System and method for planning a radiation therapy treatment

US9251302B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-9251302-B2
Application numberUS-201414154725-A
CountryUS
Kind codeB2
Filing dateJan 14, 2014
Priority dateJan 14, 2014
Publication dateFeb 2, 2016
Grant dateFeb 2, 2016

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Abstract

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A method for planning a radiation therapy treatment of a body represented by a volume of voxels determines a radiation dose matrix representing a spatial distribution of a radiation dose of beams of radiation irradiating the volume with homogeneous stopping power. The beams are collimated and are shifted copies of each other at each depth of the volume, and the spatial distribution is determined by calculating cumulative beam-axial doses in a single matrix-matrix multiplication and redistributing the cumulative beam-axial doses to all voxels in the volume using a convolution. Next, a set of correcting operations is applied to the radiation dose matrix to produce a cumulative voxel radiation dose of the volume. Each correcting operation is linear, independent from another correcting operation and has a transform.

First claim

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I claim: 1. A method for planning a radiation therapy treatment of a body represented by a volume of voxels, comprising: determining a radiation dose matrix representing a spatial distribution of a radiation dose of beams of radiation irradiating the volume with homogeneous stopping power, wherein the beams are collimated and are shifted copies of each other at each depth of the volume, wherein the spatial distribution is determined by calculating cumulative beam-axial doses in a single matrix-matrix multiplication and redistributing the cumulative beam-axial doses to all voxels in the volume using a convolution; and applying a set of correcting operations to the radiation dose matrix to produce a cumulative voxel radiation dose of the volume, wherein each correcting operation is linear, independent from another correcting operation and has a transform, wherein steps of the method are performed by at least one processor. 2. The method of claim 1 , wherein the determining comprises: multiplying a vector representing weights of the beams by a matrix representing energy profiles of the beams to estimate values of a total radiation at each depth of each beam; substituting values in an zeroed 3D array representing the voxels in the volume with corresponding values of the total radiation; and convolving each depth plane in the volume with a spreading kernel. 3. The method of claim 1 , wherein the determining comprises: determining the radiation dose matrix as a matrix-vector products Aw of a fluence matrix A representing relative intensity of radiation delivered to each voxel in the volume by each beam and a vector of nonnegative beam weights w representing time of radiation of each beam of radiation according to Aw =vec( B T mat( w )( N N )), wherein N be a matrix in which each column is a spatially shifted copy of values of lateral distribution, B is a matrix of spatially shifted energy profiles, such that each column in the matrix B includes an energy profile for the beams in the same depth, wherein is a Kronecker product of matrices, a function vec(•) vectorizes its argument, and a function mat(•) reshapes its argument into a matrix that conforms with its left and right multiplicands, and wherein T is a transpose operator. 4. The method of claim 1 , wherein the set of correcting operations includes an operation for correcting a uniformity of a lateral distribution of energy of each beam at each depth, comprising: convolving each row of the radiation dose matrix to determine the multiplication (N N), wherein the convolving includes a first convolution with a first vector in a first lateral direction, followed by a second convolution with a second vector in a second lateral direction orthogonal to the first lateral direction. 5. The method of claim 4 , wherein the convolving is according to ∑ j J ⁢ ⁢ ( ∑ i ⁢ ⁢ w i ⁢ v j ⁡ ( z ) ⁢ B i ⁡ ( z ) ) · N ⁡ ( ( x , y ) , σ j 2 ) , wherein w i is the weight on the ith beam, B i (z) is an integral of an energy profile at a depth z, and N((x, y),σ 2 i (z)) is a 2D Gaussian field of variance σ 2 i (z) centered at an axis (x, y), an v j is a spreading kernel in a set J predetermined for the depth z. 6. The method of claim 1 , wherein the set of correcting operations includes an operation for correcting an assumption of the homogeneous stopping power, further comprising: stretching each voxel in proportion to the stopping power of corresponding tissue of the volume to produce a stretched grid; determining a redistribution matrix R that linearly maps irradiation values deposited into a regular grid to values deposited into the stretched grid; and multiplying the redistribution matrix R with the radiation dose matrix. 7. The method of claim 1 , wherein the set of correcting operations includes an operation for correcting an assumption of a parallel distribution of the collimated beams, further comprising: counter-warping a Euclidean space of tissue density data of the volume before determining the radiation dose; and reversing the counter-warping after determining the radiation dose. 8. The method of claim 1 , wherein the set of correcting operations includes an operation for correcting multi-port propagation of the beams of radiation using a rotation of the volume with respect to, further comprising: counter-rotating the volume to align a grid of the volume with a port to produce a counter-rotated volume; determining a rotation matrix to redistribute the radiation dose in each voxel of the volume to corresponding voxels in the counter-rotated volume; and summing the radiation dose of the corresponding voxels of the volume and the counter-rotated volume. 9. The method of claim 1 , further comprising: adding to the volume a proximal layer of voxels with a stopping power equivalent to a cumulative stopping power of media between a source of the beams and the body. 10. The method of claim 1 , further comprising: performing transform operations to the cumulative voxel radiation dose of the volume in an order reversed from an order of operations determining the cumulative voxel radiation dose. 11. A method for planning a radiation therapy treatment of a body represented by a volume of voxels, comprising: determining a radiation dose matrix representing a spatial distribution of a radiation dose of a regular 3D grid of beam

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Classifications

  • Complex mathematical operations {(function generation by table look-up G06F1/03; evaluation of elementary functions by calculation G06F7/544)} · CPC title

  • Physics · mapped topic

  • Design optimisation, verification or simulation (optimisation, verification or simulation of circuit designs G06F30/30) · CPC title

  • A61N5/1031Primary

    using a specific method of dose optimization · CPC title

  • relating to mechanical, radiation or invasive therapies, e.g. surgery, laser therapy, dialysis or acupuncture · CPC title

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What does patent US9251302B2 cover?
A method for planning a radiation therapy treatment of a body represented by a volume of voxels determines a radiation dose matrix representing a spatial distribution of a radiation dose of beams of radiation irradiating the volume with homogeneous stopping power. The beams are collimated and are shifted copies of each other at each depth of the volume, and the spatial distribution is determine…
Who is the assignee on this patent?
Mitsubishi Electric Res Lab
What technology area does this patent fall under?
Primary CPC classification G06F17/5009. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Feb 02 2016 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 1 related publication on this page (citations in our corpus or others sharing the same primary CPC).