2022
DOI: 10.1002/mp.15998
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Novel approach for the evaluation of dose conformity in radiotherapy

Abstract: Purpose We describe a new approach to evaluate conformity of dose distributions in radiotherapy. Methods The suggested conformity factor λ is defined by using existing conformity indices and expansion of the planning target volume (PTV). If the average distance (d¯$\bar d$) between the PTV and reference isodose surface and an arbitrarily selected PTV expansion margin (dexp${d_{exp}}$) are both much smaller than the size of the PTV, then λ approximately equals the ratio trued¯dexp$\frac{{\bar d}}{{{d_{exp}}}}$.… Show more

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Cited by 2 publications
(6 citation statements)
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“…In addition, CIdexp$C{I_{{d_{exp}}}}$ can be used to distinguish between overdosing normal tissue and underdosing treatment target. The latter feature of CIdexp$C{I_{{d_{exp}}}}$ differentiates it from the conformity factor recently described in 18 . Note also that in the presented framework (see Section 2), the “pass” and “fail” criteria for dose conformity assessment can be defined by the conditions CIdexp<1$C{I_{{d_{exp}}}} &lt; 1$ and CIdexp1$C{I_{{d_{exp}}}} \ge 1$, respectively, for appropriately chosen dexp${d_{exp}}$.…”
Section: Introductionmentioning
confidence: 89%
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“…In addition, CIdexp$C{I_{{d_{exp}}}}$ can be used to distinguish between overdosing normal tissue and underdosing treatment target. The latter feature of CIdexp$C{I_{{d_{exp}}}}$ differentiates it from the conformity factor recently described in 18 . Note also that in the presented framework (see Section 2), the “pass” and “fail” criteria for dose conformity assessment can be defined by the conditions CIdexp<1$C{I_{{d_{exp}}}} &lt; 1$ and CIdexp1$C{I_{{d_{exp}}}} \ge 1$, respectively, for appropriately chosen dexp${d_{exp}}$.…”
Section: Introductionmentioning
confidence: 89%
“…Let trued¯${\bar d_{\bot} }$ denote average distance between the surfaces of the PTV and ADref${A_{{D_{ref}}}}$ (see Appendix ). If the distance between the surfaces is sufficiently small (i.e., trued¯${\bar d_{\bot} }$ is much smaller than the sizes of the PTV and ADref${A_{{D_{ref}}}}$), then we have 18 Vunibadbreak−Vintgoodbreak≈d¯SPTV.$$\begin{equation}{V_{uni}} - {V_{int}} \approx {\bar d_{\bot} }{S_{PTV}}.\end{equation}$$Likewise, in the case when dexp${d_{exp}}$ is much smaller than the size of the PTV, we also have VPTVexpVPTVbadbreak≈dexpSPTV$$\begin{equation}{V_{PT{V_{exp}} - }}{V_{PTV}} \approx {d_{exp}}{S_{PTV}}\end{equation}$$From Equations (), (), and (), it follows that CIdexpbadbreak≈trued¯dexp.$$\begin{equation}C{I_{{d_{exp}}}} \approx \frac{{{{\bar d}_{\bot} }}}{{{d_{exp}}}}.\end{equation}$$…”
Section: Methodsmentioning
confidence: 99%
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