AAPM TG 158 Flashcards

1
Q

measurement and calculation of doses outside the treated volume from EBRT

A

guidance for assessing and managing non-target doses

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2
Q

aims of report

A
  1. highlights major concersnw ith non-target radiation
  2. gives estimate of dose associated from different treatment approaches
  3. discusses dosimeters for measuring photon, electron, or neutron doses
  4. discusses calc techniques for dosimetry
  5. highlights techniques that may reduce non-target doses
  6. discusses dose reporting
  7. makes recommendations for clinical and research practise
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3
Q

concerns regarding non-target radiation

A

-secondary cancers
-cardiac toxicity
-cataracts
-pacemakers
-fetus
-skin dose

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4
Q

neutrons with pacemakers

A

-neutrons cause single-event upsets
-risk is stochastic; there is no “safe” dose

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5
Q

average energy outside of treatment field

A

for 6 MV, ~ 0.2-0.6 MeV vs 1.6 MeV in the treatment beam

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6
Q

how does out-of-field photon dose change with distance from field edge?>

A

decreases exponentially with distance from field edge

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7
Q

hoe does dose outside treatment field change with field size?

A

increases with field size because there is more patient scatter
Farther from the field edge, there is lessfield size dependence53because this dose is dominated byhead leakage. For modulated treatments, the dose outside thetreatment field also depends on beam modulation. The doseincreases with increasing modulation because more head leak-age and more collimator scatter is generated as the number ofmonitor units (MU) increases to deliver the modulatedfields. The dependence on modulation is most noticeablefarther from the treatment field; near the field edge the dose isdominated by patient scatter and patient scatter depends onlyon the volume of tissue irradiated.

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8
Q

how does dose outside tratment field change with depth and beam energy?

A

-varies little with beam energy
-pretty constant with depth, except for surface, which has electron contamination

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9
Q

what does neutron dose increase with

A

MU
beam energy
neutrons in patient decrease with depth

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10
Q

IMRT out of field dose vs 3DCRT

A

IMRT treat-ments typically have lower doses near the edge of the treat-ment field but higher doses far from the treatment field

Near the treatment field, IMRT provides better conformality,which constricts the field edge and thereby reduces the vol-ume of tissue receiving high doses.76However, far from thetreatment field, beam modulation leads to increased headleakage than can result in higher doses.

that the majority of second cancers were in organsnear the treatment field as opposed to organs far out-of-field,indicating the importance of the high-dose region. However that the majority of second cancers were in organsnear the treatment field as opposed to organs far out-of-field,indicating the importance of the high-dose region. However

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11
Q

VMAT vs IMRT

A

VMAT spreads out the dose deliveryover more angles. Consequently, while the average dose willbe similar between VMAT and IMRT, more tissue will beirradiated to a lower dose with VMAT.

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12
Q

out-of-field doses for cyberknife

A

higher, high modulation

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13
Q

out-of-field doses for tomo

A

comparable to IMRT

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14
Q

out-of-field doses for gamma knife

A

between linac and cyber knife

Because Gamma Knife units have a relatively low-energyspectrum, doses very close to the treatment field are oftenhigher than those of CyberKnife or linac systems.126,139Formost distances from the field edge, Gammaknife treatmentshave been shown to produce intermediate doses—higherthan linac-based therapy but lower than those achieved byCyberKnife

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15
Q

FFF

A

reduces out-of-field dose

It reduceshead leakage because less target current is required. Simi-larly, collimator scatter is reduced because the flatteningfilter is no longer a source of scatter. However, patientscatter may be increased in FFF modes.

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16
Q

electron out-of-field dose

A

majority is from scattered electrons
The increase in dose at~20 cm from the field edgearises from scattered electrons originating from the roundedsurface of the MLC
While out-of-field doses gener-ally decrease with distance from the edge for electron therapy,this is less pronounced than for photon therapy
-high compared to photons
-increase with energy and obliquity
-little variation with applicator size

17
Q

non-target dose from brachy

A

-similar to EBRT at close distance
-At distance > 35 cm from target, BT nontarget dose is much less than EBRT

18
Q

photon distance from target

A

remember about 1% at 10 cm from field edge but varies with FS, modulation- for 3DCRT
for imrt, closer to 5%

19
Q

why cover dose detectors with a bolus?

A

surface dose will be greater due to electron contamination and will overestimate photon dose at depth. For better estimate of dose at deoth, put bolus over detector

20
Q

issue with choosing detectors for measuring out=of-field dose

A

-beam energy is lower outside of field. Forexample if using diode, dose will be overestimated outside of field
-dosimeter dynamic range (dose outsode pf field may be too low)
-presence of other particles like neutrons can cause different detector repsonse

21
Q

limitation of using film for out=of-field dosimetry

A

-usually film is good for D> 1cGy- dose may be much less than that
-dose can span orders of magnitude- difficult to get calibration curve that accounts for this range

22
Q

most common passive thermal neutron detectors

A

TLDs (for neutrons) and activation foils

The TLDs are used in pairs, onesensitive to both photons and thermal neutrons (TLD-600)and the other sensitive only to photons (TLD-700). The neu-tron component is determined by the difference in theresponse in the two types of materials.

-require moderators

23
Q

thermal neutron vs fast neutron dose deposition

A

he fast neutron peak (which depos-its the dose) decreases sharply with depth, while the thermal neutron peak (which is often responsible for depositing signal in the detector) shows a very differentdependence on depth, increasing up to 4.5 cm depth and still being notably present at 19.5 cm depth.

therefore have to use thermal neutron detectors with moderators in order to get info about the fast neutrons that actually deposit the dose

24
Q

why not use a rem meter?

A

Because Rem meters have activedetectors, pulse pile-up is a concern and these detectors aregenerally not well suited to measurements in or near the pri-mary beam.

25
Q

why shouldn’t bubble detectors be used in beam?

A

These detectorsshould not be used in the primary photon beam because spu-rious signal has been observed within the polymer, overesti-mating the true result

The advantages of bubble detectors over otherneutron detectors are that they are very easy to use, are reusa-ble, and can be read instantaneously. Disadvantages of bubbledetectors include energy dependence, loss of linearity at highdoses, and the potential for spurious bubbles.

26
Q

why not use track etch detectors fordosimetry for neutrons in proton therapy?

A

Most track etch detectors are not suitable for measurementaround proton (or carbon) beams because of the lack ofresponse to high-energy neutrons.

Track etch detectors are very sensitive and are, therefore,suitable for use outside the primary beam in high-energy pho-ton therapy.
-can measure fast and thermal neutrons

27
Q

tissue-equivalent proportional counter

A

The absorbed dose contributions from vari-ous types of secondary particles can be differentiated via themicrodosimetric spectrum because different secondary parti-cles have different lineal energies in the active volume.

Given that the signal from this type of detector depends onthe measurement of each energy deposition event, the flux isa major concern when using this detector in radiotherapyenvironments because of pulse pile-up and dead time effects

28
Q

does TPS calc under or over estimate out of field dose

A

usually overestimates it

29
Q

Peridose

A

software developed to calculate out of field dose

30
Q

proton therapy integral dose vs IMRT

A

proton therapy is 2-3 X less integral dose

31
Q

where do TPS systems dhow large errors

A

even as close as 3 cm to field edge