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Optimizing Radiation Treatment Planning for Tumors Using IMRT

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Title: Optimizing Radiation Treatment Planning for Tumors Using IMRT


1
Optimizing Radiation Treatment Planning for
Tumors Using IMRT
  • Laura D. Goadrich
  • Industrial Engineering Department of Computer
    Sciences at University of Wisconsin-Madison
  • April 19, 2004

2
Overview
  • Radiotherapy motivation
  • Conformal radiotherapy
  • IMRT
  • Mechanical constraints
  • MIP method
  • Input/output
  • Langer, et. al. Approach
  • Monoshape constraints
  • Implementation results
  • References

3
Motivation
  • 1.2 million new cases of cancer each year in U.S.
    (times 10 globally)
  • Half undergo radiation therapy
  • Some are treated with implants, but most with
    external beams obtained using radiotherapy
    treatments.

4
Radiotherapy Motivation
  • Used to fight many types of cancer in almost
    every part of the body
  • Approximately 40 of patients with cancer needs
    radiation therapy sometime during the course of
    their disease
  • Over half of those patients who receive
    radiotherapy are treated with an aim to cure the
    patient
  • to treat malignancies
  • to shrink the tumor or to provide temporary
    relief of symptoms
  • In the use of radiation, organ and function
    preservation are important aims (minimize risk to
    organs at risk (OAR)).

5
Planning Radiotherapy- CAT scan
  • Conduct scans of the section of the body
    containing the tumor
  • Allows physicians to see the OAR and surrounding
    bodily structures

6
Planning Radiotherapy- tumor volume contouring
  • Isolating the tumor from the surrounding OAR is
    vital to ensure the patient receives minimal
    damage from the radiotherapy
  • Identifying the dimensions of the tumor is vital
    to creating the intensity maps (identifying where
    to focus the radiation)

7
Planning Radiotherapy- beam angles and creating
intensity maps
  • Multiple angles are used to create a full
    treatment plan to treat one tumor.
  • Through a sequence of leaf movements, intensity
    maps are obtained

8
Option 1 Conformal Radiotherapy
  • The beam of radiation used in treatment is a 10
    cm square.
  • Utilizes a uniform beam of radiation
  • ensures the target is adequately covered
  • however does nothing to avoid critical structures
    except usage of some blocks

9
Option 2 IMRT
  • Intensity Modulated Radiotherapy (IMRT) provides
    a shaped array of 3mm beamlets using a Multi-Leaf
    Collimator (MLC), which is a specialized,
    computer-controlled device with many tungsten
    fingers, or leaves, inside the linear
    accelerator.
  • Allows a finer shaped distribution of the dose to
    avoid unsustainable damage to the surrounding
    structures (OARs)
  • Implemented via a Multi-Leaf Collimator (MLC)
    creating a time-varying opening (leaves can be
    vertical or horizontal).

10
Classical vs. IMRT
11
IMRT machine
12
IMRT Planning- intensity map
  • There is an intensity map for each angle
  • 0 means no radiation
  • 100 means maximum dosage of radiation
  • Multiple beam angles spread a healthy dose
  • A collection of shape matrices are created to
    satisfy each intensity map.

13
Intensity map to shape matrices
Original Intensity Matrix
Shape Matrix 1
Shape Matrix 3
Shape Matrix 2
Shape Matrix 4
14
Program Input/Output
  • Input
  • An mxn intensity matrix A(ai,j) comprised of
    nonnegative integers
  • Output
  • T aperture shape matrices dtij such that zK of
    the matrices are used where K lt T
  • Non-negative integers ?t (tI..T) giving
    corresponding beam-on times for the apertures
  • Apertures obey the delivery constraints of the
    MLC and the weight-shape pairs satisfying
  • K is the total number of
  • required shape matrices

15
Mechanical Constraints
  • After receiving the intensity maps, machine
    specific shape matrices must be created for
    treatment
  • There are numerous types of IMRT machines
    currently in clinical use, with slightly
    different physical constraints that determine the
    leaf positions (hence the shape matrices)
    possible for the device
  • Each machine has varying setup times which can
    dominate the radiation delivery time (beam-on
    time)
  • To limit patient discomfort and subtle movement
    from initial placing limit the time the patient
    is on the table
  • Goals
  • Minimize beam-on time
  • Minimize number of different shapes

