Carbon ion gantries Marco Pullia Fondazione CNAO M. Pullia – Carbon ion gantries – ICTR-PHE 2012 1
What is a gantry A gantry is a rotating beam line that allows directing the beam on the patient from any direction Conventional RT Gantry M. Pullia – Carbon ion gantries – ICTR-PHE 2012 2
Why a gantry Allows better, more robust planning: e.g. minimize fields pointing towards OAR (Organ At Risk) With horizontal line only With gantry O.A.R. M. Pullia – Carbon ion gantries – ICTR-PHE 2012 3
Treatment planned with gantry + + = M. Pullia – Carbon ion gantries – ICTR-PHE 2012 4
Size and magnetic rigidity Carbon Ion Gantry Conventional RT B ρ < 6.4 Tm Proton Gantry B ρ < 2.4 Tm M. Pullia – Carbon ion gantries – ICTR-PHE 2012 5
The CNAO 90° magnet during installation in the vertical line. The size is the same as for a gantry final magnet. M. Pullia – Carbon ion gantries – ICTR-PHE 2012 6
Present Many proton gantries (tens) Only one C gantry worldwide: L = 25 m x φ = 13 m, 600 t Very large, very heavy, very expensive Fixed Isocenter 360° rotation Parallel scanning 200 mm x 200 mm 140 t magnets 120 t shielding-counterweight (Udo Weinrich, GSI) 600 t total rotating mass M. Pullia – Carbon ion gantries – ICTR-PHE 2012 7
Can we make it better? As usual we want everything and its opposite at the same time… ◦ Small aperture final magnet to lower power consumption, but scanning upstream ◦ Small radius, but space around isocenter ◦ Light magnets, but possibly non superconducting ◦ Maximum performance, but cheap ◦ … M. Pullia – Carbon ion gantries – ICTR-PHE 2012 8
Aspects and ideas to be considered Scanning or scattering Not really a choice M. Pullia – Carbon ion gantries – ICTR-PHE 2012 9
Aspects and ideas to be considered Scanning SAD and scanning magnets position M. Pullia – Carbon ion gantries – ICTR-PHE 2012 10
Scanning magnets position Large aperture dipole: weight and power consumption Large gantry radius and large room size M. Pullia – Carbon ion gantries – ICTR-PHE 2012 11
Aspects and ideas to be considered Scanning SAD and scanning magnets position 360° vs 180° M. Pullia – Carbon ion gantries – ICTR-PHE 2012 12
360° vs 180° By rotating the couch by 180°, all the beam directions are possible also with only 180° of rotation of the gantry 180° M. Pullia – Carbon ion gantries – ICTR-PHE 2012 13
Aspects and ideas to be considered Scanning SAD and scanning magnets position 360° vs 180° Field patching M. Pullia – Carbon ion gantries – ICTR-PHE 2012 14
Field patching Scan in one go Scan and move (~PSI gantry 1) Move Move Move couch couch couch Reduces magnet aperture, but slower procedure and difficulties somehow similar to simultaneous optimisation of multiple fields with IMPT M. Pullia – Carbon ion gantries – ICTR-PHE 2012 15
Aspects and ideas to be considered Scanning SAD and scanning magnets position 360° vs 180° Field patching Fixed or mobile isocenter M. Pullia – Carbon ion gantries – ICTR-PHE 2012 16
Fixed or mobile isocenter Most of the existing gantries have a fixed isocenter on the rotation axis of the gantry. This implies large masses rotating at large radius. M. Pullia – Carbon ion gantries – ICTR-PHE 2012 17
Mobile isocenter PSI gantry 1 ( E. Pedroni ) An isocenter, through which all the directions pass, exists but its position depends on gantry orientation. M. Pullia – Carbon ion gantries – ICTR-PHE 2012 18
PSI Gantry 1 M. Pullia – Carbon ion gantries – ICTR-PHE 2012 19
Mobile isocenter - 2 Side access, PIMMS Patient positioned in a small room “somewhere” 15 m 10 m 5.6 m Gantry is longer, than just the last magnet but at small r Front access M. Pullia – Carbon ion gantries – ICTR-PHE 2012 20
Aspects and ideas to be considered Scanning SAD and scanning magnets position 360° vs 180° Field patching Fixed or mobile isocenter Multi-room system M. Pullia – Carbon ion gantries – ICTR-PHE 2012 21
Multi-room system Proposed by A.Brahme 1 -90<f<-30 1 -90<f<-30 2 -30<f<30 3 30<f<90 3 30<f<90 15m 0 5m 15m 10m 0 5m 10m ( M. Kats ) M. Pullia – Carbon ion gantries – ICTR-PHE 2012 22
Aspects and ideas to be considered Scanning SAD and scanning magnets position 360° vs 180° Field patching Fixed or mobile isocenter Multi-room system Divergent scanning M. Pullia – Carbon ion gantries – ICTR-PHE 2012 23
