Radiobiological characterization of clinical proton and carbon ...Radiobiological characterization...
Transcript of Radiobiological characterization of clinical proton and carbon ...Radiobiological characterization...
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Radiobiological characterization of
clinical proton and carbon-ion beams :
Université catholique de Louvain, Brussels, Belgium
John Gueulette
Vincent Grégoire
Pierre Scalliet
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Improvement of radiotherapy
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There are several
arguments pointing at
the DNA as the main
target of ionising
radiation
What is the biological effect of ionising
radiation?
Immediate death
delayeddeath
Mitotic delay
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Ionisations along an electron track (secundary electron after low LET irradiation)
CLUSTER
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Sequence of events
• Energy deposits (primary and secondary electrons)
• DNA damage.
• DNA re-arrangement.
• Repair induction (enzyme synthesis).
• Cell cycle arrest.
• Repair vs. apoptosis.
• Cell death
• Tissue failure
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DNA is the primary target
Double
strand break
Ionisation and section
of a DNA strand
(single strand break)
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Various types of DNA damage
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Possible
consequence of
DNA damageapoptosis
ionisation
cell
DNA damage
Repair Misrepair
mutationCell death
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Cell death after misrepair
(lethal mutation)
Apoptosis
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Base pairs can be
substituted,
or deleted, or added,
all resulting in an alteration
of information.
A gene can be inactivated or
mutated.
A mutation can amplify
or decrease the gene
expression.
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A dose increment kills a fixed proportion of cells
Lo
g S
Dose (Gy)
Exponential survival
curve of prokaryotes and
bacteria
Poisson’s law
S = e-aD
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Cell survival curve
survival
dose
Saturated repair
Unsaturated
repair
Survival
curve
Experimentalpoints
Clones can be seen
2 Gy 4 Gy6 Gy
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survival
dose
Survival
without repairsaturation
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Initial part of the survival curve
A steep initial part exists on
survival curves, particularely in
resistant cells.
It is interpreted as a sign of
repair induction when and if the
damage concentration is
sufficient to « trigger » repair
enzyme synthesis.
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The linear quadratic model
survival
dose
Survivalcurve
a/b
a component
b component
-logS = ad + bd2
DNA
Double-strand break
Single-strand break
the model of radiation action
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Ionisation along a particle track
Low density of
ionisation
High density
of ionisation
ADN
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Direct and indirect effects
G Montarou, radiobiology in medicine, 17-12-2013
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ProtonsProtons are sparsely ionising, majority of indirect effects
G Montarou, radiobiology in medicine, 17-12-2013
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Carbon ionsCarbon ions are densely ionising, majority of direct effects
G Montarou, radiobiology in medicine, 17-12-2013
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Scattered
energy deposits,
repair efficient
Dense energy
deposits, repair
inefficient
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Induction of
repair
enzymes with
X-rays and
carbon ions,
same
absorbed dose
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Track structure
depends on
energy and Z
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“Size » of
radiosensitive
structures
RBE
“waste” of energy
Maximum 50 - 150 keV/mm
Ionization density (LET)
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Microdosimetry
Tissue-equivalent proportional counter :
• The sphere is the cathode, in tissue
equivalent material.
• The anode is central.
• The gas filling the sphere is tissue
equivalent (C, N, O, H).
• Its pressure can be adjusted to
simulate small volumes of tissue.
• Irradiation is delivered at extreme low
dose rate.
• Electric charges are collected,
proportional to the individual energy
deposits.
TEPC of Rossi, Columbia University
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Lineal energy, y (keV / µ m)
0.01 0.1 1 10 100
5
4
3
2
1
0
Photons
1000
y.d
y
Energy deposition along
the diameter of a sphere of
the same size as the vital
radiosensitive
structures
E
Microdosimetric spectra : a tool for
tracking the RBE variations
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Energy of the incident particles...
October 2-5, 2003 - Lyon (France)
9th Workshop on heavy Charged Particles in Biology and Medicine 2003 (HCPBM 2003)
General Meeting on the European Network for Light Ion Hadrontherapy (ENLIGHT 2003)
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Indentical nominal energy
and identical nuclear reaction ...
