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SLIDES
& TRANSCRIPTS
Tuesday,
June 19
RADIOTHERAPY
SECTION - TECHNICAL ISSUES WITH STEREOTAXIC RADIOSURGERY
Randall
Ten Haken, Ph.D.
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| Slide
1: Introduction |
DR.
TEN HAKEN: All right. I know what you are thinking. I have been
here for 12 hours now. I have got the most boring title of the
whole day, and you are going to hear a lecture by a physicist.
The good news is that both Scott and Rick asked me to not talk
about physics very much at all and as Rick just said to talk about
issues that might be of importance in a multi-institutional trial.
So, I am going to do a whirlwind tour of some issues that are
going to be of consequence in that type of a setting.
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| Slide
2: Overview |
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I
am going to go through a brief introduction. I will talk about some
of the patient immobilization and setup issues, different methods
of dealing with breathing, whether it is possible to do online imaging
and tracking and then some of the dosimetry issues that were already
alluded to.
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| Slide
3: Radiotherapy Target Volumes |
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In
radiotherapy if we are uncertain as to the clinical tumor margin
or the location of the tumor at the time of treatment we need to
treat a volume that is larger than the physical tumor to ensure
adequate coverage as the previous speaker just mentioned.
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| Slide
4: Target Volumes |
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These
are loosely called the GTV, the clinical target volume and the planning
target volume which takes into account organ motion. We have to
treat something this big to make sure that something this big gets
the dose we want.
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| Slide
5: ? |
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So,
do millimeters matter?
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| Slide
6: Target Volumes |
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Well,
I am going to do a little bit of physics not too much but a lot
of what I really needed to know about physics I should have learned
in math class and that is true in this situation, also.
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| Slide
7: mm Matter? |
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. These are the only formulas that I am going to show you, but this
is an easy one, volume of the sphere and heaven forbid this is differential
calculus but it is not that hard. If we look at the fractional change
in volume as a function of diameter it is just the differential
of this, and we can divide one by the other. If I take delta V and
divide by V I can find that the fractional change in volume is three
times the fractional change in diameter. So, what does that mean?
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| Slide
8:
mm Matter? |
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That
means that if I add a 1 millimeter margin to a 6 millimeter target
this increases the volume by 100%. It means I have to add a millimeter
to each side. So, I am increasing the diameter by 2 millimeters
and that increases the volume by 100%. If I add a 2 millimeter margin
to a 6 millimeter tumor I increase it by 200%. If I put a 3 millimeter
margin I increase the volume by 300%. Those margins are all in normal
tissue. We are treating more normal tissue by each one of these
millimeters that we add to the outside. So, these millimeters do
make a difference because we are adding them at the outside of the
target volume that we are trying to treat. So, every millimeter
we add has a big consequence.
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| Slide
9: Patient Fixation |
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First
some of the fixation techniques. As the previous speakers were talking
about there are a couple of nice devices to try to re-set up the
patient, their body habitus at least at the same point each time
that we are going to treat them. This is one such study. It uses
one device from Germany.
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| Slide
10: Patient Fixation
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They have
a sophisticated system that has a body cast and a face cast. It
has a device that you can use on the CT scanner and another localization
device that has radio-opaque markers they can use at the time of
treatment.
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| Slide
11: Patient
Fixation |
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This
is another device, and again this one was evaluated by some people
in Germany.
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| Slide
12: Patient
Fixation |
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It is
the device that the previous speaker was just referring to. This
is the stereotactic body frame which was developed by Blomgren and
Lax at the Karolinska. It has again fiducial markers, it has this
thing that you can push down on the abdomen for patient fixation.
The point of all these is to show you that there are devices that
try to place the patient at the same point each time they are going
to be treated and then try to have some assurance that they are
not going to move once they are there. This is called immobilization
or fixation.
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| Slide
13: Patient
Fixation |
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Then
at least in these people's hands what they would do is use these
external markers on the patient and some internal bony structures
and then try to treat the soft tissue lesion with some margin and
hope that it is in the same place each time they treat it, both
at the treatment planning and at the CT simulation. So, we are going
to use these external markers that I can see on imaging studies
and hope that all of the internal stuff is going to be in the same
place by using some sort of immobilization device.
