2006
DOI: 10.1007/s10479-006-0082-z
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Using eigenstructure of the Hessian to reduce the dimension of the intensity modulated radiation therapy optimization problem

Abstract: Optimization is of vital importance when performing intensity modulated radiation therapy to treat cancer tumors. The optimization problem is typically large-scale with a nonlinear objective function and bounds on the variables, and we solve it using a quasiNewton sequential quadratic programming method. This study investigates the effect on the optimal solution, and hence treatment outcome, when solving an approximate optimization problem of lower dimension. Through a spectral decompostion, eigenvectors and e… Show more

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Cited by 11 publications
(8 citation statements)
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References 11 publications
(13 reference statements)
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“…In our study, the objective function F is a weighted sum of standard IMRT penalty functions such as one-and two-sided quadratic penalty functions and gEU D, see e.g. [7] for mathematical formulations of the former and [17] for the latter. The parameters of the penalty functions are set up according to RTOG protocols; see Section 3.2 and Table 1 for details.…”
Section: Direct Step-and-shoot Optimizationmentioning
confidence: 99%
“…In our study, the objective function F is a weighted sum of standard IMRT penalty functions such as one-and two-sided quadratic penalty functions and gEU D, see e.g. [7] for mathematical formulations of the former and [17] for the latter. The parameters of the penalty functions are set up according to RTOG protocols; see Section 3.2 and Table 1 for details.…”
Section: Direct Step-and-shoot Optimizationmentioning
confidence: 99%
“…Also, the eigenvectors for the large eigenvalues span the subspace of I where F ( I ) changes rapidly, which corresponds to difficult trade-offs between targets and OARs. Carlsson et al (2006) further parameterized the intensities I by a few dominant eigenvectors from the Hessian, i.e., I = V p ξ, which is the to (5), the same as (9) except that V p contains p dominant eigenvectors from H . According Hessian in (10) can be written in the matrix form: H=ATDA,D=diagtrue{1N,,1Nwminϴ(DminDi),,1Nwmaxϴ(DjDmax),true} which depends on the dose coefficients A ij , the current dose distribution D i and the parameter settings ( w min , w max , etc).…”
Section: Methodsmentioning
confidence: 99%
“…The IMRT degeneracy problem (i.e., the phenomenon that different intensity distributions can lead to nearly identical dose statistics) is related to the small eigenvalues of H. Also, the eigenvectors for the large eigenvalues span the subspace of I where F(I) changes rapidly, which corresponds to difficult trade-offs between targets and OARs. Carlsson et al (2006) further parameterized the intensities I by a few dominant eigenvectors from the Hessian, i.e., I = V p ξ, which is the to (5), the same as (9) except that V p contains p dominant eigenvectors from H. According Hessian in (10) can be written in the matrix form:…”
Section: Dimension Reduction In the Optimized Intensity Spacementioning
confidence: 99%