NIRS-M- 257 Joint Symposium 2013 on Carbon Ion Radiotherapy
Joint
Joint Symposium Symposium 2013 2013 on on Carbon
Carbon Ion Ion Radiotherapy Radiotherapy
Fostering International Collaboration between Japan and the United States
May 2-3, 2013
DoubleTree Hotel Rochester, Minnesota
A two day symposium sponsored by:
Mayo Clinic Department of Radiation Oncology, Japan National Institute of Radiological Sciences, and Northern Illinois University Institute for Neutron Therapy at Fermilab
JAPAN
USA Mayo Clinic
Department of Radiation Oncology Phone: 507-255-2297
Fax: 507-284-0079 [email protected] [email protected]
Phone: +81-43-206-3025 Fax: +81-43-206-4061
4-9-1 Anagawa, Inage-ku, Chiba 263-8555, Japan Research Promotion Section
National Institute of Radiological Sciences
NIRS-M- 257
Joint Symposium 2013 on Carbon Ion Radiotherapy
Fostering International Collaboration between Japan and the United States
- 13 th NIRS Charged Particle Therapy Research Center Symposium -
May 2-3, 2013
Double Tree Hotel Rochester, Minnesota
A two day symposium sponsored by:
Mayo Clinic Department of Radiation Oncology, Japan National Institute of Radiological Sciences, and Fermi Lab National Accelerator Laboratory/Northern
Illinois University
Dear Colleagues,
We are pleased to welcome you to the Inaugural Joint Symposium on Carbon Ion Radiotherapy on May 2nd and 3rd at the Double Tree Hotel in Rochester, Minnesota.
This two-day symposium on carbon ion radiotherapy is sponsored jointly by Mayo Clinic, the NIU Institute for Neutron Therapy at Fermilab and the National Institute of Radiological Sciences (NIRS) of Japan.
On Day One, physicians from NIRS will present the latest clinical results with carbon ion therapy. There will also be an update on the Heidelberg Ion Therapy Center (HIT) in Germany, the European Network for Light Ion Therapy (ENLIGHT), presentations on the US Vision for hadron therapy from Mayo Clinic and Fermilab/NIU, and relevant radiobiology talks. Day Two will be devoted to presentations and discussions regarding the technology challenges, novel accelerator technologies, beam delivery and gantry designs for ion therapy.
We look forward to a very productive meeting with you all.
Robert C. Miller, M.D.
Mayo Clinic
James S. Welsh, M.D.
NIU Institute for Neutron Therapy at Fermilab
Tadashi Kamada, M.D., Ph.D.
National Institute of
Radiological Sciences, Japan
INDEX
Session 1: Clinical Presentations-NIRS Experience
History of Ion Beam Therapy ・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
Hirohiko Tsujii, NIRS
1
Overview of the Carbon Ion Therapy at HIMAC (Including Head and Neck Tumors, and Bone and Soft Tissue Sarcomas) Tadashi Kamada, NIRS
18
Carbon Ion Radiotherapy in a Hypo-fractionation Regimen for StageⅠNon-Small Cell Lung Cancer・・・・・・・・・
Naoyoshi Yamamoto, NIRS
35
Carbon Ion Radiotherapy for Liver Cancer and Prostate Cancer・・・・・・・・・・・・・・・・・・・・・・・・・・
Hiroshi Tsuji, NIRS
46
Carbon Ion Radiotherapy for Patients with Locally Recurrent Rectal Cancer and Pancreas Cancer・・・・・・・・・・
Shigeru Yamada, NIRS
59
Session 2: U.S. and European Perspectives on Carbon Ion Radiotherapy & Radiobiology
Radiobiology of Hypofractionated Radiotherapy・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
David J. Brenner, Columbia
79
Technical and Biological Strategies to Improve the Therapeutic Window in Modern Radiation Oncology・・・・・・・・
Stephanie E. Combs, HIT
* The pages from 87 to 97 are not available in the E-book at request of the author but included in the printed version.
87
ENLIGHT: An Effective Network for Hadron-therapy? ・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
Manjit Dosanjh, CERN/ENLIGHT
98
Mayo Clinic Vision for Light Ion Therapy・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
Robert C. Miller, Mayo
108
Challenges and Opportunities in Particle Radiation Therapy Research・・・・・・・・・・・・・・・・・・・・・・・・
Bhadrasain Vikram, NIH
116
Current Status & Future Vision: Particle Radiobiology・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
Eleanor A. Blakely, Berkeley
117
Session 3: NIRS Experience with Ion Beam Technologies
Overview of NIRS Accelerator Activity ・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
Koji Noda, NIRS
131
New Particle Therapy Facility in NIRS, Present and Future Plan・・・・・・・・・・・・・・・・・・・・・・・・・
Toshiyuki Shirai, NIRS
141
Modeling the Clinical and Biological Effect of Therapeutic Carbon Ion Beam・・・・・・・・・・・・・・・・・・・
Naruhiro Matsufuji, NIRS
149
NIRS Scanning System: Present Status and Future Prospects・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
Takuji Furukawa, NIRS
157
TPS for NIRS Scanning: Present Status and Future Prospects・・・・・・・・・・・・・・・・・・・・・・・・・
Taku Inaniwa, NIRS
164
Multi-dimensional Image Guided Particle Therapy・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
Shinichiro Mori, NIRS
176
Session 4: US Ion Beam Technologies and Perspectives for the Future
Proton and Carbon Ion CT Imaging for Treatment Planning in Ion Therapy ・・・・・・・・・・・・・・・・・・・・・・・・・・・
George Coutrakon, NIU
187
Advanced Accelerator Technologies for Ion Therapy ・・・・・・・・・・・・・・・・・・・・・・・・・・・・・・
Carol Johnstone, Fermi Lab
194
Joint Symposium 2013 on Carbon Ion Radiotherapy
Fostering International Collaboration between Japan and the United States in Carbon Ion Radiotherapy
A two day symposium sponsored by:
Mayo Clinic Department of Radiation Oncology Japan National Institute of Radiological Sciences
Northern Illinois University Institute for Neutron Therapy at Fermilab Double Tree Hotel, Rochester, MN – May 2-3, 2013
Thursday, May 2, 2013: Clinical Practice, Development Opportunities, and Radiobiology
Time Speakers and Topics
8:00 a.m. Breakfast and Registration Check In 8:30 a.m. Welcome and Introductions
