GSI)TB3 (GSI)
28P. A. Posocco – TH10P. A. Posocco – TH10
Thanks to all the authorsThanks to all the authors
• A. Pisent, P. A. Posocco, C. Roncolato, INFN/LNL, Legnaro (PD), Italy
• C. Biscari, INFN/LNF, Frascati (RM), Italy• G. Ciavola, S. Gammino, INFN/LNS, Catania, Italy• G. Clemente, K. M. Kleffner, M. Maier, A. Reiter,
B. Schlitt, H. Vormann, GSI, Germany • G. Balbinot, E. Bressi, M. Caldara, A. Parravicini,
M. Pullia, C. Sanelli, E. Vacchieri, S. Vitulli, CNAO Foundation, Pavia, Italy