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HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov @partners.org Jan Unkelbach, PhD [email protected] Dept of Radiation Oncology MGH April 3, 2007
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HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD [email protected] Jan.

Dec 14, 2015

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Page 1: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

HST.187: Physics of Radiation Oncology

#9. Radiation therapy: optimization in the presence of uncertainty

Alexei Trofimov, [email protected]

Jan Unkelbach, [email protected]

Dept of Radiation Oncology MGH

April 3, 2007

Page 2: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Uncertainties in RT• Intro

– Sources of uncertainty, e.g. -• Set-up, target localization (inter-fractional)• Intra-fractional motion

– Methods to counter the uncertainties• Volume definitions/ margins, treatment techniques

– Effect of uncertainties on the dose distribution

• Probabilistic planning techniques in the presence of uncertainties– Inter-fractional motion and set-up uncertainties – Proton range variations in tissue

• Handling of intra-fractional motion (respiratory) – Image-guided radiation therapy IGRT and “4D” planning– Probability-based motion-compensation– Intro to robust optimization

Page 3: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Target definition: inter-observer variation

Steenbakkers et al R&O 77:182 (2005)

Page 4: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.
Page 5: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Target motion (intra-fractional)

Targeting

Page 6: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Interplay between internal motion and the multi-leaf collimator sequence

JH Kung

P Zygmanski

Page 7: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Target motion (intra-fractional)

Targeting

Radiological depth changes

Inhale Exhale

Page 8: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Planned dose at exhale phase

Liver Tx plan, PA field Planned by J.Adams(TPS: CMS XiO)

As would be delivered at inhale

50%

Page 9: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Set-up uncertainties: day-to-day variation

Images: © 2007 Elsevier IncZhang et al IJROBP 67:620 (2007)

Variation over 8 weeks of treatment

Page 10: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Prostate treatment with protons

Page 11: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.
Page 12: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.
Page 13: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Compensatordesign

Page 14: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Variation In set-up

Page 15: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Compensatorsmear

Page 16: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Compensatorsmear

Page 17: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Intrafractional motion

Page 18: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Part 2:Probabilistic

approach to account for uncertainty in

IMRT/IMPT optimization

Page 19: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Content

• Motivation – interfractional random setup error

• Concept of probabilistic treatment planning

• Application to interfractional motion of the prostate

• Application to range uncertainties in IMPT

Page 20: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

MotivationConsider inter-fractional random setup error in a

fractionated treatment

How can we achieve an improvement?

• Lower dose to regions where tumor is located rarely

• Have to compensate for it by higher dose to other regions

safety margin:

irradiate entire area where tumor may be with the full dose

Page 21: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Motivation

25 moving voxels

45 static voxels

Example:

Question?

Are there static dose fields that yield tumor coverage and improve healthy tissue sparing?

tumor voxels are at 5 different positions equally often

Page 22: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Motivation

Example:

integral dose: 40.8 (instead of 45.0)

Page 23: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

MotivationDose in the moving tumor:

frequency for moving voxel i being at static voxel j

Have to solve system of linear equations to determine static dose field which yields D = 1

dose in moving tumorstatic dose field

Page 24: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Motivation

special solution (safety margin)

Set of solutions is affine subspace

kernel of the mapping P:

Set of static dose fields which preserve D = 1:

kernel dimension (number of static voxels) minus (number of tumor voxels)

Page 25: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Motivation

Intrinsic problems:• only handles predictable motion, not uncertainty

• cannot handle systematic errors

• cannot handle irreproducable breathing pattern

Method could in principle work if motion was predictable and treatment was infinitely long

Need more general method to handle uncertainty!

(having these ideas in mind)

Page 26: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Idea of probabilistic methodMain assumption:

The dose delivered to a voxel depends on a set of random variables

vector of random variables which parameterize the uncertainty

fluence map to be optimized

Assign probability distribution to random variables:

Page 27: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Idea of probabilistic methodApplications:

G = position of voxels

P(G) = Gaussian distribution

• Inter-fractional motion

• range uncertainty

• respiratory motion

G = amplitude, exhale position, starting phase

(note: P(G) unrelated to `breathing PDF`)

G = range shifts for all beamlets

Page 28: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Idea of probabilistic methodPostulate:

optimize the expectation value of the objective function

• incorporate all possible scenarios into the optimization with a weighting that corresponds to its probability of occurrence

Page 29: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Idea of probabilistic methodExample: quadratic objective

1st order term 2nd order term

variance of the dosedifference of expected and prescribed dose

expected dose:

Page 30: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Alternative formulations• In this talk: optimize expectation value

• most desireable might be something in between

(can be solved by robust optimization techniques in linear programming)

• alternative: optimization of the worst case

Page 31: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to prostate

Incorporating

inter-fractional motion

of the prostate

into

IMRT optimization

Page 32: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

application to prostateUncertainty G: positions of voxels

Probability distribution P(G): Gaussian

Page 33: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

application to prostate

static dose field (dose per fraction)

• expected quadratic objective function

• 30 fractions

• large amplitude of motion ( 8mm AP, 5mm LR/CC)