1. Mayo Welcome – Robert C. Miller, M.D.
2. NIRS Welcome – Tadashi Kamada, M.D., Ph.D.
3. NIU/Fermi Lab Welcome – James S. Welsh, M.D.
8:45 a.m. Presentation of Symposium Goals – Michael G. Herman, Ph.D. (Mayo) Session 1: Clinical Presentations – NIRS Experience
Chair, Tadashi Kamada, M.D., Ph.D. (NIRS)
9:00 a.m. History of Ion Beam Therapy Hirohiko Tsujii, M.D., Ph.D. (NIRS)
9:30 a.m. Overview of the Carbon Ion Therapy at HIMAC (Including Head and Neck Tumors, and Bone and Soft Tissue Sarcomas)
Tadashi Kamada, M.D., Ph.D. (NIRS) 10:00 a.m. Break
10:30 a.m. Carbon Ion Radiotherapy in a Hypo-fractionation Regimen for Stage Ⅰ Non-Small Cell Lung Cancer
Naoyoshi Yamamoto, M.D., Ph.D. (NIRS)
11:00 a.m. Carbon Ion Radiotherapy for Liver Cancer and Prostate Cancer Hiroshi Tsuji, M.D., Ph.D. (NIRS)
11:30 a.m. Carbon Ion Radiotherapy for Patients with Locally Recurrent Rectal Cancer and Pancreas Cancer
Shigeru Yamada, M.D., Ph.D. (NIRS)
12:00 p.m. Lunch
Session 2: U.S. and European Perspectives on Carbon Ion Radiotherapy &
Radiobiology
Chair – Robert C. Miller, M.D. (Mayo)
1:00 p.m. Radiobiology of Hypofractionated Radiotherapy David J. Brenner, Ph.D. (Columbia)
1:25 p.m. GSI/HIT Experience with Carbon Ions Stephanie E. Combs, M.D. (HIT)
1:50 p.m. ENLIGHT Vision for Hadron therapy Manjit Dosanjh, Ph.D. (CERN/ENLIGHT)
2:15 p.m. Fermi/NIU Vision for Hadron therapy James S. Welsh, M.D. (NIU/Fermi)
2:40 p.m. Mayo Clinic Vision for Hadron therapy Robert C. Miller, M.D. (Mayo)
3:05 p.m. Break
3:35 p.m. Challenges and Opportunities in Particle Radiation Therapy Research Bhadrasain Vikram, M.D. (NIH)
4:00 p.m. Current Status & Future Vision: Particle Radiobiology Eleanor A. Blakely, Ph.D. (Berkeley)
4:30 p.m. Conclusion of Day #1 Discussion
Friday, May 3, 2013: Technology and Physics Presentations Time Speakers and Topics
8:00 a.m. Breakfast
Session 3: NIRS Experience with Ion Beam Technologies Chair – Koji Noda, Ph.D. (NIRS)
8:30 a.m. Overview of NIRS Accelerator Activity Koji Noda, Ph.D. (NIRS)
9:00 a.m. New Particle Therapy Facility in NIRS, Present and Future Plan Toshiyuki Shirai, Ph.D. (NIRS)
9:30 a.m. Modeling the Clinical and Biological Effect of Therapeutic Carbon Ion Beam
Naruhiro Matsufuji, Ph.D. (NIRS)
10:00 a.m. NIRS Scanning System: Present Status and Future Prospects Takuji Furukawa, Ph.D. (NIRS)
10:30 a.m. Break
11:00 a.m. TPS for NIRS Scanning: Present Status and Future Prospects Taku Inaniwa, Ph.D. (NIRS)
11:30 a.m. Multi-dimensional Image Guided Particle Therapy Shinichiro Mori, Ph.D. (NIRS)
12:00 p.m. Lunch
Session 4: US Ion Beam Technologies and Perspectives for the Future Chair – Michael G. Herman, Ph.D. (Mayo)
1:00 p.m. DOE Perspective on Technology for Ion Therapy Michael Zisman, M.D. (DOE)
1:15 p.m. Ion Workshop Summary Clinical/Radiobiology John O’Connell, M.D. (Walter Reed)
1:45 p.m. Ion Workshop Summary Accelerator and Delivery Chris J. Beltran, Ph.D. (Mayo)
2:15 p.m. Carbon/Proton CT Image-Guidance George Coutrakon, Ph.D. (NIU)
2:45 p.m. Advanced Accelerator Technologies for Ion Therapy Carol Johnstone, Ph.D. (Fermi Lab)
3:15 p.m. Carbon Ion Therapy for Cardiac disease Douglas L. Packer, M.D. (Mayo)
3:45 p.m. Discussion of Symposium Goals
4:45 p.m. Tour of Mayo Clinic and Proton Beam Therapy Program Site
H. Tsujii
National Institute of Radiological Sciences (NIRS) Joint Symposium 2013 on Carbon Ion Radiotherapy Fostering International Collaboration between Japan and the United States
in carbon ion radiotherapy Double Tree Hotel, Rochester, MN – May 2-3, 2013 Joint Symposium 2013 on Carbon Ion Radiotherapy Fostering International Collaboration between Japan and the United States
in carbon ion radiotherapy Double Tree Hotel, Rochester, MN – May 2-3, 2013
History of Ion Beam Therapy
History of Ion Beam Therapy
Neon Carbon Neutron Proton Pion Electron X-ray
γ-ray 20Ne
12C
Mass 20 : 12 : 1 : 1 : 1/7 :1/1800 : -
1n 1
p
π- e-
nnn n
nn P P PP
P P Carbon Carbon
Carbon ion Carbon nucleus(6+)
CO2 CH4
nnn nn P P PP
P n P
P P Hydrogen
Hydrogen Proton
(1+)
治療に用いられる粒子線
Nuclei of the atoms that are accelerated to near the light speed is called charged particle beams.
