question about isocenter

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captainatom

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Is 'placement' of isocenter an outdated, 2D concept?

With 3D/IMRT planning, isn't isocenter the middle of your GTV/PTV? As such there is no placement, only delineation of your target. Or are there sites/scenarios where placement of isocenter is valid?

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Is 'placement' of isocenter an outdated, 2D concept?

The short answer is: no. Where you set isocenter at the time of simulation almost always matters. At times there's a question of how precise you need to be, and there are some special scenarios like tomotherapy. You can also change your isocenter later if you need to (re-marking, shifts), but it's better to get it right the first time.

There is a much, much longer answer with a wide range of possible scenarios where isocenter matters. Rather than spend an hour writing pages of material that may or may not go over your head, would you let me know your level in training and why you're asking the question?
 
The short answer is: no. Where you set isocenter at the time of simulation almost always matters. At times there's a question of how precise you need to be, and there are some special scenarios like tomotherapy. You can also change your isocenter later if you need to (re-marking, shifts), but it's better to get it right the first time.

There is a much, much longer answer with a wide range of possible scenarios where isocenter matters. Rather than spend an hour writing pages of material that may or may not go over your head, would you let me know your level in training and why you're asking the question?

R3, always appreciate your clear answers Neuronix.
 
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Isocenter position is a practical radiation concern in a few ways. This will be off the top of my head, and there may be other scenarios which I'm not considering. There are also different styles of doing this, and this just represents my particular thought process. I'll start basic and build up. I'm going to ignore tomotherapy and cyberknife for now unless someone responds with questions about how this applies to those.

For those reading who have no concept of what the isocenter is: the physical isocenter is the point at which conventional linear accelerators rotate around. A typical radiation source in the machine head rotates in a 360 degree arc around a fixed point in space. It looks something like this:

upload_2015-4-14_10-53-46.png

(coronal view adapted from: http://www.jacmp.org/index.php/jacmp/article/view/4309/3073)

220px-Linac_radiotherapy.png

(MSPaint sagittal oblique view adapted from wikipedia)


When a patient undergoes simulation, a point is chosen within the patient called isocenter that corresponds to the treatment machine's physical isocenter. From a physics and dosimetry standpoint, generally the best place for an isocenter is often in the center of the target (PTV, more on this later). In a modern CT simulation, the patient is lying on the bed/table, supposedly holding perfectly still from the time the CT scan is performed, to the time the isocenter is set and the patient is marked. The marks (temporary or permanent, e.g. tattoos) represent the surface positions on the patient to which the isocenter point corresponds deep within the patient (typically in the target). The marks are usually 2 lateral points and a single anterior or posterior point depending on how the patient is lying (i.e. if lying supine, a mark goes on their anterior body surface at the sup-inf location corresponding to isocenter).

There are a few practical problems here. The first is that an attending may not be available for the simulation. Thus the responsibility for setting isocenter often falls in the therapists. My understanding is that this is a billing gray area.

In any case, let's assume you have a gross target and want to set isocenter in the middle of it for now. If you need to contour the tumor volume, CTV expansions/nodes at risk, PTV, etc, there may not be sufficient time from time of scanning to the set the isocenter perfectly inside the PTV. This may take hours for complicated cases or even if it only takes minutes the patient may be in pain and may not tolerate lying still for long at all. Thus, fast contours of the tumor volume can be chosen on every other or third slice, interpolated, and the isocenter could be set in the middle of that, knowing that you plan to modify the contours later. Or, you can "eyeball" the tumor on the 3D scan and just pick a point that seems to correlate to the center of it. In a palliative or gross tumor (like a pre-op sarcoma) case, I often find the top slice of tumor extent, the bottom slice of tumor extent, and then do a little simple math to find the middle of those two slices and then place the isocenter in the middle of the tumor at that slice. In a situation where there is a large CTV or only a CTV, at simulation I often set the expected field borders and then place isocenter in the middle of that field.

In the days before 3D planning, the isocenter could be determined clincially based on landmarks or based on 2D films +/- bony landmarks and set to a depth. In the 2D or clinial setup days, field arrangements, matching fields, surface/bony anatomy to determine organs at risk, blocking factors like shapes and calculations for custom blocks and wedges, were highly important before 3D planning and MLCs but are easily adjusted today. E.g. You didn't want to have a custom block made and then have to re-do it because you screwed up where the tumor really was. Or, you didn't want to set your depth too shallow and underdose the target. Or you didn't want to have your field going through a critical structure that would seem obvious now on a 3D scan. Thus, I've noticed that some older attendings pay particular attention to how the isocenter is selected compared to some younger attendings.