Divergent scanning Last drift 2m SAD 5.5 m (1 plane only!) Quad g = 8 T/m Gap reduced by 30% Scan ¡V Scan ¡H Quad M. Pullia – Carbon ion gantries – ICTR-PHE 2012 24
Aspects and ideas to be considered Scanning SAD and scanning magnets position 360° vs 180° Field patching Fixed or mobile isocenter Multi-room system Divergent scanning Superconducting magnets M. Pullia – Carbon ion gantries – ICTR-PHE 2012 25
Superconducting magnets If possible no He, use cryo-coolers Fabbricatore et al, 2001 M. Pullia – Carbon ion gantries – ICTR-PHE 2012 26
Straight coil heads Difficult to wind GFR 200 mm x 60 mm (field patching) Fabbricatore et al, 2001 M. Pullia – Carbon ion gantries – ICTR-PHE 2012 27
Preliminary studies done at Saclay ▪ Preliminary study for IBA (2008 - … ) - Irfu (SACM, SIS) - Focused on the SC 90 d° dipole - End of the first part: mid 2010 (Courtesy of F. Kircher) - Prolongation of the study under discussion Ulice meeting 23/11//2010 28
Double helix 5 T, Large good field region (26 cm diameter) Courtesy of Caspi, Robin, Arbelaez, Sessler, Sun, Hafalia, Yoon, Wan M. Pullia – Carbon ion gantries – ICTR-PHE 2012 29
Aspects and ideas to be considered Scanning SAD and scanning magnets position 360° vs 180° Field patching Fixed or mobile isocenter Multi-room system Divergent scanning Superconducting magnets FFAG gantry M. Pullia – Carbon ion gantries – ICTR-PHE 2012 30
FFAG Gantry 150-400 MeV/u 1500 kg of magnets Very large M. Pullia – Carbon ion gantries – ICTR-PHE 2012 31
FFAG Gantry (D. Trbojevic) M. Pullia – Carbon ion gantries – ICTR-PHE 2012 32
Other ideas Active alignment Active compensation of magnetic defects (scanning quadrupoles and sextupoles) Scanning by moving magnets … M. Pullia – Carbon ion gantries – ICTR-PHE 2012 33
Gantry in european projects Gantry studies have been proposed in the framework of european projects: ULICE and PARTNER M. Pullia – Carbon ion gantries – ICTR-PHE 2012 34
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Functional specifications survey Involve users (doctors) since the beginning of the study 37 https://espace.cern.ch/project-ULICE-WP6-Hadrontherapy-Survey/Lists/ULICE%20WP6%20Questionnaire/AllItems.aspx
Specs from questionnaire analysis Gantry functional specifications ¡ Field size ¡ 15 x 15 cm 2 or 10/15 x 20 cm 2 ¡ Number of fields per session ¡ 4 ¡ Penetration depth (range) ¡ 3 – 30 cm (corresponding energy: p = 60 - 220MeV; ¡ C ion = 120 – 430 MeV/u) ¡ Voxel dose accuracy ¡ ±1% ¡ Dose uniformity ¡ ±2.5% ¡ Voxels characterization ¡ 3 x 3 x 3 mm 3 ¡ Voxels out of range ¡ 1% ¡ Field position accuracy ¡ ±0.5 mm ¡ SAD ¡ 4 m ¡ Maximum treatment time ¡ 30 min ¡ Required space around isocentre ¡ 60 cm ¡ Achieved beam directions ¡ ALL ¡ “Deliverable Report JRA6.1 – Functional specifications”, June 2010 38
The 90° conventional dipole GFR 20 x 20 cm GFR 20 x 15 cm Max 3.208 (T) Max m 3.208 (T) 3 3.0 2.5 2.5 2.0 2.0 m 20cm 15cm 1.5 1.5 20cm 20cm 1.0 1.0 0.5 Min 2.57x10 -9 (T) 1.89 m Min 2.57x10 -9 1.78 m 20 ton gain 39
March 2011: choice of typology The ULICE WP6 collaboration decided to realize the conceptual design of a 180°, normal conducting, mobile isocenter gantry, 20 x 20 cm 2 field , revisiting the layout of the Riesenrad gantry investigated by the PIMMS Rationale for our choice Cheaper and simplified mechanical structure Design conceived for conventional magnets • • Less magnets in the gantry line Well known magnet technology • • Total weight reduced as well as deformations Layout adaptable to SC magnets • • LOWER COST ESTIMATE by mechanical firms with experience in the field
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Access M. Pullia – Carbon ion gantries – ICTR-PHE 2012 42
Mechanical structure: preliminary study Gaddi: Physics Dep. CERN 43
Conclusions Carbon ion gantries are needed There are margins for optimisation There are studies ongoing It looks likely that new carbon ion gantries will be built in the next future M. Pullia – Carbon ion gantries – ICTR-PHE 2012 44
That’s all,folks Thank you for your attention M. Pullia – Carbon ion gantries – ICTR-PHE 2012 45
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