16
Approach Langer, et. al.
  • Mixed integer program (MIP) with Branch and Bound
    by Langer, et. al. (AMPL solver)
  • MIP linear program with all linear constraints
    using binary variables
  • Langer suggests a two-phase method where
  • First minimized beam-on time
  • T is the upper bound on the
  • number of required shape matrices
  • Second minimize the number of segments (subject
    to a minimum beam-on time constraint)
  • gt 1 if an element switches from
  • covered to uncovered (vice versa)
  • 0 otherwise

17
In Practice
  • While Langer, et. al. reports that solving both
    minimizations takes a reasonable amount of time,
    he does not report numbers and we have found that
    the time demands are impractical for real
    application.
  • To obtain a balance between the need for a small
    number of shape matrices and a low beam-on time
    we have found that
  • numShapeMatricies7 beam-on time
  • Initializing T close to the optimal number of
    matrices 1 required reduces the solution space
    and solution time

18
Constraint Leaves cannot overlap from right and
left
  • To satisfy the requirement that leaves of a row
    cannot override each other implies that one beam
    element cannot be covered by the left and right
    leaf at the same time

ptij 1 if beam element in row i,
column j is covered by the right leaf
when the tth monitor unit
is delivered 0 otherwise ltij is similar
for the right leaf dtij contains the final tth
monitor unit
19
Constraint Full leaves and intensity matrix
requirements
  • Every element between the leaf and the side of
    the collimator to which the leaf is connected is
    also covered (no holes in leaves).

20
Constraint No leaf collisions
  • Due to mechanical requirements, leaves can move
    in only one direction (i.e. the right leaf to the
    right). On one row, the right and left leaves
    cannot overlap

21
Constraint Shape matrices reqs
  • The total number of shape matrices expended it
    tallied
  • z 1 when at least one beam element
    reamins exposed
  • when the tth monitor unit in
  • the sequence is delivered
  • 0 otherwise
  • I is the number of rows
  • J is the number of columns
  • Must satisfy the intensity matrix for each
    monitor unit.
  • I is the intensity assigned to
  • beam element ij

22
Constraint Monoshape
  • The IMRT delivery is required to contain only one
    shape matrix per monitor unit, a monoshape
  • First determine which rows in each monitor unit
    are open to deliver radiation

deliveryit1 if the ith row is being used
a time t 0 otherwise
  • Determine if the preceding row in the monitor
    unit delivers radiation

dropit1 if the preceding row (i-1)
in a shape is non-zero and the
current row (i) is 0 0 otherwise
23
Constraint Monoshape
  • Determine when the monoshape ends

jumpit1 if the preceding row (i-1)
in a shape is zero and the current
row (i) is nonzero 0 otherwise
  • There can be only one row where the monoshape
    begins and one row to end

24
Complexity of problem
  • To account for all of the constraints there is a
    large number of variables and constraints.

25
Comparison of results
  • Corvus version 4.0

26
Comparison of results
  • Corvus version 5.0

27
Referenced Papers
  • N. Boland, H. W. Hamacher, and F. Lenzen.
    Minimizing beam-on time in cancer radiation
    treatment using multileaf collimators. Neworks,
    2002.
  • Mark Langer, Van Thai, and Lech Papiez, Improved
    leaf sequencing reduces segments or monitor units
    needed to deliver IMRT using multileaf
    collimators, Medical Physics, 28(12), 2001.
  • Ping Xia, Lynn J. Verhey, Multileaf collimator
    leaf sequencing algorithm for intensity modulated
    beams with multiple static segments, Med. Phys.
    25 (8), 1998.
  • T.R. Bortfield, D.L. Kahler, T.J Waldron and
    A.L.Boyer, X-ray field compensation with
    multileaf collimators. Int. J. Radiat. Oncol.
    Biol. 28 (1994), pp. 723-730.
  • Bortfield, Thomas, et. al. Current IMRT
    optimization algorithms principles, potential
    and limitations Presentation 2000.
  • Dink, Delal, S.Orcun, M. P. Langer, J. F. Pekny,
    G. V. Reklaitis, R. L. Rardin, Importance of
    sensitivity analysis in intensity modulated
    radiation therapy (IMRT) 2003.
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