There are some cases even in the 3D era where isocenter position remains of critical importance for field matching or divergence. For example, in the monoisocentric breast technique, the isocenter is set at level of the inferior clavicular head (for pictures of this see: http://clinicalradiotherapy.weebly.com/breast.html). Since there is no field divergence at isocenter, this allows you to match multiple fields at that point for treatment. Another commonly tested treatment where all of these concepts of gantry angles, collimator angles, couch kicks, skin gaps, feathering of junctions, are tested is in the photon craniospinal setup (without tomotherapy).

Even eliminating these special cases where isocenter needs to have specific positions, we have to keep in mind that the collimator size is limited. Conventional linear accelerators generally have a size on the order of 40 x 40 cm. From the isocenter, that's 20cm in each direction. If you have a large field, you may not be able to encompass the entire target unless the isocenter is in the center of the target. The best way to evaluate this is on a "beam's eye view" which looks like the following when rendered using reconstructed bony anatomy from the simulation CT:

roj-31-252-g002-l.jpg

http://synapse.koreamed.org/DOIx.php?id=10.3857/roj.2013.31.4.252&vmode=PUBREADER

Now on this pelvis field, you can see the isocenter position (where the two lines labeled X and Y intersect) is not in the exact center of the field. That's ok. The small hash marks are 1cm, the large hash marks are 5cm. You can see that on the A-P view (A), the field is about 11.5cm in Y1. You can imagine some point at which if the isocenter was set too high, the field would not be able to open far enough (past 20cm) to cover the target.

So what if you do set the isocenter in the wrong place or decide later it needs to be changed? Generally you have two options. You can place new marks on the patient. That's easy with temporary markings, but patients don't like getting more tattoos than they have to. So instead, you can instruct the therapists to perform daily isocenter shifts. That is, line up to the marks on the patient, and then move the table so many centimeters in some direction to the new treatment isocenter. The problem with either of these approaches is that there is margin for error. If the therapists shift in the wrong direction one day, you will miss completely. You may not even know it happened unless you're doing daily image guidance.

So that is what happens if you're grossly off of the right position. There's a second, more subtle and more recent issue I can't find a good picture to describe. That is that many accelerators now use MLCs that have multiple widths depending on distance from isocenter. In the pelvis field above, each of those little white boxes on the sides represent the position of a single MLC "leaf" which move in and out (left-right on the images). The width (in the sup-inf axis) is determined based on how the MLC is manufactured. For example, the "High Definition" Varian MLC has 8cm of 2.5mm width MLCs, then 5mm width MLCs, but there are many different MLC products of different sizes and widths. The finer the MLCs, the easier it is to shape your field to the target and spare critical structures. Thus, it is often desirable to have finer width MLCs on your target, and not the thicker ones.

Another practical concern is that the beam's eye view can be a digitally reconstructed radiograph (DRR). DRRs are pictures made by the planning system. They use the attenuation values from the simulation CT to reconstruct what a 2D x-ray film would look like for various positions of the imager (i.e. for the image A, above, that is that the x-ray source is above the patient, and for B that is that the x-ray source is lateral to the patient). So for positioning that pelvis in the images above for treatment, I would compare the DRRs to actual A-P and lateral x-rays of the patient in treatment position that are obtained on the first day of treatment and weekly. Now depending on the bony landmarks of the patient, if your target is very much in soft tissue or is in a place that has complicated anatomy (like the head and neck for example), it may make more sense to set the isocenter somewhere where it is easy to align. So some attendings pick an isocenter in a standard position for that site. For example, for many head and neck tumors, that spot may be the anterior-inferior point of the C2 vertebral body. That makes the setup images much easier to evaluate.


Hope that all makes sense. I'm out of time for now.
 
Great reply, Neuronix. Should be required reading for newly-minted radonc residents.

I do, however, think that attending presence is required for simulations. There is a professional component to the billing, which usually does imply the physician needs to be present for the setup at the time of the procedure. Now, not every academic institution does this, but IMO attendings should absolutely be present for simulation, unless you want to bill the technical charge only...which no one does.
 
Great response neuronix.