Sir W. H. Bragg, Adelaide, Australia
Ionization density of air increased at end of range in Ra α rays
(Bragg, WH, and Kleeman, R, “On the Ionization Curves of Radium,” Philosophical Magazine, 8: 726-738 (1904).
Bragg curve
•
LET: 20 40 60 80
RBE: 2.0 2.3 2.5 3.0
LET & RBE Values used in Clinical Study
(Carbon ion, 290MeV, SOBP=60mm)
RelativeDose
Density of ionization increases with depth
Bragg-peak Plateau
Equivalent to fast neutron
Peak-to-Plateau Ratio of RBE
for Jejunal Crypt Cell RBE
sdRBE
2Ion Peak/Plateau Ratio Peak/Plateau Ratio
Proton 1.2/1.1 1.1 1.3/1.2 1.1
Helium 1.2/1.1 1.1 1.5/1.3 1.2
Carbon 1.4~1.5/1.3 1.1~1.2 1.6~2.2/1.3 1.2~1.7 Neon 1.5~1.6/1.4 1.1 2.6~3.0/2.1 1.2~1.4 Argon 1.8~2.0/2.1 0.9 3.6~3.8/4.3 0.8~0.9 RBEsd:single dose, RBE2: fractionated
(Goldstein et al.: Radiat. Res. 86, 542-558, 1981)
Carbon-ions have the best balance in terms of dose distribution and
increasing biological effect with depth.
Carbon Proton
Beam Spots vs. Depth - protons and carbon ions -
Carbon
Proton Carbon (285MeV/u)
Proton (150MeV/u)
Comparison of Dose Distribution with Broad Beams
(Courtsy of Dr Murakami, Hyogo)100% 50% 90%
10% 90% 30% 50% 100%
0 20 40 60 80 100 120
0 50 100 150 200 250
深さ(mm)
相 対 線 量
0 20 40 60 80 100 120
0 50 100 150 200250 深さ(mm)
相 対 線 量
Proton Beam Carbon Ion Beam
RelativeDose
RelativeDose
Depth (mm) Depth (mm)
History of Particle Beam RT
Year
1895 Discovery of X-rays 1896 First use of x-rays for RT 1903 Discovery of Bragg peak 1931 First construction of Cyclotron 1946 Proposal for use of ion beam for RT 1954 First proton therapy at LBNL 1961 Proton therapy started at MGH/HCL 1973 Development of CT
1975 First heavy ion therapy at LBNL 1990 Hospital-based proton center atLLUMC 1994 C-ion RT started at NIRS, Japan 1997 C-ion RT started at GSI, Germany(until 2008) 2002 C-ion RT started at Hyogo, Japan 2006 C-ion RT started at Lanzhou, China 2009 C-ion RT started at Heidelberg, Germany 2010 C-ion RT started at Gunma, Japan
W.H.Bragg
E.Lawrence
R. Willson
G.Hounsfield
E.O. Lawrence developed Cyclotron
• Inspired by a paper from Norwegian engineer Rolf Wideroe, Lawrence invented a unique circular particle accelerator, which he referred to as his "proton merry-go- round," but which became better known as thecyclotron(1931).
• Lawrence’s first cyclotron, all of4 inches in diameter, was small enough to hold in one hand. This tiny apparatus of brass and sealing wax, which cost about $25 to build, successfully accelerated hydrogen molecular ions to 80,000 volts.
1932-The 11-Inch Cyclotron,1 pA of 1.2 MeV protons, was housed in a laboratory without shielding.
1937- Historic37-Inch Cyclotron, 8 MeVd (displayed at the Lawrence Hall of Science)
1939 -The 60-Inch Cyclotron, deuteronsto 19 MeV.
•Robert Stone and John Lawrence
→Fast neutron therapy.
•Melvin Calvin used C14as a tracer to study photosynthesis (Nobel prize).
QuickTime™and a decompressor are needed to see this picture.
1931- The invention of Cyclotron,4-inchdiameter, 80 keV protons → then 9-inch
1933 -The 27-Inch Cyclotron, 4.8MeV p and d, was installed in the Rad Lab on the UC Berkeley campus.
Courtesy of W.Chu
→ 1stfast neutron therapy in 1939
Fast neutron therapy
by Robert Stone and J Lawrence (1937-1943)
Currently
• Nearly all Centers Closed
• Unacceptably high NTCP
• In TCP, except for low/tumors?
• RBE Normal > RBE Tumor
Author Site No. Cont- Compli- Survival
rolled cation
Caterall (1979) Soft 28 75% 32% -
Ornitz (1980) B&S 20 65% - -
Salinas (1980) B&S 34 62% 12% 59%(5-62mo)
Battermann(1981) B&S 22 36% 27% -
Cohen (1984) B&S 51 47% 38% 39% (>2yr)
Schmitt (1983) Soft 60 50% - -
(1982) Bone 24 50% 33% -
Wambersie (1984) Soft 22 18% 18% -
Duncan (1986) B&S 30 38% 50% -
Schwarz (1998) Soft 1171 50% - -
Local Control, Complications and Survival
in Neutron Therapy for Bone/Soft Tissue Sarcomas
Carbon-ion Therapy in Bone & Soft Tissue Sarcomas Local Control and Morbidity by Dose
50%
(3/6) 67%
(10/15) 81%
(13/16) 87%
(19/23) 89%
(26/29)
0%
(0/6) 0%
(0/15) 0%
(0/16) 6%
(4/61) 33%
(9/27)
70.4 GyE/16fx/4wk
Robert Wilson proposed the use of Bragg Peak for RT in1946.
R.R. Wilson
Dose localization
•Lower entrance dose
•No or low exit dose
•In 1947, the 184-inch cyclotron produced its first high-energy proton beams (380MeV).
•In 1954, the first patient with disseminated breast cancer was treated with protons.