October 2-5, 2003 - Lyon (France)
9th Workshop on heavy Charged Particles in Biology and Medicine 2003 (HCPBM 2003)
General Meeting on the European Network for Light Ion Hadrontherapy (ENLIGHT 2003)
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Depth ...
Surface7 cm
October 2-5, 2003 - Lyon (France)
9th Workshop on heavy Charged Particles in Biology and Medicine 2003 (HCPBM 2003)
General Meeting on the European Network for Light Ion Hadrontherapy (ENLIGHT 2003)
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Summary of pertinent conclusions (1)
Conceptually, RBE is a measure of the biological effectiveness differences related to radiation quality only
RBE is essentially variable and depends on numerous factors related 1) to biology or, 2) to the beam delivery technique
RBE is correlated with ionization density. Roughly speaking, it increases with LET.
Biology : the main sources of RBE variation are : • the biological system (tissue, endpoint, etc.) and • dose, dose rate and fractionation
Beam : the main sources of RBE variation are : • Depth (for heavy ions), • filtration (for fast neutrons), • collimation, etc.
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Summary of pertinent conclusions (2)
When determining RBEs, all conditions - but the radiation quality - have to be the same for the intercompared beams
Inherent performance of the beam generators as well as practical reasons (e.g, distance) prevent from adopting ideal experimental procedure
Microdosimetry is a powerful tool for tracking the potential RBE variations
Recourse to indirect method for RBE determination is often required (RBE ratios)
Recourse to fractionated irradiations is most of the time required to determine RBEs for small doses
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Bragg peak
Plateau region
Fall-off region
Fragmentationregion
PROTONS
HEAVY IONS
Depth in tissue
Rela
tive d
ose
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Most events are in the 1
keV/mm range, with a
significant component
around 10
End of Bragg peak
Most events are in the
range 10-30 keV/mm
range, with a significant
component around 100.
Plateau (entry beam)
Proton beam (Nice)
Spectrum : sum of individual energy deposits
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Proton beam (Nice)
Let increases
as the beam
progresses
in depth
(SOBP)
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Density of energy deposits in
the Bragg peak of carbon ions
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Linear energy transfer (LET)
• LET is the physical
quantity of ionisation
density; its unit is the
keV/mm.
• The higher the LET, the
broader the DNA
damage and, hence, the
larger the biological
effect
dose
survival High LET
Low LET
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RBE ?
The relative biological
effectiveness is a ratio of
dose:
DlowLET/DhighLET
for any given level of effect
survival High LET
Low LET
Dlow Dhigh
S
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0
1
10
100
1000
0 5 10 15 20
Nu
mb
er o
f r
egen
era
ted
cryp
ts
Dose / Gy
Neutrons [p(45)+Be] (Seattle)
Cobalt-60 gamma-rays
R
B
E
All the irradiations
performed under the
same conditions, e.g. :
Animals from the same population
Same day (and moment in the day)
Randomized (dose / radiation quality)
Acute dose rate
Irradiation in a single fraction
Same experimenters
Reliable dosimetry
Etc.