Page 34: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

application to prostateexpected dose in the moving tumor coordinate system

• Best estimate for the dose delivered to a voxel

Page 35: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

application to prostateProblem: Uncertainty implies that we don‘t know the dose distribution which will be delivered

standard deviation: assess uncertainty of the dose in each point

treatment plan evaluation difficult

Page 36: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

application to prostateProbability for the delivered dose to be below/within/above a 3% interval around the prescribed dose

below abovewithin

(D Maleike, PMB 2006)

Page 37: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

application to prostatePrototype GUI to view probabilities for over/under dosage

(D Maleike, PMB 2006)

• user may select dose intervals of interest

Page 38: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to prostate

• Incorporate organ motion in IMRT planning to overcome the need of defining safety margins

• resemble the idea of inhomogeneous dose distributions on static targets in order to achieve better healthy tissue sparing

• control the sacrifice of guaranteed tumor homogeneity

Probabilistic approach can ...

Page 39: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to range uncertainties

Handling range uncertainty

in

IMPT optimization

Page 40: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to range uncertainties

degraded dose distribution if the actual range differs from the assumed range

assumed range + 5 mm - 5 mm

Conventional IMPT treatment plans may be sensitive to range variations

Page 41: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to range uncertaintiesWhy? Because ...

• pencil beams stop in front of an OAR

• dose distributions of individual beams are inhomogeneous

Page 42: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to range uncertainties

Range uncertainty assumptions for probabilistic optimization:

• 5 mm uncertainty (SD) of the bragg peak location for each beam spot

• Gaussian distribution for the range shifts

• is considered a systematic error (no averaging over different range realizations in different fractions)

Page 43: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to range uncertainties

assumed range + 5 mm - 5 mm

• Probabilistic optimization can significantly reduce the sensitivity to range variations

convetional plan

Page 44: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to range uncertaintiesWhy? Because ...

• lateral fall-off of the pencil beam is used

• dose distributions of individual beams are more homogeneous in beam direction

convetional plan

Page 45: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to range uncertaintiesPrice of robustness:• lateral fall-off is more shallow

convetional plan

plan quality for the assumed range is slightly compromised

- higher dose to OAR or reduced target coverage

probabilistic plan

Page 46: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Application to range uncertainties

• take advantage of the characteristic features of the proton beam and the many degrees of freedom in IMPT to make treatment plans robust with respect to range variations

(which cannot be achieved by other known heuristics)

Probabilistic approach can ...

Page 47: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Part 3: Intrafractional motion

Page 48: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Continuous irradiation

Page 49: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

IMRT delivery to a moving target

Int map no motion motion 1 fraction motion 4 fx

Page 50: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

The effect of target motion on dose distribution

Page 51: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Coverage assured with planning margins

Page 52: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Gated Tx at MGH

Varian RPM-system

marker block with IR-reflecting dots

IR-source + CCD camera

Page 53: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

External-internal correlation Tsunashima et al IJROBP 2003

Page 54: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Gierga et al IJROBP 2004:

correlation differs between markers

Page 55: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Phase shift

HHoisak et al IJROBP 2003

Page 56: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

External-internal correlation

• Generally well-correlated, but…

• Not necessarily linear• Phase shift has been observed, not

necessarily constant on different days

• Proportionality coefficients, phase may vary with – marker position– respiratory “discipline” (e.g. compliance with

breath-training/coaching)

Page 57: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

(“Fast”) tracking delivery

Page 58: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Inverse optimization

• Dose calculation using (Dij) matrix:

beamlet jx

voxel i

Page 59: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

4D- influence matrix (D-ij) approach

• Dij ’s are precalculated for all beams and all instances of geometry (4D-CT phases)

• At instance (phase) k we have

k = 1, …, 5: breathing phase

beamlet jx

voxel i

Page 60: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Eike Rietzel, GTY Chen “Deformable registration of 4D CT data” Med Phys 33:4423 (2006)

• Determine voxel displacement vector field between Pk and P0 (reference phase)

P0 (inhale) P4 (exhale)

Page 61: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

• Deformations are then applied to all pencil beams in Dij matrix

pencil beam in P4 (exhale)

same pencil beam transformed to P0(inhale)

x

x

A Trofimov et al PMB 50:2779 (2005)

Page 62: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Continuous irradiation: instantaneous dose distribution

Page 63: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

From a different prospective: a moving instant. dose in a fixed reference geometry

Page 64: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Approaches to temporo-spatial optimization of IMRT

(1) Planning with optimal margins (Internal Target Volume)

(2) Planning with Motion kernel(a) Uniform approach (motion PDF)(b) Adaptive approach (sum influence matrix)

(3) Gating / Unoptimized tracking – plans optimized separately, 1 best plan chosen out of several or all delivered dynamically

(4) Optimized tracking – several plans optimized simultaneously, delivered dynamically

A Trofimov et al PMB 50:2779 (2005)

Page 65: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Lung: CTV vs Internal Target Volume (ITV)

Page 66: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Planning with “Internal” margins - ITV