Berkeley
1931: Invention of cyclotron (Ernest Lawrence)
1946: RR Wilson published his seminal paper on particle therapy 1952: Firstbiological investigation with accelerated nuclei
(C Tobias and JH Lawrence)
1954: First therapeutic exposure of humans to protons and alphas (Tobias and JH Lawrence)
1975: Clinical trials with accelerated light ions at LBL (Castro) Gustav Werner Institute and Theodor Svedberg Lab
1949: Synchrocyclotron at the Gustav Werner Institute (Uppsala) 1950s: Pre-therapeutic experiments with protons (B. Larsson) 1957: First patient treated with proton beam
1994: The cyclotron was upgraded Harvard Cyclotron Laboratory
1938: First Harvard Cyclotron completed (Bainbridge, Street and Hickman) 1943: Moved the cyclotron to Los Alamos (RR Wilson)
1949: Second Harvard Cyclotron completed (Norman F. Ramsey): 95-110 MeV protons 1955: Second Harvard Cyclotron: 160 MeV protons
1962: Proton radiotherapy - first steps (Sweet, Kelleberg) 1972: Clinical trials with protons (Suit, Koehler, Goitein, Richard Wilson)
Early History of Proton and Ion-Beam Therapy 1904 WH Bragg and R Kleeman, “On the ionisation curves of radium,” Phil. Mag. 8 (1904)
Sites USA Europe USSR Japan Total Eye (Melanoma) 1,698 2,196 355 44 4,293 35.1%
Skull base &
Intracranial tumor 3,132 15 1,678 58 4,883 39.9%
Head & neck 79 20 0 21 120 1.0%
Thorax & abdomen 2 0 0 127 129 1.1%
Pelvis(incl Prostate) 469 41 242 61 813 6.6%
Others 18 12 77 128 235 1.9%
Unknown 709 27 1,025 0 1,761 14.4%
Total 6,107
(49.9%) 2,311 (18.9%)
3,377 (27.6%)
439 (3.6%)
12,234 (100%)
%
Proton Therapy Facilities and Number of Patients by Tumor ( 1993.05 )
In the initial phase of proton therapy, indications were mainly focused on ocular melanoma and skull base/intra-cranial neoplasmas.
Proton Medical Research Center of Tsukuba University
(1983-2000 : n=700)Booster Synchrotron of KEK Liver34.0%
Lung8.3%
Head & neck6.0%
Skull base6.3%
In proton therapy at Tsukuba University, in advance of the world, major efforts have been placed on treatment ofdeep-seated organsincluding the liver, lung, esophagus as well as the head and neck and bladder.
Esophagus8. 6%
Uterus4.1%
Bladder5.4%
Prostate3.8%
Others12.6%
Metastatic tumor5.1%
Anteriovenous malformation5.4%
R.R. Wilson and C.A. Tobias for Hadron Therapy
Cornelius A. Tobias
1948: Biology experiments using protons 1952: Human exposure to accelerated p, d, He 1954: 1
sttherapeutic exposure of PBT to humans 1957: 1
stReport of PBT of humans
1956-1986: Clinical Trials:
1,500 patients treated with p and He
1st He pat 06/75 1st C pat 05/77 1st Ne pat 11/77 1st Ar pat 03/79 1st Si pat 11/82
Clinical Trials at LBNL/Bevalac, 1975–1992
J.R. Castro conducted clinical trials at LBNL.
1975-1993
He ions = 2,054 pats Neon ions = 433 pats Other ions = 23 pats
Biomed Facility
Carbon ion / EB Doses 10 MeV Electrons :
25, 30, 35 Gy/10 fxs/12 days 308 MeV Carbon:
10,14,17 Gy/10 fxs/11 days
Courtesy of J. Castro
1988
• Early RBE values:
about 2.8-3.0
• Late skin RBE:
~3.0~3.3
( 7-10 years post Rx)
Carbon ion RBE for skin treatment
Clinical Impressions - LBL Heavy Ion trial-
• Potential tumor effectiveness in salivary, bone & soft tissue, bile duct tumors.
• Increased effect in slow growing tumors, hypoxic tumors.
• Increased RBE /normal tissue damage with Neon ions, esp. CNS, GI tract (with 1980’s techniques ).
• Silicon ions : accelerated skin /subcutan damage.
• CARBON IONS MIGHT BE BEST ION FOR CLINICAL TRIAL.
Unfortunately, after > 1,400 patients were
treated the Berkeley facility was closed in 1992
History of Particle Beam RT
Year
1895 Discovery of X-rays 1896 First use of x-rays for RT 1903 Discovery of Bragg peak 1931 First construction of Cyclotron 1946 Proposal for use of ion beam for RT 1954 First proton therapy at LBNL 1961 Proton therapy started at MGH/HCL 1973 Development of CT
1975 First heavy ion therapy at LBNL 1990 Hospital-based proton center atLLUMC 1994 C-ion RT started at NIRS, Japan 1997 C-ion RT started at GSI, Germany(until 2008) 2002 C-ion RT started at Hyogo, Japan 2006 C-ion RT started at Lanzhou, China 2009 C-ion RT started at Heidelberg, Germany 2010 C-ion RT started at Gunma, Japan
J.Castro
Y. Hirao H.Tsujii
G. Kraft J. Debus
T. Kanai T. Nakano Y. Hishikawa
At the PTCOG held in NIRS (1992)
HIMAC
New Treatment Building
Scanning Rotating gantry 1994 Broad beam irrad
2011 Active scanning
Treatment rooms Biological Experiment Ion
Source Linear
Accelerators
Main Accelerator (Synchrotron)
HIMAC
(HeavyIonMedicalAccelerator inChiba)Progress of C-ion RT at NIRS
• Since 1994, carbon ion RT has been focused on development of irradiation technique and dose- fractionation for various types of tumors at NIRS.
• The total number of patients treated by March 2013 is > 7,000 pats.
• The number of the patients enrolled has
increased year after year. This increase is due to the fact that the treatment regimen has become established and smoothly executed as well as the number of fractions and treatment period per patient has been significantly reduced.
RBE vs Fraction Size in Carbon Ion Irradiation
2.2 2.4 2.6 2.8 3 3.2 3.4
2 4 6 8 10 12 14
P.77DoseRBE/010219
77 keV/mm 1.4
1.6 1.8 2 2.2 2.4
0 5 10 15 20
P.42DoseRBE/010219
42 keV/mm
Dose per Fraction(Gy)
Skin
Tumor
Skin
Tumor Dose per Fraction(Gy)
Dose per Fraction(Gy)
Skin
Tumor 1.2
1.4 1.6 1.8 2 2.2
0 5 10 15 20 25 30
P.20DoseRBE/010219
skin tumor
20 keV/mm
Koike S, et al: Radiat Prot Dos. 2002;99: 405-408.