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| Slide
14: Patient
Fixation |
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The point
of this graph is to show that they needed to leave at least a 5-millimeter
margin to cover most of these people's tumors and even if they left
a 10-millimeter margin which this, you might not be able to see
this graph very well - each one of these columns still shows one
patient that exceeded the 10-millimeter reference. So, the bottom
line for this type of immobilization at least in their conclusion,
was that in single cases of soft tissue targets of the planning
target volume would not sufficiently cover target deviation without
isocenter correction. This indicates to them at least that CT simulation
prior to treatment should be performed if you are trying to do more
heroic things than on the order of 10-millimeter margin, particularly
if you want to do it several times and cover every patient. Now,
you just heard a previous speaker say that they can do better in
some cases, but this is just using the marker. So, if you are going
to try to push on the abdomen to keep them from breathing and try
to set them up you still need to leave a bigger margin for multiple
fractions.
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| Slide
15: Dealing with Respiratory Motion |
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How
do we deal with this respiratory motion? As many people have mentioned,
the patients breathe. We want them to be breathing when we are done
treating them, too. So, this is a good thing. As previous speakers
also mentioned, the planning target volume margins that we use are
uniform sometimes but usually they are asymmetric. Things move under
motion more in one direction than they do in the other. So, there
are ways to try to minimize this, using shallow breathing, an abdominal
belt or pressure on the abdomen. We can gate the treatments to the
breathing cycle, just turn on the accelerator when the patient is
at the same point in the breathing cycle or we can try to stop the
motion using voluntary breath hold or actively control the breath
hold. I am going to go through a few quick examples of each one
of these.
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| Slide
16: Minimize Motion |
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This, again, by the Swedish group, the diaphragmatic movement as
measured by fluoroscopy under free breathing has this range, 15
to 25 millimeters. With this abdominal pressure they were able to
reduce it to the 5-to-10-millimeter range, very similar to what
the previous speaker just mentioned. So, this type of thing can
reduce that margin substantially. It is not zero, but it reduces
it.
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Slide 17: Shallow Breathing |
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Another
way to do this is with shallow rapid breathing with oxygen. This
is by one of the Japanese groups with the abdominal belt which was
optional. We see that the breathing motion is less than 10 millimeters
in just about all the patients, less than 5 millimeters in some
of the patients.
So, we are getting close. We are getting things that are pretty
small, but we are not completely eliminating this.
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| Slide
18: Gating |
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Gating
experience, I am just listing these for the purpose of showing it.
The idea is that you try to pick some phase of the breathing cycle
and just turn on the accelerator to treat the patient during that
part of the breathing cycle. It is up to you to try to pick how
much of the breathing cycle you want to use and then you can use
the smaller margin. I just wanted to go through this quickly to
show that there are a variety of methods going back to 1989, again
in Japan for the early experience for this and moving on now to
other manufacturers.
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| Slide
19:
Gating |
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In
the Japanese experience for some of these tumors they resulted in
a 28 to 85% reduction in the amount of lung that was irradiated
in their heavy ion therapy project but they still required a safety
margin of 10 to 15 millimeters despite the use of gating to account
for the continuous organ motion and unexpected excursions.
So, you have to narrow down the window when you want to treat. If
you are only going to treat when the lung tumor is at one spot you
are not going to have the beam on very long and it is going to take
a long time to treat. So you have to pick some window that you are
going to use, and this data describes experience in their hands
with their limit. Again, this is a similar number to what we were
hearing in the last couple of slides.
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| Slide
20: ABC |
There has been something popular in this country over the last
couple of years called active breathing control which was first
pioneered at William Beaumont Hospital by John Wong and collaborators.
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| Slide
21: ABC Device |
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It
looks like this in their hands. It is essentially a pneumotach that
is connected to a box that has a valve where the air goes in and
out, and it has some sort of a device, a computer that monitors
the breathing wave form.
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| Slide
22:
ABC Device |
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There
is another system that we have been using at our institution that
is made by Sensor Metrics. It is another similar thing.
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| Slide
23: ABC
Device |
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This
is something that they use for doing lung function testing for athletes
and it looks like this. It has again a flow sensor, a mouthpiece
that goes into the patient's mouth, which then just opens out to
the air. So, you breathe through it normally. There is a little
thing in here that detects the flow and provides electrical signals.
Then there is a bladder here that can open or close this opening
so that you cannot breathe anymore.
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| Slide
24: Breath Hold at Normal Exhale |
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So what happens is a form of gating actually. As the valve is opened
the patient is breathing. We can look at pressure. We can look at
volume. Then we close the valve and turn on the beam for some part
of the cycle. We choose whatever part of the breathing cycle that
we think is the most reproducible and try to treat the patient at
that point. Then we treat for a reasonable amount of time, 10 or
20 seconds, let them breathe and then recapture again at the same
point in the breathing cycle and turn the beam on.