My two cents shorter version, you can frequently get away with a sub optimally placed ISO. Usually I would say. A really good attending will force you to set the ISO. The but the best way to learn the importance is to try to plan off a poorly placed ISO. At least for me. You can save a dummy plan and move the ISO to see what affect that has on your planning. Junior residents should try it out.
 
Quick follow up question- for a whole breast, is there a problem in keeping the iso in the middle of the breast? I realize it's kept deep to that so you can block the beam (I still don't understand what 'half beam block' means since you may not exactly be blocking half the beam), but what if you keep it in the breast and just angle the gantry so it doesn't diverge into the body?
 
Quick follow up question- for a whole breast, is there a problem in keeping the iso in the middle of the breast? I realize it's kept deep to that so you can block the beam (I still don't understand what 'half beam block' means since you may not exactly be blocking half the beam), but what if you keep it in the breast and just angle the gantry so it doesn't diverge into the body?

For whole breast without nodal irradiation or for a di-isocentric technique, that's fine.

Half beam blocking refers to the MLC positions that extend to midfield--halfway. Hence for monoisocentric breast with treatment of a supraclavicular field, it looks like this:

upload_2015-4-16_8-47-58.png

(Copied from Perez and Brady 7th Ed. Chap 56 p.1119)

The point in the patient where the crosshairs meet (isocenter) is the same in both pictures. The gantry has been rotated between the two views and the MLC positions have changed. The left picture has the lower half of the beam blocked by closing the MLCs, and the right picture has the upper half blocked. Note you can also see that these MLCs are finer in the center than in the periphery as I was describing in my earlier post.

Now there are some caveats to half beam blocking. Given scatter and MLC leakage, it's not perfect. The planning system gives very strange dose profiles at the isocenter slice. But for breast cancer, this is felt to be "blurred" by daily setup variability and respiratory motion.
 
Quick follow up question- for a whole breast, is there a problem in keeping the iso in the middle of the breast? I realize it's kept deep to that so you can block the beam (I still don't understand what 'half beam block' means since you may not exactly be blocking half the beam), but what if you keep it in the breast and just angle the gantry so it doesn't diverge into the body?

Follow-up question, what is the prescription point and why is it different from isocenter? For example postmastectomy RT prescription point is anterior to isocenter.
 
Thanks for the answer to the half-beam block. Now you got me thinking about field matching. When you match 2 fields, it's to prevent divergence and a hot/cold spot. Now, don't beams diverge naturally anyway? So if you have the above monoiso breast, won't the photons diverge after they hit the jaws/MLCs. Why do beams diverge anyway - just interaction with air?
 
Thanks for the answer to the half-beam block. Now you got me thinking about field matching. When you match 2 fields, it's to prevent divergence and a hot/cold spot. Now, don't beams diverge naturally anyway? So if you have the above monoiso breast, won't the photons diverge after they hit the jaws/MLCs. Why do beams diverge anyway - just interaction with air?

Divergence is a geometric process shown in the image below. Field matching refers to taking the edges of two beams geometrically and aligning them such that they don't overlap in ways you don't want (creating hot spots) or aren't too separated (creating cold spots in your target).

Photon beams don't significantly interact with air in this context. You may be confusing this with electron beams. Electrons are appreciably scattered by air, which is why the electron cone or collimator is applied as close to the patient as possible--less distance for the electrons to undergo scattering.

upload_2015-4-19_14-22-38.png

(adapted from: http://www.jmp.org.in/article.asp?i...=39;issue=2;spage=71;epage=84;aulast=Ayyangar)

This diagram, the simplest I could find to explain divergence, illustrates the divergence shown in one plane for a Cobalt source. The field size is defined by the solid lines, but note that they are not straight up and down. The radiation beams themselves don't come perfectly forward (regardless if that's from a Cobalt source or generated by a target in a linear accelerator). There is also divergence in the other axis as well (i.e. into and out of the screen).

I've also crudely drawn in red the space between the dashed line and the solid line called the physical penumbra. The dose is decreasing in the left-right axis between the solid and dashed line. It also continues to decrease past the dashed line given partial attenuation by the blocks where photons only travel through part of the thickness of the collimator. E.g. imagine the dashed line angled slightly more outwards so that it just clips, and is not fully blocked by, the corner of the collimator.