Ando et al. : J.Radiat.Res.,46:51-57, 2005
Single fraction RT with C-ions 34GyE
Pneumonitis appeared corresponding to the high dose area.
. 67 y/o、M
S4, 70mm 72.0GyE/15frs
5 yr
73 y/o, M S1、48mm 66.0GyE/12frs
2.5 yr
.
1 yr 72 y/o, M S1、46mm 52.8GyE/4frs
. 71 y/o, M S7, 11.2cm 48.0GyE/2frs
2 yr
Chordoma of the Sacrum
3.5 yrs after Case 1.81 y.o.M.
Case 3.83 y.o. M.
Case 2.57 y.o.F.
4.5 yrs after 4 yrs after
Carbon Ion RT
• An advantage for C-ion RT over proton or x-ray RT, suggesting higher biological effects of C-ions, has been demonstrated in:
H&N: Non-SCC (ACC, MM)
Skull base and sacrum: Chordoma, Chondrosarcoma Lung: NSCLC (T2 tumor)
Pelvis and para-spinal regions: B&S sarcoma Prostate: intermediate and high risk group Post-ope local recurrent tumor of rectal cancer Renal cell cancer
• Incidence of GIII late injury was lower for C-ion RT in
chordoma of the skull base, sacral chordoma, H&N tumor,
stage I NSCLC, prostate ca and pancreas ca.
Outline of Carbon Facilities in Operation in the World
Institute /Hospital
Location (Country)
Start year Rooms
Irradiation method
Max.
Energy MeV/u
Operation schedule NIRS (Japan)Chiba 1994 ~ 3+2 Layer stackingWobbler
HybridScanning
400(C) 24 hours /6 days /10 month
GSI Darmstadt(Germany) 1997~2008 1 RasterScanning 400(C) 3 blocks /year
HIBMC (Japan)Hyogo 2001~ 5 Wobbler 320(C) 230(p)
16 hours / 5 days /12 month
IMP Lanzhou(China) 2006~ 2 Layer stackingWobbler 100 for V 400 for H
24 hours /7 day /variable
HIT
Heidelber g (Germany)
2009~ 3 RasterScanning 430(C)
250(P) 16 hours / 5 days /12 month
GHMC Gunma(Japan) 2010~ 3 Layer stackingWobbler 400(C) 8 hours / 5 days /12 month CNAO Pavia(Italy) P: 2011~(C: 2012) 3 RasterScanning 400(C)
250(P) 220 days/yr
Outline of facilities under Construction or Planning
Institute
/Hospital Location Country Start
year Ion Room Irradiation
method Max. Energy MeV/u Fudan
University
Shanghai
China 2013 C
P 3 Scanning 430 (C)
250 (p)
SAGA-HIMAT Saga
Japan 2013 C 3 Wobbler /
Scanning 400 (C) EBG
MedAustron Wiener Neustadt
Austria 2015 C
P 3 Scanning 400 (C)
iROCK
Kanagawa CC Kanagawa
Japan 2015 C 4 Wobbler /
Scanning 400 (C) PTC
UKGM
Marburg Germany
2013
? C
P 4 Scanning 430 (C)
250 (p)
ETOILE Lyon
France 2016? C 3 Wobbler 400 (C)
KIRAMS Pusan
Korea 2016
? C 3 Scanning 400 (C)
GSI: principle of beam scanning (1997 - 2009)
In order to get an exact positioning of the target volume the head of the patient is fixed with an individually manufactured mask.
The end of the beam pipe with ionization and multi-wire chambers for the beam control is visible at the left side. During irradiation, the PET cameras above and below the ionization chambers are placed over the patient.
clinical dose (3.3GyE to chordoma)
ID: CIZ251-#44 (FEB05)
clinicaldose[GyE]
Red: GSI
White: HIMAC
~20%
Tumors eligible for C-ion RT so far are:
* Skull base tumours:
o
chordoma
ochondrosarcoma
omal. schwannoma
oatyp. meningeoma
oadenoidcystic ca.
* Tumours close to spinal cord:
o
sacral chordoma
ochondrosarcoma
osoft tissue sarcoma
* rapidly growing tumours
* metastasizing tumours
* by law: children under 18 Tumors which
are not eligible right now are:
Experiences of GSI (Germany)
• Compact design 60m x 70m
• Raster scanning
• World-wide first ion gantry
• >1000 pats (>15.000fr/yr)
• Low-LET modality:
Protons(later He)
• High-LET modality:
Carbon(Oxygen)
• Ion selection within minutes
Heidelberg Ion Therapy Center (HIT)
(2009~ )
19 Novembre 2009 37
Carbon Ions Clinical Protocols at CNAO
• Chordoma/Chondrosarcoma of Skull Base
• Chordoma/Chondrosarcoma of Column
• H&N Adenocarcinoma
• Salivary glands tumours
• Mucosal & Skin Melanomas
• Bone & Soft Tissue Sarcomas of H&N
• Bone & Soft Tissue Sarcomas of other sides
• Lung
• Digestive Tract
Centro Nazionale di Adroterapia Oncologica (The National Center for Oncological Hadrontherapy)
Proton Carbon
38
MedAustron : Ground floor – functional design
ÖGRO, 20.11.2010
Personaleingang (Medizin, Forschung, Technik) RettungPatienten
137 m
90m
M. Benedikt Synchotron
1 Research room – horizontal fixed beam 3 Treatment rooms
Horizontal and vertical fixed beam
Protons and carbon ions
Horizontal fixed beam
Protons and carbon ions
Gantry(-30/+180) in cooperation with PSI
Protons
Shanghai Particle Therapy Hospital (SPTH) Siemens Synchrotron
Proton 50-250MeVandCarbon 85-430MeV/u Slow extraction of beam over 1-10 s Shift from carbon to proton: less than 1 min.