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| Slide
25: ABC |
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This is a type of reproducibility that you can see using this technique.
Here is with normal breathing. We notice that we see artifacts in
CT scans where the diaphragm shows up on some slices and then disappears
again. Other things are moving around. These are two CT scans that
were separated by 30 minutes in time which look for all practical
purposes to be nearly identical. So, the short-term reproducibility
of this is quite good.
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| Slide
26: ABC |
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In
their hands for two CT scans separated by 30 minutes they were seeing
these types of reproducibility on the order of 2 to 4 millimeters.
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| Slide
27: On-line |
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We
have been doing an online study where we have been looking at using
the ABC device in a treatment room we have equipped with diagnostic
x-ray tubes that are mounted on the walls of the room and a detector
which you can use to see inside the patient fairly well.
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| Slide
28: Image Alignment |
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Then
we can do an online analysis where we compare the DRR to the images
that we get at the time of treatment and in this case we are looking
at the position of the diaphragm.
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| Slide
29: ABC Reproducibility |
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In our hands again we get numbers that are quite small for the standard
deviation of these patients during one treatment, and they again
are averaging on the order of 2 millimeters or so. Even between
one treatment and the next the margin increases slightly. As this
patient is being treated over the course of many weeks, the diaphragmatic
position is not completely reproducible vis-a-vis the part of the
respiratory cycle and we see that we need to increase this margin.
But what is even a little bit more alarming is that these maximal
excursions are almost on the same order of magnitude as the free
breathing which to us it is quite stable during one treatment, but
to use it over a long period of time you need to do some sort of
online imaging to re-establish patient position.
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| Slide
30: Online Radiographic Localization |
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So, this brings us naturally to online radiographic localization.
If we are going to try to use some device that to try to suspend
ventilation or do something heroic like this, are we able then to
see anything on a daily basis? Well, there are obstacles. There
is difficulty in landmark visualization, the ability of quantitative
analysis tools, speed in doing this, the speed of making a correction
once you see that something is wrong. But we have one advantage
over diagnostic procedures that we were talking about today, and
that is that we have prior information. We know there is something
there and we know approximately where it is. We don't have to go
look for it and screen the whole lung to find out where it is. We
know that somebody else told us there is a nodule there or we implanted
a radio-opaque marker someplace or there is something that we know
about, and so we can use this to our advantage to look in the right
spot.
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| Slide
31: Soft Tissue Imaging |
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In
preparation for this meeting we did a couple of measurements this
weekend and I must admit that I was completely floored when people
started talking about how small these things are. I was even more
floored when I started doing some measurements. We wanted to see
if we could see some of these little soft tissues on a megavoltage
x-ray film. Remember we are using 6 or 10 MV photons to treat these
patients and we want to see if we can see a soft tissue mass on
some sort of a port film, and so I have got some balls here. This
is a 9.5 millimeter plastic ball. This little guy here is a 3 millimeter
Teflon ball, and when you say 3 millimeters in diameter, it sounds
big, but when you look at a circle there is not a lot of mass there.
These are small things which again floors me when I hear the discussions
today when taking out big chunks of tissue and there are still having
problems with controlling these things. So, these are small.
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| Slide
32: Soft Tissue Imaging |
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So,
can we see them? I don't know if we can with the lights up like
this, but this is the way that the x-ray film turned out. If we
enhance it a little bit yes we can see them, but I know where they
are. With prior knowledge I know where we placed them on the surface
of the phantom. I know we placed them in this region here, and maybe
you can start to get an inkling of where they are. I will help you
out a little bit. Again, I don't know if you are going to be able
to see this with the lights up, but this is in this region. There
is one. The largest ball is here. The second largest ball is here.
The third largest ball is here, and you can start to imagine the
last one.
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| Slide
33: Soft
Tissue Imaging |
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So,
this is a blown-up area of that image. This is the 9.5-millimeter
ball. This is the 8-millimeter one. This is the 6.5-millimeter one,
and I can imagine something might be there for the little guy.
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| Slide
34: Soft
Tissue Imaging |
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We
can do some enhancement, histogram equalization of things in that
region and we can start to see these things a little bit better
but yes, at least from a physics standpoint these things could be
visible in megavoltage x-rays if we knew where to look and we could
see them on a daily basis.
