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S191

ESTRO 36 2017

_______________________________________________________________________________________________

Fig 1: Dose mean lineal energy ratios between Co-60 and

100 kVp Fig 2: Dose mean lineal energy ratios as a

function of

scoring diameter

X-rays as a function of scoring diameter. The dotted line

corresponds for various brachytherapy sources.

to α-ratio of 1.20.

Conclusion

Currently, the International Commission on Radiation

Protection (ICRP) assigns a radiation weighting factor of

unity for all photon emitting sources, equating the RBE of

high and low energy photon sources. However, the clinical

RBE for lower energy brachytherapy sources are

considerably above unity and should be taken into account

during the treatment planning process, to ensure that the

equivalent dose delivered to the tumour is similar for

different sources.

OC-0360 Dose warping uncertainties for the

cumulative rectal wall dose from brachytherapy in

cervical cancer

L.E. Van Heerden

1

, N. Van Wieringen

1

, C. Koedooder

1

,

C.R.N. Rasch

1

, B.R. Pieters

1

, A. Bel

1

1

Academic Medical Center, Radiation Oncology,

Amsterdam, The Netherlands

Purpose or Objective

Brachytherapy (BT) is part of radiotherapy for women with

locally advanced cervical cancer; nowadays, BT is

commonly given in multiple applications to the tumour

area. In clinical practice, the 2 cm

3

receiving the highest

dose (D

2cm3

) in the rectum is calculated by assuming that

the high dose volumes overlap for each treatment. To

account for rectal deformation due to differences in filling

and/or the presence of air, many authors state it is

preferable to sum the 3D dose distributions using dose

warping after deformable image registration (DIR).

However, little is known about the reliability of DIR for

dose warping. The purpose of this study is to quantify the

dose warping uncertainty in the rectum using a physically

realistic model, which describes rectal deformation.

Material and Methods

Seven patients were studied, treated with MRI-guided PDR

BT (two times 24 x 0.75 Gy, given in two applications BT1

and BT2). DIR was performed using the Feature-Based

Deformable Registration (FBDR) tool, connected to a

research version of Oncentra®Brachy (Elekta

Brachytherapy, Veenendaal, the Netherlands). The

delineated rectums were converted to 3D surface meshes,

and a mapping was established to propagate elements on

the surface of rectum

BT1

to the surface of rectum

BT2

. The

transformation vectors were used to deform the BT1 dose

distribution. Next, the BT1 and BT2 doses were summed

voxel-by-voxel. To investigate the dose warping

uncertainty a physically realistic model (PRM) describing

rectal deformation was used. In this model the central

axes of rectum

BT1

and rectum

BT2

were constructed. The

axes were assumed to be fixed in length. For both

rectum

BT1

and rectum

BT2

, orthogonal planes were

reconstructed at 5 evenly spaced positions on the axis

(Fig. A). 100 points were evenly distributed over the

intersection curve of each plane with the rectal wall. It is

assumed that the most dorsal point of the rectum is fixed

and also that the rectal wall only stretches

perpendicularly to the central axis. For point pairs on

rectum

BT1

and rectum

BT2

that were at the same location

according to the PRM, the dose for BT1 and BT2 was added

(D

PRM

) and compared as a 'ground truth” to the DIR

accumulated dose (D

DIR

) in the BT2 point. For BT, the high

dose regions in the OAR are most relevant and points

within the 2 cm

3

volume receiving the highest dose should

be correctly identified. We therefore evaluated the

percentage of points where D

PRM

and D

DIR

were both >D

2cm3

.

Results

Over all patients, D

DIR

varied between 1.1-44.4Gy

EQD2

and

D

PRM

varied between 1.1-40.1Gy

EQD2

(α/β=3Gy for late OAR

toxicity, T

1/2

=1.5 hours). For point pairs, the absolute

difference between D

DIR

and D

PRM

was 0-8.3Gy

EQD2

(Fig. B).

The 2 cm

3

volumes receiving the highest dose according to

the two models have an overlap of 66% (Fig. C).

Conclusion

With the rectal model it is feasible to quantify dose

warping uncertainties, which could be as high as 8.3

Gy

EQD2

. Most points (>66%) in high dose regions were

correctly identified as part of D

2cm3

.