Proton
Carbon Fudan University
Shanghai Cancer Center (FUSCC)
•Staff: 1800
•In-patient bed: 1250
•2009 workload: Surgery 13,743;
In-pts 18,722 pts Out-pts 516,638
In operation
In planning stage or under construction Gunma University Heavy Ion Medical CenterGunma University Heavy Ion Medical Center
HIMAC, NIRS
Kanagawa Cancer Center Hyogo Ion Beam Medical Center
(Carbon, Proton) Hyogo Ion Beam Medical Center
(Carbon, Proton) SAGA-HIMAT
Carbon Ion Therapy Facilities in Japan
Ion beam therapy in Hyogo (HIBMC)
Proton Carbon-ion
•Energy 70 - 230 MeV 70 - 320 MeV/u
•Range 4 - 30 cm 1.3 - 20 cm
•Gantries 2 none
•Fixed beams 3 (H/V + H) 3 (H/V + Oblique)
Development of Compact Accelerator Development of Compact Accelerator
Ion source
120m
65m
45m
57m R&D for small-sizing
(2004~2005)
prototype Gunma University
NIRS
Catalog product for spread HIMAC
SAGA-HIMAC
1/3
Small-size and less expensive machine with high performance
Ion generator
Linear accelerator Treatment rooms
synchrotron
PET/CT MRI
simulator
Ent
20m R&D room
Building :60 m x 45 m and 15 m in height
Rooms: 3 rooms (A:horizontal, B:hori.+vert., C: vertical ) for clinic and 1 room for research
Synchrotron:20 m in diameter
Ion species:Carbon only,Max energy:400 MeV/n ( 25 cm in water) Field size:22 cm in diameter, Dose rate:5 GyE/ minute
Gunma University Heavy Ion Medical Center
Research port
A B C
Development of Charged Particle Facility at NIRS
・He~Ar
・Emax800MeV/n
・Wobbler method
・Respiratory gating
・Broad beam method
HIMAC Compact Facility at
Gunma
・C
・Emax400MeV/n
・Spiral wobbler
・Respiratory gating
・Stack layer irrad
New Treatment Research Facility
・C, O,(11C,15O)
・Emax430MeV/n
・Respiratory gating
・3D Scanning
・Rotating gantry
Photograph of a New Facility
Building facade with green curtain Entrance hall (1F)
Waiting hall (B2F) Treatment Room E (B2F) NIRS, TOSHIBA Co.
NIHON SEKKEI, Inc.
High conformation to irregular shape
High beam efficiency
No need to use bolus and collimator
scanning
magnets range shifter ( tentative)
New Beam Delivery Technique
• Broad-beam
Kanai et al. IJROBP1999, 44:201-210scatterer wobbler
magnets ridge filter compensator collimator
• Scanning
Variable energy( up to147 energies)
100 120 140 160 180 200
-40
-20
0
20
40
Non-gating
Gating Gating
with rescanning (8 times)
100 120 140 160 180 200
-40
-20
0
20
40
100 120 140 160 180 200
-40
-20
0
20
40
0 0.1 0.2 0.3 0.4 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.1
Motion:7mm in gate
Simulation of moving tumor irradiation
In order to avoid hot/cold spot due to target motion, we decided to employ “gating method” with rescanning.
Example:
Φ40mm spherical target
Moving Target Irradiation ~ NIRS approach
Fast Scanning is the key technologyfor completing rescanning within a short time.
How many pats need particle therapy?
Author Type oof Study Conclusion
Bengt (Sweden)
Rad Onc, Physicist, Tumor registry states for Sweden , literature,
# getting RT
2200 – 2,500 / year or
14 ~ 15% of all RT pats Orrecchia (Italy) Estimated based # RT pts 16%
Baron (France) Estimated based # RT pts 14.5%
Mayer (Austria) Estimated based # RT pts 13.5%
Mack Roach III (USA) Estimated based # RT pts SF-Bay area > 1,848/yr
Tsujii (Japan)
Estimated based # RT pts, literature, Statistices, # RT pts
6.5%
Thank You
Tadashi KAMADA, MD
Research Center for Charged Particle Therapy National Institute of Radiological Sciences, Chiba, JAPAN
Over view of Carbon Ion Therapy at HIMAC
(Including Head & Neck Tumors, and Bone & Soft Tissue Sarcomas)
Room for scanning Fusin of auto-activation
& dose distribution in scanning NIRS, Mayo Clinic, and Fermi Lab/NIU Joint Symposium 2013 on Carbon Ion Radiotherapy
Double Tree Hotel, Rochester, MN - May 2-3, 2013
Particle Therapy Research at NIRS
1975-1994 Neutron therapy( about 2000 patients) 1979-1995 Proton therapy (less than 150 patients) 1984~ Heavy ion cancer treatment project 1994~ Carbon ion clinical trial using HIMAC 2003~ Carbon ion “clinical practice” approved 2010~ Compact C-ion facility(1/3size&cost) at Gunma 2011~ Pencil beam scanning clinical application 2013 ~ Almost 8,000 patients received CIRT
Neon
Carbon
Neutron Proton Pion Electron X-ray20
Ne
12
C
1
n
Relative mass
: 12 :1
π
-e
-1
p
Why Carbon Ion Beam ?
Rationale
• High conformality
• High biological effects Carbon ion beam
A suitable beam for cancer treatment Severe DNA damage
Lessons in
“Neutron therapy”(1975-1994)
High “LET” beam “without” high physical selectivity could never be a major player in
radiation oncology.”
Key point : High LET beam with high physical selectivity(conformality)
Lessons in
“LBNL Ion Therapy”(1975-1992)
Ions for cancer treatment
Heavier than carbon ion like neon ion : High LET at entrance : Risk of normal tissue!
Lighter than carbon ion like helium
: Lower LET at peak : Less biological advantages!
Key point : Not so Heavy and Not so Light !
Not so Heavy and Not so Light-
Carbon is a well balanced particle for cancer treatment !
possesses optimal properties in terms of biologically effective dose localization.