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| Slide
35:
Soft Tissue Imaging |
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We
can also see them on electronic portal imagers. This is not a complete
state of the art portal imager, but we can see an electronic portal
imager, meaning we can get a digital online image which we can manipulate
to make a decision about how to reposition the patient.
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| Slide
36: Direct Online Imaging |
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Okay,
those are points inside the patient that I am trying to see on flat
films to try to align the patient. If I do an orthogonal set of
films then I can do triangulation and do a 3D correction of the
patient position, but I still cannot see the whole soft tissue mass.
So the next thing is doing something maybe more heroic, placing
a CT scanner in close proximity to the treatment unit or trying
to use the treatment beam itself or some diagnostic beam to do online
imaging. Now, this is something that not very many places are doing
but I am trying to give you a flavor of the variety of things that
could be available at certain institutions to attack this problem.
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| Slide
37: Tumor Tracking |
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These
types of things are clear. The leaders in this field have been several
groups in Japan and I am going to show you a few things from their
work.
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| Slide
38: Tumor
Tracking |
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In
this institution they actually have a treatment room that has a
CT scanner and a simulator. This is a source of diagnostic x-rays
that rotates on a C arm around the patient and megavoltage treatment
unit that are all in the same room. They have a couch that moves
on a rail system and rotates from one machine to the other. So,
this patient can be inserted into the CT scanner to do a CT scan,
rotated, put underneath the simulator to watch under fluoroscopy
to see how much things move up and down with breathing, rotated
around in the other direction and inserted into the treatment unit
and be treated. This is truly a heroic effort to localize things,
to do soft tissue, online soft tissue localization.
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| Slide
39:
Tumor Tracking |
Another group is this group in Tokyo which is doing online megavoltage
CT. They are using the treatment beam itself to do computer tomography
and try to get an idea of where the sections of the patient are
at the time of treatment. This would look something like this.
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| Slide
40: Tumor
Tracking |
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This
is a planning scan where they are going to try to treat this lesion
with some sort of a margin and this is an image that they would
get at the time of the treatment using the megavoltage source of
treatment. So, you can see that they are off a little bit, more
than they wanted to be. So, they move the beam over to where they
want to be and try to continue the treatment.
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| Slide
41:
Tumor Tracking |
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They
also have a nice little system where they can have a monitor for
the therapist to watch so that they can project the beam edge that
is detected by a detector onto the scan that they had previously
and try to make sure that things are in. I will give you a little
visual cue to see that things are in the right place.
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| Slide
42:
Tumor Tracking |
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The
most heroic effort I think is probably being done here in Sapporo
where they are actually doing real-time tumor tracking.
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| Slide
43: Target Motion |
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This
is done by means of some x-ray tubes which are mounted in the floor
and some image intensifiers which are mounted in the ceiling of
a patient so that no matter what position this gantry is at a couple
of these can see through the patient if they have diagnostic x-rays
that are on at the same time.
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| Slide
44: Tumor Tracking |
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They
would implant, for instance, a fiducial marker or something close
to the inside of the patient and then gate the radiation by that
image that is coming out of the beam. Not just by a scan that is
connected to the patient or something with their breathing but actually
looking at the image that is transmitted through the patient, turn
on the beam when everything is in the right spot. So, when things
are in the right position they turn the beam on.
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| Slide
45: Tumor
Tracking |
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When they are not in the right position they turn the beam off,
and they can move. This is a 10-millimeter circular aperture and
this is placed on a radiographic film. This is what it looks like
with breathing motion. This is what it looks like if they don't
take into account the slight time delay between trying to decide
whether things are in the right place and turning on the beam. So,
there is a little delay. If they take that delay into account they
can get a very tight distribution, and you will have to believe
me when I say that this is on the order of 10 millimeters. It is
the same size as the aperture.
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| Slide
46: Lung Dosimetry |
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Okay, almost there. So, what the previous slide should have showed
you is that there are lots of techniques to try to localize patients
and each one of those techniques will determine how big of a margin
you need to leave around the tissue to treat it. The other major
issue is lung dosimetry, and I am going to show you a couple of
titles of papers and discuss the major issue associated with this
without trying to get into too much physics. This has to do with
the dose calculations and the way radiation interacts in tissue.
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| Slide
47: Lung
Dosimetry |
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These
are a tumor volume inside of a lung phantom. This is a mock-up.