RBE accounts for the biological effectiveness difference
related only to the radiation quality difference
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Different radiation quality have
different RBE’s
& X-rays
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Oxygen effect
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4MeV d-Be
OER = 3.0OER = 1.7
Reduced effect of oxygen
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As LET increases OER decreases
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Healthy tissues
Tumor
Reduction of radiosensitivity differences :
Potential therapeutic advantage
when the tumor is radioresistant
in comparison with healthy tissues
Potential therapeutic benefit due to the reduction
of an unfavourable differential effect
Dose (gamma) Dose (neutrons)
Surv
ivin
g F
ractions (
%)
Surv
ivin
g F
ractions (
%)
Radioresistant
or hypoxic
tumour
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Healthy tissues
Tumor
Reduction of radiosensitivity differences :
contra-indication
when the healthy tissues are radioresistant
In comparison with the tumor
Contra-indication due to the reduction of
a favorable differentiel effect
Surv
ivin
g F
ractions (
%)
Surv
ivin
g F
ractions (
%)
Dose (gamma) Dose (neutrons)
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Buid-up of radiobiological
experience and disclosure
of potential benefits
Safe and optimum
clinical application
Transfer of radiobiological /
clinical information and
coherency of treatments
« Pretherapeutic »
experiments
Radiobiological
Calibration /
Intercomparison
« Preclinical »
experiments
Hadron RBE is
different than that
of photons
RBE varies with
« radiation quality »
All the beams are
different
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Protons
Heavy ions
Neutrons
Summary of in vivo data on jejunal crypt cells
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RBE variations related
to biological system
RBE variation related
to radiation quality
(energy)
Rationale for clinical
application of high-LET
radiations
Emergence
of problems
related to :
Transferring clinical and radiobiological information
Pooling clinical data
Optimizing clinical applications
Comparing with conventional radiations
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Differential
Effect(neutrons, ions)
NO
differential
effect
(protons)
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Potential advantage of protons
is essentially ballistic
Proton RBEs are too small to result
in a workable differential effect
Proton RBEs are big in comparison
with dose accuracy requirements ...
and raise essentially
Bio-dosimetry questions
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Gamma Equivalent Dose =
physical dose x RBE
Uncertainties in RBE values lead to
equal uncertainties in the derived
Gamma Equivalent Doses
The dose accuracy required in
radiotherapy is 3.5 %
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Substantial spread between cell lines and
conflicting conclusions about :
In vitro systems
(Proton RBE = 0.94 - 1.63)
• RBE value in reference conditions (energy, depth)
• possible RBE increase with depth
• possible RBE increase with SF (or fractionation)
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Possible causes of the spread of the data :
In vitro systems
(Proton RBE = 0.94 - 1.63)
• Dosimetry ?
• Underlying theory (model to fit the data)
• Randomization ?
• Platting efficiency ?
Uncertainties above 20 %
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Limited amount of data. Present-day questions are :
In vivo systemsProton RBE 1.08 - 1.17
• RBE increase with fractionation ?
• RBE difference for early and late tissue tolerance ?
• RBE increase with depth ?
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Which system to use for
calibrating
intercomparing
clinical proton beams ?
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Systems and endpoints which
result in widely different values for
the RBE of neutron relative to X-
rays ...
n g1
EBR =
2
Neutronscompared
with gamma
... give similar values for the
RBE differences between two
closely related neutron energies
1n2 n
EBR =
1.1
Neutrons compared
with neutrons
1 gn
3
n n12
1.1
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Consequently, the choice
of a biological system for
intercomparisons should be governed
largely by its
• portability,
• repeatability
• and convenience.J. Hall, 1979
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Intestinal crypts
regeneration in mice
In - vivo system, based on
Cell lethality
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84 hTested beam
Clinical dose rate
Position dependingon the type of beam
Reference beam
Cobalt-60 or 7 MV
1 Gy / min
Depth of the peak
dose
Single fraction
Irradiation to the
whole body
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Protons
Neutrons
Reproducibility...
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Radiobiological
characterization
(protons)
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Influence of depth
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< 5 %
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PSI
Spot scanning
RBE =
1.11 1.16 1.21
~ 4 %
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Dose / Gy
Num
ber
of re
genera
ted c
rypts
per
circum
fere
nce
RBE difference of 7 %
End SOBP
Middle
SOBP
0 1 2 3 4 5 6 7
SOBP (cm)
7 %
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1 fract. 10 fract.3 fract.
RBE = 1.14
± 07
RBE = 1.15
± 0.6
Num
ber
of
regenera
ted c
rypts
per
cir
cum
fere
nce
RBE = 1.15
± 0.5
RBE (end) / RBE (middle) ~ 1.08
i = 4 h
Intestine (10 fractions)
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Selective thoracic irradiation in mice
Irradiation in 10 fractions (i = 12 h)
(middle vs end of the SOBP)
< 6 %
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RB
E r
ela
tive t
o p
hoto
ns
RBE increases
suddenly
by 6 - 10° %
from the middle
to the end of the
SOBP
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200 MeV
protons
More precise irradiation is possible
1.5 cm
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iThemba LABS (2006)
200 MeV protons, 7-cm SOBP
0,1
1
10
100
1000
8 10 12 14 16 18
End
SOBP
Middle
SOBP
Dose / Gy
Nu
mb
er
of re
ge
ne
rate
d c
ryp
ts
pe
r cir
cu
mfe
rence
RBE (end)
RBE (middle)= 1.10
7 cm
3 mm
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As an increase in RBE is
observed at the end of the SOBP
in all biological systems, it is
advisable to allow for it.