Page 67: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 1: Optimal margins (ITV): lung

Page 68: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

DVH for ITV plan recalculated for different geometries (CT phases): lung

Page 69: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Approaches to Temporo-Spatial Optimization of IMRT

(1) Planning with expanded margins (ITV)

(2) Planning with modified dose kernel (b) Uniform approach (motion PDF)(a) Adaptive approach (sum influence matrix)

(3) Gating / Unoptimized tracking – plans optimized separately, 1 best plan chosen out of several or all delivered dynamically

(4) Optimized tracking – several plans optimized simultaneously, delivered dynamically

Page 70: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Motion probability distribution function (PDF)

Page 71: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Motion-compensation in IMRT treatment planning• If the motion (PDF) is known

(reproducible), the dosimetric effect can be reduced – Deconvolution of intensity map– Planning with “smeared” beams

– .

Page 72: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Reduction of integral dose with motion-adaptive planning

Page 73: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

.

Motion kernel: “one-size-fits-all” vs. “custom-made”

Original beamlet

=

Convolved “motion” beamlet Sum of deformed beamlets

Page 74: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

IMRT with motion-compensated Tx PlanInt map no motion motion 1 fraction motion 4 fx

Page 75: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Patient data

lung liver

Page 76: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 2a: Motion kernel plan, DVH recalculated for 5 ph’s

Page 77: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

MK plan: DVH recalculated for diff phases

Page 78: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 2b: with averaged Dij-matrices (liver)

Page 79: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 2b: with averaged Dij-matrices (liver)

Page 80: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 2b: with averaged Dij-matrices (liver)

Inhale (recalc’d to reference) Exhale (reference)

Inhomogeneous “per-phase” doses are designed so that the some conforms to the prescription

Page 81: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Approaches to Temporo-Spatial Optimization of IMRT

(1) Planning with expanded margins (ITV)

(2) Planning with modified dose kernel (Motion kernel)(a) Uniform approach (motion PDF)(b) Adaptive approach (sum influence matrix)

(3) Gating / Unoptimized tracking – plans optimized separately, 1 best plan selected for gated delivery or all delivered dynamically

(4) Optimized tracking – several plans optimized simultaneously, delivered dynamically

Page 82: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 3: Gating / Unoptimized tracking (liver)

Page 83: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 3: Gating / Unoptimized tracking (lung)

Page 84: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Approaches to Temporo-Spatial Optimization of IMRT

(1) Planning with optimal margins (ITV)

(2) Planning with modified dose kernel (Motion kernel)(a) Uniform approach (motion PDF)(b) Adaptive approach (sum influence matrix)

(3) Gating / Unoptimized tracking – plans optimized separately, 1 best plan selected for gated delivery or all delivered dynamically

(4) Optimized tracking – several plans optimized simultaneously, delivered dynamically

Page 85: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 4: optimized tracking (lung)

Page 86: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

App. 4: Optimized tracking (lung)

Page 87: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

DVH comparison for the lung case

Page 88: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

DVH comparison for liver case

Page 89: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Ideal case for tracking delivery (vs gating)

Page 90: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

DVH and dose for different “gated” (single phase) plans for the lung case

Page 91: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Sources of delay: RPM: 60-90 ms , 75 ms averageSystem response time : < 5 msWait for the next modulation cycle: 0-100 ms

Total delay: 65-195 ms, average 130 ms

Delivery of gated proton treatment : Timing

Delivery restricted to complete modulation cycles: on/off at the stop block position only

100 ms

Hsiao-Ming Lu

Page 92: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Residual motion with gating Probability distribution

Page 93: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Inter-fractional variability

Liver-2

Page 94: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Cardiac-1

Page 95: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Cardiac-2

Page 96: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Cardiac-1

Time

Positio

nPositio

n

Page 97: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Variability between patients

Lung-2

Liver-2Cardiac-2

Page 98: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Robust formulation for probabilistic treatment planning:

– Tim Chan et al: Phys Med Biol 51:2567 (2006)

– Outcome will be “acceptable” as long as the realized motion is within the expected “limits”

Page 99: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

PDFuncertaintybounds

Realized PDF

Realized PDFPlanning PDF

Planning PDF

Dose to moving target

Page 100: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Summary• (Some) sources of uncertainty in RT:

imaging, target definition, dose calc, set-up, inter-, intra-fractional motion

• Margin/ITV approach is the most robust for target coverage, but substantially increases dose to healthy tissue

• Image-guided RT improves dose conformity, reduced irradiation of healthy tissues, BUT relatively complex delivery, not error-proof

• Probabilistic motion-adaptive treatment planning in combination with image-guided delivery may be the optimal solution

Page 101: HST.187: Physics of Radiation Oncology #9. Radiation therapy: optimization in the presence of uncertainty Alexei Trofimov, PhD atrofimov@partners.org Jan.

Acknowledgements

J Adams

T Bortfeld, PhDT Chan, PhDS Jiang, PhDJ Kung, PhDHM Lu, PhDH Paganetti, PhD

E Rietzel, PhD

C Vrancic