SIEMENS/DANFYSIK Partikel Terapi acceleratoren - AU · PDF fileSIEMENS/DANFYSIK Partikel...

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1 Motivation: Cancer Krav til beam Acceleratorer til partikel terapi DF/SAG accelerator systemet Opsummering SIEMENS/DANFYSIK Partikel Terapi acceleratoren S S ø ø ren Pape M ren Pape M ø ø ller ller DANFYSIK DANFYSIK http://cern.ch/AccelConf/p07/PAPERS/THPMN004.PDF

Transcript of SIEMENS/DANFYSIK Partikel Terapi acceleratoren - AU · PDF fileSIEMENS/DANFYSIK Partikel...

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Motivation: CancerKrav til beamAcceleratorer til partikel terapiDF/SAG accelerator systemetOpsummering

SIEMENS/DANFYSIKPartikel Terapi acceleratoren

SSøøren Pape Mren Pape MøøllerllerDANFYSIKDANFYSIK

http://cern.ch/AccelConf/p07/PAPERS/THPMN004.PDF

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Dose and intensity• Range of 30 cm →• Proton energy: (50-)250 MeV• Carbon energy: (100-)430 MeV/u=5GeV

• Dose of 2 Gy (=J/kg) in 2(10) l in 2 min. →• Particle intensity 6⋅1011 p in 2 min

or 2⋅1010 C in 2 min

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Lineær accelerator

Synkrotron

Cyclotron

Acceleratorer til PT

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SIEMENS (DANFYSIK)heavy-ion therapy

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18t

Ø8m

SAG-DF-MTA gantry

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Udfordringer ved et PT anlæg

• Kompleksitet• Pålidelighed - QA• Økonomi• Logistik

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SIEMENS/DANFYSIK PT system

10m

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DF-SAG facility

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Semi-vertical beamline

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PT RKA

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11<0.1%Variations in mean energy from synchrotron

<30%Integral intensity (fill)

<0.5 mmPosition variations at isocenter (including feedback)

<20%Beam width at variations at isocenter

<3Max/min intensity for faster sampling (down to 10 µs)

<+30%/-50%Extracted intensity (300 ms) sampling

Stability during spill

0.001-1Intensity variation

1⋅109Maximum number of carbon ions at end of HEBT per spill

4⋅1010Maximum number of protons at end of HEBT per spill

>95-98%System uptime

<8 s (TBC)Time to switch beam from room to room

<5 s (TBC)Time for energy change (stop extraction to start extraction)

<10 s (up to 30 s)Extraction time from synchrotron

<1 sRamping time of synchrotron to highest magnetic field

<10 sTime to change between ion species

88-430 MeV/uCarbon ion energy range

48-250 MeV/uProton energy range

Main specs. to the PT accelerator system

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DF-SAG facility

15mA

0mA

Un-separated DC beam from sourceH3

+, H2+, H+, …

C4+, …

8 keV/amu

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DF-SAG facility

2mA

0mA

Separated DC beamH3

+

C4+

8 keV/amu

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DF-SAG facility

2mA

0mA

Separated chopped beam

200μs

5 Hz

8 keV/amu

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DF-SAG facility

2mA

0mA

Bunched beam acceleration in LINAC

216MHz

200μs

..…………...

7 MeV/amu

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DF-SAG facility

100mA

0mA

10-turn multiturn injection into synchrotron

2μsH+, C6+

stripper

7 MeV/amu

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DF-SAG facility

20mA

0mA

Synchrotron acceleration during 1 s

..…

1-7 MHz

7-430 MeV/amu

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DF-SAG facility

0.1pA-10nA

0

Extraction of DC beam

50-430 MeV/amu

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LEBT, RFQ, LINAC, MEBT samt injektion

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LEBT

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ECR Ion Source

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Beam after ion source

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IS + LEBT i Heidelberg

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LEBT

•Macro-pulsechopper

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Solenoide

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RFQ + LINAC

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IH-accelerator

• 56 accelerating gaps within 3.8 m

• Accelerates from 400 keV/u to 7 MeV/u

• About 850kW of RF power needed

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HIT-IH Cavity

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Electric field IH-cavity

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Magnetic field IH-cavity

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Fields inside the IH-cavity

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LINAC quadrupoles

Ramped lenses with 5Hz

15ms ramp-up-time, 3ms flat-top, 25ms ramp-down-time

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The RF-system consists of:

- 200 kW amplifier at 0,5% duty cycle

- 1,4 MW amplifier at 0,5% duty cycle

- 4 kW amplifier at 0,5% duty cycle

Photos byHIT

RF amplifiers

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Radial Envelopes

0 100 200 300 400 500 600

-5

0

5ra

dial

env

elop

es x

and

y [m

m]

z[cm] beamaxis

-35° -35° -35°0° 0° 0°

L L

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MEBT

Vertical correctors

chopper

Injection septum

Stripper foil

debuncher

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MEBTHorizontal beam envelope [m] versus distance [m]

Vertical beam envelope [m] versus distance [m]

Note: Linear optics

0.000

0.000

14.574

14.574

0.025000

0.025000

-0.025000

-0.025000

Betatron envelope Momentum envelope

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Chopper

slit

bend chop bend

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Charge separation

The most closely spaced ions, from a not complete stripping process, will be O7+ and O8+.