TPS should include biological
weighting functions
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Influence of
fractionation
(or dose)
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Crypt regeneration in mice
Bloomington, IN (USA) Midwest Proton Radiation-therapy Institute, Friday, July 9, 2004
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Protons
Cobalt
Bloomington, IN (USA) Midwest Proton Radiation-therapy Institute, Friday, July 9, 2004
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Bloomington, IN (USA) Midwest Proton Radiation-therapy Institute, Friday, July 9, 2004
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1 fract. 10 fract.3 fract.
RBE = 1.14
± 07
RBE = 1.15
± 0.6
Nu
mbe
r of
rege
ne
rate
d c
rypts
per
cir
cum
fere
nce
RBE = 1.15
± 0.5
Irradiation at the middle of a 7 cm SOBP
in the 200-MeV proton beam produced at the
National Accelerator Centre (NAC) of Faure (South Africa).
i = 4 h
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Late tolerance
(Survival after selective irradiation
of the thorax in mice)
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8 months 9 months
6 months 7 months
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RBE = 1.14
± 07
Lung (10 fractions) Intestine (10 fractions)
For both systems (10 fraction irradiations)
RBE at the end of the SOBP ~ 6 % greater that at the middle
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Proton RBE (at the middle of the
SOBP) does not vary with dose
(or fractionation) for in vivo systems
A generic RBE value of 1.10 at the
middle of the SOBP (i.e. point of dose
specification) seems to be appropriate
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Proton RBE In-vitro, as a function of
dose, for all “clinical” energies
All in vivo
Late
reactions
Acute
reactions
All in vitro
V79 lines
non V79
lines
Proton RBE In-vivo, as a function of
dose, for all “clinical” energies
1.10
1.10
1.10
1.19
1.24
1.12
From Paganetti et al. (2002)
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HEAVY IONS
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He
C
PMegavoltage
X rays
Neutrons
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Salivary gland tumour treated with fast neutrons
Study results (± 1985)
17% ± 11 vs. 67% ± 14 25% ± 14 vs. 62% ± 14
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Randomized clinical trial of photons vs mixed
beam neutrons plus photons for prostate Ca
RTOG 77-04
Laramore et al, 1993.
Prostate carcinomas are slow
growing and hence should be well
suited for neutron therapy. The
neutrons are usually used for the
small “boost” volume in order to
minimize late normal tissue
damage.
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Laramore, 1993
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Nature April, 2014
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Which RBE to apply ?
Late tolerance of healthy surrounding tissues
Dose per fraction of 2 Gy photon equivalent
Not a single value
• due to the diversity of the clinical situations
• due to variation of RBE with depth/dose
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Density of energy deposits in
the Bragg peak of carbon ions
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From Peter Peschke, Heidelberg
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Depth in water / mm
RB
E
1,0
1,2
1,4
1,6
1,8
2,0
2,2
0 50 100 150 200
HIMAC (Japan) : Carbon-12
(290 MeV/uma)
6-cm SOBP
EBR = 1.3
EBR = 1.6
EBR = 1.7
EBR = 1.9
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1
3
2
0
50 100 150
Depth / mm
Ab
sorb
ed
do
se /
Gy
1
3
2
Isoe
ffective
do
se / G
y
0 200
x1.6
: 1.3
:1.6 :1.7 :1.9
Biologically
effective dose
Physical
dose
Depth in water / mm
Ab
so
rbe
d d
os
e /
Gy
Compensate the RBE
increase by
decreasing the
physical dose
by factors
corresponding to the
(local) RBE
Method used in static beam delivery
systems (Chiba, Japan)
Effe
ctiv
e d
ose/ G
y
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1
3
2
0
50 100 150
Depth / mm
1
3
2
0 200
Carbon dose x RBE
Iso
effe
ctiv
e d
ose/ G
y
Ab
so
rbe
d d
os
e /
Gy
Depth in water / mm
x1.6x1.7
x1.9
x1.3
Photon
equivalent
biologically
effective dose
A given dose of carbon is biologically
equivalent to the same dose of
gamma multiplied by the carbon RBE
Physical d
ose
Ab
sorb
ed
do
se /
Gy
Iso-doses (in Gy) in a given
tissue do no longer
correspond to
iso-biologically effective
doses !!!