“Four Rs” in Radiobiology
From E. Hall : Radiobiology for the Radiologist
1920~1930s in Paris
Repair
Redistribution Reoxygenation Repopulation
0 20 40 60 80 100
0 20 40 60 80 100 120 140 160
TUMORCONTROL(%)
DOSE (Gy) γ-ray
Single fraction
5 Fractions
0 20 40 60 80 100
0 20 40 60 80 100 120 140 160
TUMORCONTROL(%)
DOSE (GyE) Carbon
74 keV/mm
Single fraction
5 Fractions
γ-ray Carbon
5 fractions
Ando et al. unpublished data at NIRS
Repair
Comparison of radiation cell survival levels in synchronized CHO cells irradiated with 4 Gy X-rays
and 2 Gy 70 keV/µm carbon ions.
Kato et al. unpublished data at NIRS
0.0001 0.001 0.01 0.1 1
0 5 10 15 20 25 30 35
Survivngfraction
Dose (Gy)
γ-ray
Hypoxic
Oxic
0.001 0.01 0.1
10 5 10 15 20 25 30 35
Survivingfraction
Dose (GyE)
carbon
74 KeV/ hypoxic
74 KeV/ oxic Oxygen effect
γ-ray Carbon
hypoxic oxic
Ando et al. Int J Radiat Biol 1999
Beyond “4 Rs” with Hypo-F CIRT
Low repair
Cell cycle non-specific
Low OER(re-oxygenation)
Low repopulation
(short overall treatment time)Advantages of Fractionation ?
Hypo-fractionation matches with high LET “conformal” C-ion beam
Conformal
Experiments with carbon ions and fast neutrons demonstrated that increasing their fraction dose tended to lower the RBE for both the tumor and normal tissues, but the RBE for the tumor did not decrease as rapidly as the RBE for the normal tissues.
These results substantiate that the therapeutic ratio increases rather than decreases even though the fraction dose is increased.
Another Biological Background for Hypofractionated Radiotherapy with Carbon Ion beams
Koike S, et al: Radiat Prot Dos. 2002;99: 405-408.
Ando et al. : J.Radiat.Res. 2005;46:51-57.
Denekamp J: Int J Radiat Biol. 1997;71: 681-694,.
To prove efficacy and safety of C-ion RT Carbon Ion Clinical Trials at NIRS
a) Establish safe and precise C- ion RT technique b) Conduct phase I study ⇒ phase II study 1. Achieve local control in radio-resistant tumor 2. Demonstrate hypo-fractionation in common cancer
(and conduct comparative study, if necessary) Based on “high physical selectivity” & “biological effectiveness”
Hypo-fractionated
Treatment Rooms Room for Biological
Experiments
Beam Lines for Physics Research Ion Source
Linear Accelerators
Main Accelerator (Synchrotron)
HIMAC(Heavy Ion Medical Accelerator in Chiba)
• Ion : He ~ Ar
Max energy: ~800Mev/n
• Treatment room(3) Fixed vertical : room A Fixed horizontal : room C Fixed V & H : room B
• The accelerated energy V. beam (140, 290, and 400 MeV/u) H beam (140, 290, and 430 MeV/u)
• The range of C-ion beam in water 290-MeV/u : 15 cm
400-MeV/u : 25 cm 430-MeV/u : 28 cm
• Maximum field size 15 cm by 15 cm
A C B
Specification of HIMAC
Sato et al. Nuclear Physics A.
1995; 588: 229—234
250M EURO
Simulation and Rehearsals
Treatment Planning
CT gantry PSD
LED
Obtain CT data
(Respiratory-gated)
Obtain CT data
(Respiratory-gated)
Immobilization Devices
CT+MRI
CT+PET
Treatment Planning for Head and Neck Tumor Using Fusion Images
ACC
After RT Before RT
Dose distributions
scatterer ridge filter compensator collimator
HIMAC Beam Delivery Techniques
• Broad-beam(passive) irradiation
wobbler magnets
To produce uniform irradiation fields, a passive beam delivery system was employed. We use a pair of wobbler magnets and a scatterer. The range shifter is used for adjusting the residual range of carbon ions in the patient. The ridge filter is used to spread out the Bragg peak in the depth-dose distribution of carbon ions.
Compensator and Collimator are used for shaping target volume.
Kanai et al. IJROBP1999, 44:201-210
The Image Intensifier was replaced by high resolution FPD
Treatment Room
Positioning with orthogonal projections
Horizontal Beam Horizontal Beam
Vertical Beam Vertical Beam
I I FPD
End-expiratory irradiation
Respiration gating for irradiation
Reduction of volume
Minohara et al. IJROBP 47:1097-1103, 2000
Site ‘94 ‘95 ‘96 ‘97 ‘98 ‘99 ‘00 ‘01 ‘02 ‘03 ‘04’05 ‘06‘07 ‘08’09 ‘10 H&N:
All sites Lung :Peripheral Central Locally advanced Med.L/N Liver Prostate:C-ion+HR C-ion alone B&STS Uterus:Sqcc
Adc Brain Skull base Esoph:Pre-op/Radical PK:pre-op
Radical Rectum(P/0 rec)
Eye melanoma Lacrimal gland
②16/4w
①18X/6w
①18x/6w ③16x/4w
①15x/5w
①20x/5w
①X ray + chemo + C-ion
①16x/4w
①
Preop, Radical (end)
①16x/4w
②9x/3w
③9x/3w
④9x/3w
②12x/3w → 8x/2w → 4x/1w ③4x/1w
⑥4x/1w
②Hormone ③High & Middle risk Low risk
②C-ion alone ③+TMZ
②16x/4w
② ③
①pre-op
Mucosal melanoma16x/4w
Phase I/II Phase II
Sarcomas16x/4wks
②pre-op 8x/2w
①(5x/1w)
⑦16x/4w
1x/1day
④2x/2日
⑤16x/4w
①Pre-op 8x/2w②Radical 12X/3wks
①20x/5w
①12x/3w
③radical12x/3w ④+GEM 16x/4w