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MEBT 25° dipole

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Debuncher

Beam at the stripper:

After the debuncher:

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DF synchrotron

Bumper

Elektrostatiskinjektionsseptum

Elektrostatiskekstraktionsseptum

Magnetiskeekstraktionssepta

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Synchrotron

BumperElektrostatiske septaMagnetiske septaBeam position monitor

Beam strøm transformereFluorescerende skærmeLong. og transv. pickupsExciter elektroderScrapers

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Synchrotron dipole

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Non-linear EFB variation, Pre-prototype exit, y=0, 100%

-0.00100

-0.00080

-0.00060

-0.00040

-0.00020

0.00000

0.00020

0.00040

0.00060

0.00080

0.00100

-100 -80 -60 -40 -20 0 20 40 60 80 100

x (mm)

dLre

s/Lh

alf (

T)

dLres/LhalfdInt_Rel Calculated

Maximum field, Pre-prototype exit, y=0, 100%

-0.00500

-0.00400

-0.00300

-0.00200

-0.00100

0.00000

0.00100

0.00200

0.00300

0.00400

0.00500

-100 -80 -60 -40 -20 0 20 40 60 80 100

x (mm)

dB0/

B0 (T

)

dB0/B0dB/B0 Calculate

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Electrostatic injection septum

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ElectrostaticExtraction septum

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Magnetic extraction septum

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Extraction straight section

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Synchrotron sextupole

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Synchrotron cycle

•0

•0,2

•0,4

•0,6

•0,8

•1

•1,2

•0 •1 •2 •3 •4 •5 •6 •7

•time (s)

•B/B

max

•low-energy protons•high-energy protons•low-energy carbon•high-energy carbon

•"chimney"

•dB•/•dt•/•Bmax •=1/s

•Extraction•1-10s

•Injection

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Beam envelope at injection

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Injection bump

Bumper magnet #1 #2 #33.2 mrad. 6.3 mrad. 7.6 mrad.

septum

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Bumper supply

time

Magnetic field

18 μs

Turn 4 15

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Multi-Turn-Injection

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Synchrotron cavity

2.5 kV

Rf: 1-7 MHz

Omløbsfrekvens 0.5-3.5 MHz

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Synchrotron dump

Vertical beam envelope [m] versus distance [m]

Note: Linear optics

11.220 18.422

0.040000

-0.040000

Betatron envelope Momentum envelope

Note: Linear optics

0.000 64.800

0.025000

-0.025000

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Slow Extraction

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HEBT

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HEBT

Survey-Plot [mm] 108000

HC

HS

1

HC

VS

1

HC

HS

2

HC

VS

2H

CP

G1

HC

HS

3

HC

HS

4

HC

VS

4H

CP

G2

HC

PG3

HC

HS

5

HC

VS5

HC

PG4

H1PGT

H2PGT

H3PGT

H4H

S1

H4V

S1

H4H

S2

H4V

S2

H4P

G2

H4HS3

H4VS3

H4PGT

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Fast Beam Abort System

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HEBT

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Vertical beamline for Japan

HC

HS

3

HC

HS

4H

CQ

D6

HC

QF7

HC

VS

4H

CP

G2

H1B

M1

HC

QF8

HC

QD

9H

CP

G3

H2B

M1

HC

HS

5H

CQ

DA

HC

QFB

HC

VS

5H

CP

G4

H4BM

1

H4BM2

H4HS1

H4QF1H4QD2

H4VS1H4BM3

H4BM

4

H4H

S2

H4Q

F3H

4QD

4H

4VS

2

H4P

G2

H4B

M5

H4B

M6

H4H

S3

H4V

S3

H4Q

D5

H4Q

F6H

4SC

VH

4SC

H H4B

M7

H4BM8

H4BM9

H4PGTISO-TR4

H3B

M1

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HEBT quadrupole

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HEBT beam + conditioninge

time

Magnetic field

2s

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67SHZ1-L/R-01 FCP1-L/R-01 VSC1-L/R-01

SHZ1-L/L-01 FCP1-L/L-01 VSC1-L/L-01

PRF1-L/R-01 (DCCT - in review)

PRF1-L/L-01 (DCCT - in review)SHZ1-L/C-01 SVT1-L/C-01 PRF1-L/C-01

RFQ

Chopper1

DTL

D Switch

D AnalyserD Analyser

Source

Source

D 25 degr

D 25 degr

DQVst

D

QVst

Q

[ PU1 Siemens ]