So, they put a soft tissue mass, a piece of plastic with an ion
chamber inside of a phantom that has air or a lung-like material
surrounded by other normal tissue and are looking at the dose distribution.
If the patient were made completely of water this would all be fairly
uniform. It is not. The patient is not made out of water. So, a
couple of things happen, and one of the big things that happens
is that the beam spreads out at the edges.
Another thing that happens is that the dose in the center of the
field is not what you would expect, and I am going to talk a little
bit about why that is true.
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| Slide
48:
Lung Dosimetry |
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There
are better ways of doing the dose calculation, and this is one of
the early papers that talked about doing this. There is something
called Monte Carlo calculations of dose which actually track each
one of the photons through the patient, use some physics, look up
tables to decide what type of interaction it had and deposit the
dose.
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| Slide
49: Lung
Dosimetry |
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They
are sort of the most accurate dose calculations that we have today,
and they are here compared to some measurements. I apologize for
the fuzzy graphs. The message to get out of this is that these are
all three different dose calculations of what the dose would be
for this four-by-four centimeter field in this air volume between
normal tissue, air and lung. This is as we go deep into the phantom.
As I go crosswise across the beam you notice this is spread out,
and again, I get three different predictions depending upon what
the dose calculation model is of what the dose would be in profile
at this spot. This is clearly a problem in terms of recording what
the dose would be.
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| Slide
50: Single Beam Dose |
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Finally,
Bob just lent me these slides which I think very nicely illustrate
the dose buildup and build-down effect. If we have a beam that is
coming into the patient phantom, and here we have a nodule, if we
assume that this patient is all made out of water, the dose builds
up the normal way. This is called the depth dose, and it falls off
as a function of depth, and this gives a very nice rounded edge.
If we have now a lung that starts about here and goes to about here
with this nodule in the center of it, the dose falls off and builds
up again inside of this little solid tissue, falls off again and
then builds up again when it gets back into the normal tissue. This
is for two different beam energies. This is for a high-energy beam
where the effects are worse and for a low-energy beam where the
effects are better.
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| Slide
51: Lung Geometry |
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They also did some measurements in a phantom trying to mock-up some
of these small tumors.
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| Slide
52: Tumor |
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So,
they have a small tumor inside of this essentially water phantom
that is going to have some cylinders which will have air-like or
tissue-like materials and they did some Monte Carlo calculations
of that situation, and this is what you would normally get from
a planning system for a homogeneous medium. As Bob mentioned to
you they are prescribing to this outside of the circle and with
little margin at all. In this case they would think that the 75%
isodose line covers this, and things are fairly uniform.
They did this for higher energy x-rays just to magnify the effect.
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| Slide
53: Tumor |
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If
we actually look at this now surrounded by lung a couple of things
happen. First of all we notice that the dose in the center is not
what it was before. It is not 1000. It is a little bit less. The
dose at the periphery is not 1000. It is a little bit less now,
and there is, also, a higher dose in the center, and so this demonstrates
the two effects that are going on. You are going to hear people
talk about heterogeneity corrections and dose calculations. There
are two things going on. One is this beam that is going through
the air. It is not attenuated as much as it would have been in water.
So, in one circumstance we are getting photons that reach this target
volume that normally wouldn't have. The other effect is the way
photons deposit their dose in tissues. The photons interact. They
set in motion electrons. Those electrons deposit the dose and if
this is all surrounded by water and this is a broad beam there are
just as many electrons coming into this point as there are going
out of that point, and we have what is called electronic equilibrium.
If we surround this with lung-like material, these electrons go
whizzing away, deposit their dose some other place, and there is
not a compensatory effect of coming back in, and so this is spread
out. The dose is spread out at the margin. I just have a couple
more.
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| Slide
54: Tumor |
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This
is almost the second to last slide. This is just to demonstrate
that again this is much worse for 15 MV photons than it is for the
6 MV photons. In this case I think you said that only the 50% isodose
line was covering as opposed to what they would have hoped originally.
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| Slide
55: Summary |
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Okay,
so, in summary it was sort of a long whirlwind tour to show you
I think there are two primary concerns from a physics standpoint
from multi-institutional trials and QA of those trials. First of
all, the differing immobilization techniques, online imaging capabilities
and methods of dealing with breathing lead to a range of margins
that individual institutions should use to treat these lesions.
The second thing is that the differing methods to compute the dosimetric
effects of tissue and homogeneities can lead to disparities in the
reported dose and, also, what you are really doing in reality to
what you thought you might be doing.
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