Protocols and Time Line of Carbon Ion Clinical Trials (1994-2010)
④12x /3w
Total
7,849 Clinical Practice
(CP): 4,505 Prostate 1718(21.9%)
CP:1386
Sarcoma 1025(13.1%)
CP:773
Head & Neck 848(10.8%)
CP:523 Lung 783(10.0%)
CP:195 Liver 483(6.2%)
CP:249 P/O Rectum
403(5.1%) CP:333 GYN
205(2.6%) CP:9 Eye melanoma
127(1.6%) CP:85
Pancreas 345(4.4%) CP:106 CNS
106(1.4%) PA Lymph node
92(1.2%) CP:85 Esophagus
70(0.9%) Skull base
85(1.1%) CP:56
Lacrimal 23(0.3%)
Scanning
11(0.1%) Miscellaneous 1525(19.4%)
CP:705
Patient Distribution Enrolled in Carbon Ion Therapy at NIRS (Treatment: June 1994~February 2013)
1) C-ion RT is successful in the not treatable by other means
• Advanced Head & Neck cancers
• Large skull base cancers
• Inoperable sarcoma
• Post-op recurrent rectal cancer
• Re-irradiation after photon radiotherapy
• Lung cancer ( Single irradiation)
• Liver cancer ( Two fractions)
• Pancreatic cancer (8-12 fractions)
• High risk prostate cancer (16 fractions)
2) Promising results are obtained in C-ion hypo- fractionated RT
All 16 fractions In 4 weeks
Head-and-Neck Cancers
0 12 24 36 48 60 72 84 96 108 120 132 144 156 168 180 0
10 20 30 40 50 60 70 80 90 100
TIME IN MONTHS
April 1997~August 2011
Local Control according to Histological Types
5-year Local Control Rate Adenoid cystic carcinoma (156) 76%
Malignant melanoma (102) 79%
Adenocarcinoma (50) 82%
Squamous cell carcinoma (25) 77%
MELANOMA
36 M
12 M 60 MCombined Chemotherapy and C-ion RT for MMM
Local Control and Overall Survival of Mucosal Malignant Melanomas
TIME IN MONTHS
PROBABILITY
C-ions alone (n=102) 5-year; 76%
C-ions + DAV n=85) 5-year; 81%
PROBABILITY
C-ions alone (n=102) 3-year; 53%, 5-year; 37%
C-ions + DAV ( n=85) 3-year; 67%, 5-year; 62%
TIME IN MONTHS
Local Control Overall Survival
Five-year Survival Rates in
Mucosal Malignant Melanoma of the Head & Neck
1) Gilligan D et al. Br J Radiol 1991; 64: 1147-1150. 2) Shibuya H et al. IJROBP 1992; 25: 35-39.
3) Chang AE et al. Cancer 1998; 78: 1664-1678. 4) Shah JP et al. Am J Surg 1977; 134: 531-535.
5) Patel SG et al. Head Neck 2002; 24: 247-257. 6) Lund VJ et al. Laryngoscope 1999; 109: 208-211.
7) Chaundhry AP et al. Cancer 1958; 11: 923-928.
Authors N 5-ye ar O S (% )
Radiothera p y G illigan 1) 28 18
(+/ - Su rgery) Shibuya2) 28 25
Su rge ry Chang 3) 163 32
(+/ - RT , +/- Chemo ) Shah4 ) 74 22
Patel5) 59 35
Lund6) 58 28
C haudhry7) 41 17
Carb on ion alone N IRS 102 37
Carb on ion + Chemo N IRS 85 62
Local Control and Overall Survival compared with Carbon Ion Dose
Bone and Soft-Tissue Sarcomas (Head & NECK)
Low Dose Carbon vs. High Dose Carbon
TIME IN MONTHS
PROBABILITY
70.4 GyE (n=33) 3-year; 92%, 5-year; 79%
64 or 57.6 GyE( n=14) 5-year; 24%
PROBABILITY 70.4 GyE (n=33) 3-y; 76%, 5-y; 54%
64 or 57.6 GyE (n=14) 3-year; 43%, 5-year; 36%
TIME IN MONTHS
Local Control Overall Survival
IJROBP 2012
Case: 76 y.o. Female
Chordoma originating from the clivus Carbon ion dose: 60.8 GyE/16 frs.
Pre-treatment Dose distribution 67 months later
Clinical characteristics of the reported cases of skull base chordoma
Median dose Median
f/u (y)
Local control rate (%)
Authors N 3-y 5-y 10-y
Photon Catton et al . 1996 24 50 5.2 23 15
Romero et al. 1993 18 50 3.1 17
Forsyth et al. 1993 39 50 8.3 39 31
Magrini et al. 1992 12 58 6 25 25
Proton (+/- photon)
Munzenrider et al.
(MGH) 1999 169 66-83 3.4 73 54
Noel et al. (CPO) 2003 100 67 2.6 86 (2y) 54 (4y) Igaki et al. (Tsukuba)
2004 13 72 5.8 67 46
Ares et al. (PSI) 2009 42 73.5 3.2
(mean) 81
Helium Castro et al. (LB) 1994 53 65 4.3 63
Carbon Shults-Ertner et al.
(GSI) 2007 96 60 2.6
(mean) 81 70
Present study 44 60.8 4.8 91 88 79
These sarcomas were treated at NIRS and all have been controlled. Sarcoma
Bone and Soft Tissue Sarcomas Result of CIRT: Phase II Study n=495 pts
2-year(%) 5-year (%)
Local Control 85 69
Overall Survival 79 59
Local Control
n=514 lesions
Overall Survival n=495
pts
Bone and Soft Tissue Sarcomas Late Morbidities after CIRT: Phase II Study
Impairment ADL (peripheral nerve dysfunction) : 27 Femoral neck fracture : 4 ( all ilioacetabular sarcoma )
Grade
Number 0 1 2 3 4 5
Skin/soft tissue
506 4 475 20 8 1 0
GI tract 439 437 2 0 0 0 0
Spinal cord
46 45 0 1 0 0 0
Edema 14 8 5 1 0 0 0
Unresectable sacral chordoma
5 years after C-ion RT Sacral osteosarcoma
13 years after C-ion RT
Calf soft tissue sarcoma
5 years after C-ion RT Pelvis chondrosarcoma
28 months after C-ion RT Married and had her baby
Local Control and Survival Rate in Sacral Chordoma 1996.6-2012.2 n=185
Follow-up period : 68 mths (7- 165)Median Age : 67 yo ( 26-87) Median volume : 636 cm3 5y-LC: 78%, 5y-OS: 85%
97% pts remained ambulatory
LC OS
mths