SHZ1-L/C-02 FCP2-L/C-01 PRF1-L/C-02

PU1-M-01 PRF1-M-01 FCT1-M-01

PU1-M-02

D inflectD

D

D

D

DD

D

D

D

D

D

D

D

D

D

QQ

QQ QQ QQQ

Vst

Q

ScnXY ScnXY ScnXY

DQQ

Q S

Debuncher

Chopper2

SHZ2-M-01 FCP2-M-02 PRF1-M-02

PU1-M-03 FCT1-M-02 PRF1-M-04 FCP2-M-03

PRF1-M-03

RF cavity

QS

QVst

Q

QSDCCT2-S-01 FCT2-S-01

BPM1-S-06

BPM1-S-01

BPM1-S-02

BPM1-S-03

BPM1-S-04

BPM1-S-05

BLM1-S-01

BLM1-S-02

BLM1-S-03

SLM1-S-02(Schottky PU)

SLM1-S-01(BTF exciter)

SLM1-S-03(KO exciter)

SQ

SCP1-S-01

VSC2-S-01

VSC2-S-02

MWPC1-H/C-01ION1-H/C-01

SNT1-H/C-01

SCP2-H/C-01

Q Vst

Q S

MWPC1-H/C-02ION1-H/C-02

SNT1-H/C-02

MWPC1-H/V1-01ION1-H/V1-01

SNT1-H/V1-01

Mag sept

[ BAMS ]

VSC2-H/C-01VSC2-H/V1-01

Rev: 8 Date: 07 Nov 2006Drn: JG Chk:

Sol

Q

QQQ

Sol

QQ

QQQ

Q

Sol

D v corr

QQ

ES septum

SS1

SS2

Inj bumper 1

SS3

Vst

SS4

SS5

SS6

ES septS

Mag sept

Inj bumper 2

Inj bumper 3

Fast AbortQ QQ

D

QQQ

DD

DD

D

D

QQ

D

ScnXY

[ BAMS ] [ BAMS ]

[ BAMS ]

Stripper

FCP2-M-01

MWPC1-H/C-03ION1-H/C-03

SNT1-H/C-03

MWPC1-H/C-04ION1-H/C-04

SNT1-H/C-04

Hst Hst HstHst VstHst

Vst

H/Vst

QQHst Vst QQHst Vst QQHst Vst

QQHst

SHZ2-M-02

SHZ1-L/R-02 FCP1-L/R-02

SHZ1-L/L-02 FCP1-L/L-02

sa, sa pa pa

pa

sa, sa pa

sa, sa pa pa

pa

sa, sa pa

sa, sa sa, sa pa

sa, sa pa pa

pa pa

pa

sa pa pa

sa

pa

pa pa pa

pa

pa

pa

pa

papa

pa

pa

pa

pa

pa

pa

pa

pa

Key

[ Device acronym Device subtype # - Region/Subregion - Sequential # ]

Regions Diagnostic devicesL LEBT: Acronym LE ME SY HE Qty Description

/L Left-hand source arm BLM 3 3 Beam loss monitor/R Right-hand source arm BPM 6 6 Beam position monitor, X,Y (with Schottky o/p)/C Common section DCCT1 0 (2) 0 DC (parametric) current transformer (2: in review)

DCCT2 1 1 DC current transformer integrated with FCT M MEBT: FCP1 4 4 Faraday cup high power (cooled)S Synchrotron FCP2 1 3 4 Faraday cup low power (uncooled)H HEBT FCT1 2 2 AC current transformer

/C Common section FCT2 1 1 AC current transformer integrated with DCCT /H1 Horizontal line 1 ION 5 5 Ionisation chamber (3 with readout)/H2 Horizontal line 2 MWPC 5 5 Multiwire prop chamber/H3 Horizontal line 3 PRF 4 4 8 Profile grid harp array, in vacuum/V1 Vertical line 1 PU 3 3 Capacitive pickup, non-position sensitive

SCP1 1 1 Scraper (synchrotron beam dump)SCP2 1 1 Scraper (Fast abort beam dump)

Other devices SHZ1 6 6 Horizontal slit pairRFQ Radio frequency quadrupole SHZ2 2 2 Horizontal slit single bladeDTL Drift tube linac SVT 1 1 Vertical slit pairChopper1 200us chopper SLM 3 3 Stripline xy (RF exciter or Schottky PU)Chopper2 36us chopper SNT 5 5 Scintillator, pulse countingAmag Analyser magnet (m,q) VSC1 2 2 Viewing screen, tantalum, high powerD Dipole magnet VSC2 2 1 3 Viewing screen, phosphor, dual positionHst Horizontal steerer magnetVst Vertical sterrer magnet ActuatorsQ Quadrupole magnet sa 14 2 16 Stepper axisS Sextupole pa 11 9 2 12 34 Pneumatic axisScnXY Scan magnets, X,YBAMS

Excludes items in Siemens scope (qty 1 PU)

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Faraday Cup

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AC DC transformer

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70

Profile Grid in LEBT/MEBT

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71

Slits/scraper/stripper cooled/uncooled

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72

Phase Probe for MEBT

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73

Beam Position Monitor

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74

Schottky probe

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75

Beam Loss Monitor

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76

Scintillation counter in HEBT

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77

MWPC in HEBT

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78

Ionisation chamber

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79

Fluorescent screen in HEBT

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Accelerator Control System

• Eckelmann