Protons - 1 Flashcards

1
Q

What is the rational for proton therapy?

A

No exit dose part the target
Reduced morbidity - good for paeds
Dose escalation - Can increase curative treatment options - good for adults

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2
Q

What interaction types do protons undergo?

A

Coulomb interactions with electrons
Coulomb interactions with nuclei
Inelastic collisions with nuclei

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3
Q

What is the result of a coulomb interaction with electrons for protons?

A

Secondary electron produced
Proton loses energy - slows down
Probability of further coulomb interactions increased
Produces the Bragg peak

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4
Q

What is the equation for the stopping power, mass stopping power and Bethe-Bloch equation for coulomb interactions with electrons?

A

S = -dE/dx
S/p = -1/p dE/dx
S/p prop 1/v^2 . Z/A . z^2 where v = velocity of proton, Z = atomic number of nucleus, A = relative atomic mass of nucleus, z = atomic number of proton

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5
Q

What is the source of the Bragg peak?

A

As protons slow, the rate of energy deposition increases - the range is therefore dependent upon the initial energy - range prop E^2

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6
Q

What is the equation for the velocity of a proton?

A

v = (c^2 - ((m0^2.c^6)/E^2))^1/2

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7
Q

What is the equation for the Lorentz factor?

A

gamma = 1/(1 - v^2/c^2)^1/2

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8
Q

What are the deliverable energies for pencil beam scanning systems?

A

70-230MeV

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9
Q

What is the source of range straggling?

A

The continuous slowing down approximation is only an approximation
Energy loss occurs at a very large number of discrete interactions with particles in the medium
Energy loss is a statistical process
Not every photon stops at the same point
The distal edge of the Bragg peak therefore has a distal edge

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10
Q

What is the result of coulomb interactions with the nuclei?

A

Proton direction is changed
Produces lateral scatter in beam
The spreading has a gaussian distribution

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11
Q

What is the result of inelastic collisions with the nuclei?

A

Nuclear fragments may be produced
Original proton can’t generally be identified
Produces the halo

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12
Q

What is the standard layout of a proton centre?

A

Accelerator
Proton beam line into multiple rooms - beam can only go to one room at a time
3 rooms if doing complex treatments, up to 5 if only doing simple treatments

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13
Q

What are the important factors for cyclotrons for proton production?

A

Single energy
Stable beam energy
Continuous beam
High intensity

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14
Q

What are the important factors for synchrotrons for proton production?

A

Variable output energy

Beam has dead time

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15
Q

For a varian probeam PTS what are the maximum field sizes and maximum depth tht can be treated at?

A

Max field size = 30x40cm

Treats up to 35cm depth

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16
Q

What are the two types of delivery systems used in proton centres?

A

Scattering systems

Pencil beam scanning systems

17
Q

What is the equipment for a scattering system?

A

Range modulator wheel - energy spreading
Two scattering foils - lateral spreading
Perspex compensator
Brass collimator

18
Q

What is the equipment for pencil beam scanning system?

A

Energy selection

Steering magnets

19
Q

What factors affect choosing a scattering system?

A

Dose delivered to entire target simultaneously - good for moving targets
Longitudinal length of spread-out-Bragg-peak is fixed - extra dose must be delivered proximal to the target
Field-specific hardware is needed - additional source of neutrons, manufacturing, manual handling, storage, recycling, rad protection issues, more difficult to adapt treatments

20
Q

What factors affect choosing a pencil beam scanning system?

A

Improved ability to conform to target
No field-specific hardware
Get interplay effects for moving targets
Lateral edge of field is less sharp for shallow targets

21
Q

What is the purpose of a range shifter?

A

To treat targets at depths of <4cm which the deliverable energies wouldn’t allow

22
Q

What are the characteristics of a range shifter?

A

Acts as a scatterer - spot size at shallow depths increases and spot has greater divergence
Air-gap should be minimised to reduce effect of increased spot divergence
Lateral edge is less sharp than for a scattering system with a collimator defining the field edge

23
Q

What is the virtual source axis distance?

A

The distance from the isocentre to the apparent source of the proton beam - may differ in x and y depending on the design and position of the steering magnets
Divergent steering gives finite VSAD, Parallel steering gives infinite VSAD

24
Q

What are the HU of a CT converted to for proton planning?

A

Relative proton stopping power - uncertainty due to imaging and treatment using different particles

25
Q

What method is used to convert HU to relative proton stopping power?

A

Stoichiometric method

26
Q

What measurements are needed to commission a beam model?

A

Bragg peaks in water - characterises range as a function of energy and dose delivered/MU to be defined
Lateral profiles in air - allows beam optics to be characterised

27
Q

What chambers should be used for measuring Bragg peaks in water?

A

Large chamber with a small field
Small chamber with a large field
Chamber needs to be large enough to capture entire lateral profile of a single Bragg peak including the halo

28
Q

Why is a 1D Bragg peak curve called an integrated depth dose curve?

A

Integrates the charge collected over the 2D plane of the detector

29
Q

How can the halo be modelled?

A

MC dose calcs

Analysis of difference between large and small detector methods

30
Q

What is the current code of practice for protons?

A

IAEA TRS-398 CoP - designed for scattering systems - primary standard: graphite callorimeter, reference beam: Co-60

31
Q

How are the MUs defined for protons?

A

MU chambers located in nozzle, up-stream of range shifters
IDDs measured using traceable parallel plate chamber
Reference point is taken at a point in the entrance region of Bragg peak - 2cm
Charge collected by MU chamber related to dose at this point
Match gantries by adjusting gain on MU chambers - best fit for all energies

32
Q

How are the beam optics commissioned?

A

Use film or scintillation screen for high spatial resolution
Measurement of lateral beam done in air at a range of distances from nozzle - at least 3 to fit hyperbola on
Dose outside chamber estimated by using MC dose calcs
Laterally beam has gaussian profile, longitudinally beam has hyperbola
Beam waist is at isocentre then focussing is weak