BNCT System Using 30MeV H CyclotronCyclotron · 2011-11-03 · BNCT System Using 30MeV...

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1 BNCT System BNCT System Using 30MeV H Using 30MeV H - - Cyclotron Cyclotron T. Mitsumoto a , K. Fujita a , T. Ogasawara a , H. Tsutsui a , S. Yajima a , A. Maruhashi b , Y. Sakurai b , H. Tanaka b a Sumitomo Heavy Industries, Ltd. (SHI) b Kyoto University Research Reactor Institute (KURRI) Cyclotrons 2010 (Lanzhou, China) September 6-10, 2010

Transcript of BNCT System Using 30MeV H CyclotronCyclotron · 2011-11-03 · BNCT System Using 30MeV...

Page 1: BNCT System Using 30MeV H CyclotronCyclotron · 2011-11-03 · BNCT System Using 30MeV H-CyclotronCyclotron T. Mitsumoto a, K. Fujita , T. Ogasawaraa, H. Tsutsuia, S. Yajimaa, ...

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BNCT System BNCT System Using 30MeV HUsing 30MeV H-- CyclotronCyclotron

T. Mitsumotoa, K. Fujitaa, T. Ogasawaraa,H. Tsutsuia, S. Yajimaa,

A. Maruhashib, Y. Sakuraib, H. Tanakab

a Sumitomo Heavy Industries, Ltd. (SHI)b Kyoto University Research Reactor Institute (KURRI)

Cyclotrons 2010 (Lanzhou, China) September 6-10, 2010

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1.1. AcceleratorAccelerator--Based Boron Neutron Based Boron Neutron Capture Therapy (BNCT) SystemCapture Therapy (BNCT) System

2.2. Current Status of Sumitomo BNCT Current Status of Sumitomo BNCT System at Kyoto Univ.System at Kyoto Univ.

3.3. Schedule and Future PlanSchedule and Future Plan

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1. Accelerator1. Accelerator--Based Boron Based Boron Neutron Capture Therapy (BNCT)Neutron Capture Therapy (BNCT)

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11--2. Nuclear reactor to accelerator2. Nuclear reactor to accelerator

Conventional BNCT system Conventional BNCT system with nuclear reactorwith nuclear reactor

•• Easy to manageEasy to manage

•• CompactCompact

•• Acceptable to the publicAcceptable to the public

Accelerator based BNCTAccelerator based BNCT

Accelerator is desirable in hospitals

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11--3. Basic configuration3. Basic configuration

AcceleratorAcceleratorModeratorModeratorModerator

Boron compounds

Boron Boron compoundscompoundsFast

neutronsFast Fast

neutronsneutrons

InfusionInfusion

TargetTarget

Irradiation SystemIrradiation System

Proton Proton beambeam Epithermal Epithermal

neutronsneutrons

AcceleratorAccelerator--Based BNCT SystemBased BNCT System

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11--4. Comparison of accelerators4. Comparison of accelerators

Cyclotron Middle Energy Linac Low Energy Linac(Electrostatic or RF)

Energy 10 ~ 30 MeV 10~15 MeV ~ 3 MeVAverage Beam Current 1 ~ 3 mA 2~3 mA ~20 mA

Target Beryllium (Solid) Beryllium (Solid) Lithium (Solid/Liquid)

Neutron Energy at Target

~30 MeV (peak at ~1MeV)

~15 MeV(peak at ~1MeV) ~1 MeV

Moderator Size Larger Larger SmallerRadiation Shield Larger Larger Smaller

Technical Hurdle Almost nothing High duty linac High current linacTarget

Accelerator Size ~3 m ~10 m ~3 m

We selected cyclotron

stopwarninggo

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2. Current Status of Sumitomo2. Current Status of Sumitomo

BNCT System at Kyoto Univ.BNCT System at Kyoto Univ.

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22--1. BNCT in Kyoto Univ.1. BNCT in Kyoto Univ.Kyoto University Research Reactor Institute (KURRI)and Sumitomo Heavy Industries (SHI) started collaboration in 2007

Kyoto Univ. Research Reactor (KUR)

1F2F

3F

Innovation Research LaboratoryInnovation Research Laboratory

The BNCT system was installed in 2008The BNCT system was installed in 2008

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22--2. Layout of the BNCT system2. Layout of the BNCT system

HMHM--30 Cyclotron30 Cyclotron

TargetTarget

Treatment CouchTreatment Couch

Beam Transport Beam Transport SystemSystem

ModeratorModerator

Irradiation Irradiation and Treatmentand TreatmentSystemSystem

15m15m

8m8m

10m10m

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22--3. HM3. HM--30 cyclotron for BNCT30 cyclotron for BNCT