For a half beam block, see the image below

upload_2015-4-19_14-32-15.png

(This is from Khan's textbook, I grabbed it from: http://www.ebah.com.br/content/ABAA...f-radiation-therapy-faiz-m-khan-13khan?part=3)

So A shows a full field coming from a point source. You can see how the half beam block removes half of the beam as part of a setup in the middle and right images. For a point radiation source, there is no geometric divergence at the middle (i.e. individual photons from either side aren't crossing the midline).

Where this becomes even more relevant and is frequently tested (such that you must understand it) are the several different ways to set up conventional craniospinal irradiation. What I think is the simplest method (but still utilizing field matches with skin gap, half beam blocking, and junction feathering), is well described here: http://citeseerx.ist.psu.edu/viewdoc/download?doi=10.1.1.111.1895&rep=rep1&type=pdf
 

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Thanks Neuronix. I have a couple questions of follow-up. In the first figure, the divergence seems to be coming from the collimators that are angled. I can see that there can be divergence with any collimators though, whether they're angled as a V, || or ^. What I don't understand is when you half-beam block, as in the last diagram, why the beam doesn't diverge between the half-beam block and the patient (i.e. why the beam stay completely straight after the beam block but not after the collimator right after the source).

Also, while I'm at it, is the dose at the center of a square field the same as the periphery? I've seen figures that have horns at the sides saying it's higher in the periphery, but I've also seen figures saying that the periphery corresponds to only the 50% isodose line. COnfusing...
 
Thanks Neuronix. I have a couple questions of follow-up. In the first figure, the divergence seems to be coming from the collimators that are angled. I can see that there can be divergence with any collimators though, whether they're angled as a V, || or ^. What I don't understand is when you half-beam block, as in the last diagram, why the beam doesn't diverge between the half-beam block and the patient (i.e. why the beam stay completely straight after the beam block but not after the collimator right after the source).

Note that the x-rays are traveling in straight lines. If you blocked every ray on the right side, now only rays in the center or to the left are going to pass. the rays on the left can continue to diverge because they're angled outwards. The rays in the center continue straight. The rays traveling right are blocked. This is just a matter of straight lines. See the image below.

The text in the image below pertains to your other question.
06-chap-04-clinical-radiation-generators-10-728.jpg

(Taken from this presentation: http://www.slideshare.net/wfrt1360/06-chap-04-clinical-radiation-generators)

The collimator takes on that wedge shape because it is following the straight angles of the beam. The beam has to travel through the whole collimator to be fully attenuated. If you made the collimator square, in the diagrams above, the penumbra of the beam would be much larger. So the collimator isn't creating the divergence, it's just giving the best beam profile it can knowing the divergence is there.

Also, while I'm at it, is the dose at the center of a square field the same as the periphery? I've seen figures that have horns at the sides saying it's higher in the periphery, but I've also seen figures saying that the periphery corresponds to only the 50% isodose line. COnfusing...

This is what the dose looks like across one axis:
field10.gif

http://totlxl.to.infn.it/NewSite/Strip_pixel_chambers/photons.html

The borders of the field are calibrated to be where the dots reach 50%. The machine is calibrated that way and that's part of the QA process. I'm not entirely sure what these horns are that you're mentioning. The shape of the field is generated by the flattening filter inside the head of the machine. The flattening filter is designed to give a flat profile (+/- a tolerance, 3%/3mm is common) for a beam of a certain size at a certain depth.
 
Good Golly, Neuronix - fantastic answers! I really wish I had this explanation early in residency.
 
Regarding the horns question, I don't think you're totally off base. I believe the flattening filter is designed to give a perfectly flat profile at a given depth (say 5cm; I don't recall the exact number). Because of scattering out of the field, the filter ends up yielding a little extra dose at the edge (producing the horns) shallow to the reference depth, and a little less dose at the edge (producing a rounded shape) deep to the reference depth.
 
I believe the flattening filter is designed to give a perfectly flat profile at a given depth (say 5cm; I don't recall the exact number). Because of scattering out of the field, the filter ends up yielding a little extra dose at the edge (producing the horns) shallow to the reference depth, and a little less dose at the edge (producing a rounded shape) deep to the reference depth.

Ah right. If you want pics go to: https://www.aapm.org/meetings/09SS/documents/11Palta-PhotonBeamDosimetry.pdf Slide #31 (in that pic the shallower profile with horns is at the top and the bowed deeper profile is at the bottom)
 
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