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1
3
2
0
50 100 150
Depth in water / mm
No
rma
lize
d a
bs
orb
ed
do
se
1
3
2
No
rma
lize
d is
oe
ffec
tive
do
se
0 200
CARBON ION BEAM
290 MeV / amu
X 2.7
X 3.4
X 3.0
X 2.1
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LEM“Local effect Model” (Scholz et Kraft, 1994)
Derivation of parametres determining the biological
response to a Carbon ion exposure from the
response parameters to a photon irradiation
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The biological effect in a cell nucleus sub-volume is exclusively determined by theenergy deposit in this sub-volume
The biological effect is independent from theradiation quality of the beam
A local dose deposit with Carbon ionsproduces the same biological effect than thesame dose deposit with photons
Therefore, the different biological effects ofCarbon ion and photons result fromdifferences in spatial dose deposition
Assumptions
Consequences
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Local Effect Model (LEM)(Scholz and Kraft)
Dose-effect relationship for photons (low LET)
Probability of a letal event
Physical data on track structures
Determination of local dose deposits
Experimental measurement of cell nucleus size
Determination of radiosensitive area size
Parameters exclusively determined on the basis of :
(nucleus diameter)
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Advantages :
• Uncertainties on RBE calculation algorithm (LEM, other…)
• Lack of transparency and total confidence in
calculation model
• Impossibility (for the physician nor for the physicist)
to judge directly the appropriateness of treatments plans.
Dose distributions have to be re-calculated with the model.
Inconvenients
• Conformational possibilities
• Possibility to treat sub-volumes
• Possibility of dose « modulation » within each volume of interest
• all RBE variation taken into account
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RBE
NIRS neutrons
80 keV/mm
8 mm apart from
the distal edge
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RBE
NIRS neutrons
Neutron clinical
RBE = 3
Carbon clinical RBE at the
center of the SOBP = 2.38
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Scanner magnets
Raster scan system at GSI, Germany
from : D. Schulz-Ertner, O. Jäkel, W. Schlegel
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i.e. a system where :
“several thousands of narrow ion pencil beams
with individual lateral positions, ion energies
and particle fluences are combined to form an
intensity-modulated field of high granularity”
(M. Krämer, 2001)
Consideration of RBE variations is only
possible in an integrated calulation code
allowing iterative interaction between both
physical and biological input parameters
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Integrated algorithm allowing for the iterative
interaction between physical (e.g. energy/LET) and
biological parameters (e.g. intrinsic radiosensitivity,
oxygenation, dose rates, micro-fractionation, etc.
An RBE weighting factor should be applied at each point
of the irradiated volume, taking RBE variation with energy,
dose, biological system, etc, into account
Particules of variable energy are also delivered at variable dose rates or in multi - micro
fractions.
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Over dosage
M oving target
Under dosage
M oving target
The “Inter–play” effect (Protons, PSI)
Number of regenerated
crypts per circumference
Sta
ndard
devia
tion
Dose heterogeneity
~ 15% / mm
U
T
U
T
T
T
Rel
ativ
e d
ose
y - axis y - axis
x -
axis
a b
a
b
a
b
diffusion
PBS
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Pitfalls...
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~ 1 % of the surface
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~ 1 % of the surface
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Finally, which recommendation for irradiation
schedule?
Short hypofractionated schedules
• Less tumour repopulation.
• More damage to quiescent cells.
• More microvascular damage.
• Differential release of cytokines and special
immunologic effects?
• Too much assumptions in radiobiological
models??