Accelerator Name HM-30Particle H-

Energy 30 MeVExtraction Method Foil strippingMaximum Beam Current 1.1 mA (2 mA is possible)Maximum Power 33 kW (60 kW)Size W 3.0 m × D 1.6 m × H 1.7 mWeight 60 tons

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22--4. Features of HM4. Features of HM--3030

• Injection15 mA volume cusp type H- ion sourceTwo solenoids and one RF buncher in LEBTNew type tilted spiral inflector for axial injection

• AccelerationDesigned with a Runge-Kutta tracking code for

minimizing beam off-centering and maximizing beam transmission

• ExtractionCarbon foil stripper

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22--5. New type spiral inflector5. New type spiral inflector

By adding skew-quadrupole component to the electric field, the vertical beam divergence has been reduced

by beam tracking

oldnew

skew quadrupole strength (%)applying for patent

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22--6. Examples of beam current (1)6. Examples of beam current (1)1 m A運転トレンド

0.0

0 .2

0 .4

0 .6

0 .8

1 .0

1 .2

1 6 :4 8 1 7 :0 2 1 7 :1 6 1 7 :3 1 1 7 :4 5 1 8 :0 0 1 8 :1 4

時間

ビーム電流(mA)

55 min.

The maximum current is limited to 1.1 mA by The maximum current is limited to 1.1 mA by KURRIKURRI’’ss regulationregulation

Time

Bea

m c

urre

nt (m

A)

Beam current at target position is very stable Beam current at target position is very stable during about 1 hour operationduring about 1 hour operation

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22--6. Examples of beam current (2)6. Examples of beam current (2)

中心領域加速試験20 0 9 / 1 1 / 1 2 R= 5 0 m m

0 .0

0 .5

1 .0

1 .5

2 .0

2 .5

1 5 :5 0 1 6 :0 4 1 6 :1 9 1 6 :3 3

時間

メインプローブ電

(mA)

30min

Beam current at central region of HMBeam current at central region of HM--3030

Beam current at central region is very stable, and current at central region is very stable, and exceeds 2mAexceeds 2mA

TimeTime

Bea

m c

urre

nt

Bea

m c

urre

nt

(mA

)(m

A)

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22--7. Irradiation system7. Irradiation system

Irradiation Port Horizontal, Fixed (1set)Thermal Neutron Flux(at 20mm depth in the water phantom)

1.8×109n/cm2/sec/mAField Size 250mm×250mmTreatment Couch Bed and Chair

(Changeable) Patient Positioning Laser Marker and X-ray system

1.5m

CollimatorCollimatorLaser MarkerLaser Marker

Treatment CouchTreatment Couch

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22--8. Neutron yield8. Neutron yield

Target

Fast neutrons are moderated to epithermal regionFast neutrons are moderated to epithermal region

fast neutron

Irradiation Port

epithermal neutron

Neu

tron

yie

ld p

er le

thar

gy (n

/cm

2 /s/m

A)

Iron

CaF2

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22--9. Neutron flux at 1mA9. Neutron flux at 1mA

0.00E+00

2.00E+08

4.00E+08

6.00E+08

8.00E+08

1.00E+09

1.20E+09

1.40E+09

1.60E+09

1.80E+09

2.00E+09

0 20 40 60 80 100 120 140 160 180Distance from surface (mm)

Ther

mal

neu

tron

flux

(neu

tron

s/cm

2 /s @

1mA)

CalculationMeasurement

Attained enough neutrons for treatmentAttained enough neutrons for treatment

1.8×109 n/cm2/sthermal neutrons

MCNPXcalculation

Measurement

WaterWater Phantom Phantom

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3. Schedule and Future Plan3. Schedule and Future Plan

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2008/92008/9 Installed in KURRIInstalled in KURRI2009/12009/1 Commissioning Test StartedCommissioning Test Started2010/2 2010/2 DosimetryDosimetry and Cell / Animal Test and Cell / Animal Test

CompletedCompleted

Now we are working for obtaining approval of Now we are working for obtaining approval of medical product registration in FY2012medical product registration in FY2012

33--1. Schedule1. Schedule

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SummarySummary

Kyoto university and Sumitomo developed a BNCT system using 30 MeV H- cyclotron.

Peak thermal neutron flux is 1.8x109 n/cm2/sec in a water phantom, which is enough for a BNCT treatment.

We finished animal tests in 2010. Now we are working for obtaining approval of medical product registration in FY2012.

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Thank you for your attentions!Thank you for your attentions!