L 18: Particle therapy Flashcards

(34 cards)

1
Q

Daily QA for Protons

A
  • Dosimetry and beam delivery
  • Proton beam output check for a defined operating condition to verify correct operation of beam monitoring system
    and monitor unit calibration
  • For a scattered beam verification of the integrity of scatterers, alignment of scatterers and beam penetration
  • Checks of Bragg peak width and lateral beam profile including flatness and symmetry, for scattered beam,
  • uniform scanned (beam) and pencil beam scanning
  • Back-up monitor constancy
  • Mechanical
  • Localization lasers
  • Snout alignment
  • Beamline inspection
  • Distance indicator (ODI)
  • Modulator wheel interlocks (barcodes etc.)
  • Beam delivery system interlocks
  • Safety
  • Door interlocks
  • Audiovisual patient monitors
  • Treatment room area radiation monitors
  • Function of motion stops on all moving systems (gantry, patient position, etc.)
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2
Q

Weekly QA for Protons

A
  • Dosimetry and beam delivery
  • For a randomly selected patient, compare calculated planned dose at selected points to measured dose points in a phantom
  • Respiratory gating equipment
  • Mechanical
  • Gantry/collimator angle indicators
  • Imaging equipment
  • Alignment of x-ray imaging devices relative to beam axis and/or isocenter (orthogonal imaging, cone beam CT, etc.)
  • Quality of images
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3
Q

Monthly QA for Protons

A
  • Dosimetry
  • Verify integrity of modulator system
  • Mechanical
  • Light/radiation field congruence
  • Field size indicators (MLC)
  • Jaw symmetry
  • Cross-hair centering
  • Patient positioner readouts and tolerances
  • For gantry determine isocenter location and check tolerances
  • Coincidence of collimator, gantry, and couch axes at isocenter
  • Safety
  • Emergency off switches
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4
Q

Annual QA for Protons

A
  • Dosimetry and beam delivery
  • Extensive recalibration of output under a wide variety of operating conditions
  • Checks of modulators, range shifters, or energy selection systems as appropriate
  • Lateral profile flatness and symmetry as a function of gantry angle
  • Check location of virtual source
  • Primary MU linearity check
  • Check beam monitors for saturation conditions
  • Measure dose per MU for primary and backup channels as a function of gantry angle
  • Check dose per MU against standard laboratory or other institution using independent standard (e.g., ion chamber or TLD)
  • Mechanical
  • Patient position tolerances including table sag
  • Safety
  • Calibrate area radiation monitors throughout facility
  • Comprehensive test of all accelerator, beam line, gantry, and nozzle safety systems
  • Imaging equipment
  • X-ray kVp, mA, timer, and magnification
  • CT unit HU calibration
  • Full check of all simulation devices CT, PET /CT. MRI
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5
Q

Protons

A
  • Charged particles
  • Better dose distribution
  • Low LET
  • RBE similar to photons
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6
Q

Neutrons

A
  • Better cell killing
  • High LET: direct killing/DNA damage
  • High RBE (4 times RBE of protons/electron/gamma)
  • Used for inoperable, radioresistent tumors
  • Dose to kill is 1/3 of dose required by photons
  • Alpha particle causes DNA Damage
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7
Q

Stopping theory for Protons

A
  • Rate at which protons lose energy increases as they slow down
  • So rate of energy depends on proton energy and stopping material used.
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8
Q

Scatter theory for protons

A
  • MCS = Multiple columb scattering
  • MCS angles < 16deg
  • Due to elastic columb interactions with the target nuclei
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9
Q

How do protons interact

A
  • Incoming proton enters the nucleus of the tumor and displaces the constituent proton/neutron/light nuclon clusters
  • The secondary proton has much lower energy and larger angles than primary protons
  • Outgoing proton retains characteristic non elastic collisions
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10
Q

Bragg peak / Pristine Bragg peak

A
  • Loses more energy per unit length
  • Reaches a peak where it loses all its energy and then stopped.
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11
Q

Modulators

A
  • Range wheel modulator
  • Can adjust the beam length and bragg peak with this
  • If the wheel stopped spinning, tumor would be partially overdosed and partially underdosed; pristine bragg peak would be delivered with inhomogeneous dose to the target
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12
Q

Surface dose depends on

A

Modulator factor
* Higher the dose, deeper the tumor, higher the skin dose

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13
Q

Compensator

A
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14
Q

Proton Beam Path components

A
  1. First scatter
  2. Second Scatter
  3. Range shifter : determines where the beam stops
  4. Range Modulator: spreads the peak: SBP
  5. Patient Aperture: finds the edges of the beam, made of brass
  6. Patient compensator: gives conformality, reduces scatter in beam, made of wax
  7. Tumor target
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15
Q

Spot scanning
Pencil beam scanning

A

Advantage:
* Less interplay of patient motion with beam

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16
Q

S.I Unit

A

RBE = 1.1equivalent

17
Q

Disadvantages of protons

A
  • Complex margins
  • Motion effects are more important
  • RBE effect
  • If the tumor shrinks the plan changes
  • IGRT technology differs
18
Q

PTV margins for protons

A
  • beam dependent
  • non-Isotropic
  • extend in the beam direction
19
Q

Ion chamber used

A

Multi layer ion chamber
* Zebra
* Giraffe
* Matrixx PT

20
Q

Carbon Ion

A
  • Has 12 protons in the nucleus
  • These are called heavy ion beams
  • High LET, so high dose beyond bragg peak
  • Smaller penumbra than protons
  • Less MCS than protons
  • RBE = 3 or larger equivalent
21
Q

Proton scattering

A

Active Scanning:
* Uses orthogonal magnets
* deflects proton pencil beam
* delivers dose in dmall spots
* susceptinle to missing parts of the tumor as it moves.
* There is proximal dose conformality

Passive Scattering technique:
* USes filters of varying thickness such as modulation wheel to spread the bragg peak.
* Scattering foil in place to spread the beam laterally
* Patient specific aperatures and compensator is designed

22
Q

Deflector

A
  • Generates electrostatic field to redirect protons out of centripetal motion
23
Q

Scattering foil

A

Placed directly into the beam line to widen the beam

24
Q

Range

A
  • The depth of the material at which half of the protons undergo Electromagnetic interactions.
  • Depth at 50%
25
Robust planning
TO minimize uncertainty from tissue heterogeneity during IMPT planning
26
Fast Neutron therapy
* Due to bombarding protons into target * Used for adenoid cyctic carcinomas of H&N * Higher RBE
27
Range Shifter
~ to bolus Used for treating superficial tumors
28
Recoil Protons
They are a result of neutrons interacting with nuclei, hydrogen nucleus It is due to HIgh LET particles resulting form collision of a neutron with a proton.
29
Neutron shielding
* Hydrogen rich materials such as water, concrete, polyethylene, borated polyethylene, compacted earth are used for shielding. * Hydrogen nucleus is approximately the same mass of a neutron, so collision with neutrons will transfer energyvia collision. * After slowing down, these neutrons can be absorbed. * Lead is NOT recommended for shielding Neutrons
30
Proton range
DIstal side of the spread out bragg peak
31
Modulation width
Width of the spread out bragg peak
32
Robustness of proton treatment is insensitivity of PTV and OAR changes in
* Range uncertainty * Patient setup uncertainity * Internal Anatomy
33
Inter play
* Interplay effect occurs when scanning proton beams interact with moving patient anatomy, breath hold and respiratory gating
34
Damaging Neutron range
100 Kev - 2 MeV * They have an RBE from 5 to 20.