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S934

ESTRO 36 2017

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compared to NTCP models that predict the risk of

pneumonitis.

Material and Methods

A cohort of 9 NSCLC patients made up of 4 patients (ID 71

to 74) that developed pneumonitis after radiotherapy and

5 patients that remained asymptomatic after radiotherapy

(ID 10 to 14) was selected. Radiotherapy planning CT

images were acquired at 3 mm slice thickness with a pixel

resolution of 1 mm. 6 patients were treated with 55 Gy in

20 fractions and 3 patients with 60 Gy in 30 fractions.

Treatment plans were produced on Eclipse using a pencil

beam convolution dose calculation algorithm. 7

radiobiological models were used to calculate NTCP on the

whole, right and left lungs. Image texture analysis was

used to calculate 99 unique features on 32x32 and 20x20

pixel

2

subimages within the whole lung volume. Redundant

texture features were removed and a neural network (NN)

trained to classify the results.

Results

The predicted NTCP values are shown in Figure 1 for the

analysis of the whole lung volume (normal lung tissue

excluding the GTV). Similar results were obtained for the

right and left lungs. Although model 5, symptomatic or

radiographic pneumonitis <=6 months, showed high NTCP

values this was not specific to patients with confirmed

pneumonitis. Similar values were obtained in patients

showing no signs of pneumonitis. The image texture

analysis results identified the risk of pneumonitis most

notably in the right lung (87.49%).

Figure 1

: NTCP results on the 9 patients (ID 10-14

asymptomatic, 71-74

symptomatic).

Table 1

: Texture analysis classification on the whole lung

and right and left lung volumes.

Conclusion

These preliminary results show that it is possible to predict

radiation-induced pneumonitis, both prior to treatment

and independently of dosimetric evaluation, using image

texture analysis of the radiotherapy planning CT images.

However further validation on a larger patient cohort is

required.

EP-1726 Efficacy of vendor supplied distortion

correction algorithms for a variety of MRI scanners

E.P. Pappas

1

, I. Seimenis

2

, D. Dellios

2

, A. Moutsatsos

1

, E.

Georgiou

1

, P. Karaiskos

1

1

National and Kapodistrian University of Athens, Medical

Physics Laboratory - Medical School, Athens, Greece

2

Democritus University of Thrace, Medical Physics

Laboratory - Medical School, Alexandroupolis, Greece

Purpose or Objective

Although inherently distorted, Magnetic Resonance Images

(MRIs) are being increasingly used in stereotactic

radiosurgery (SRS) treatment planning in order to take

advantage of the superior soft tissue contrast they exhibit.

MR scanner manufacturers have equipped their units with

distortion correction algorithms to mainly compensate for

gradient nonlinearity induced spatial inaccuracies. The

purpose of this study is to assess the accuracy of these

algorithms by comparing distortion maps deduced with

and without the optional distortion correction schemes

enabled for a variety of MRI scanners.

Material and Methods

A custom acrylic-based phantom was designed and

constructed in-house. Its external dimensions were limited

to approximately 17x16x16 cm

3

in order to accurately fit

in a typical head coil while extending to the edges of the

available space. On eleven axial planes, a total of 1978

holes were drilled, the centers of which serve as control

points (CPs) for distortion detection. Center-to-center CP

distance is 10 mm on x and y axis and 14 mm on z axis,

resulting in adequately high CP density. The phantom was

filled with copper sulfate solution and MR scanned at 1.5T

(SIEMENS Avanto, Philips Achieva) and 3.0T (SIEMENS

Skyra) using the corresponding standard clinical MR

protocol for SRS treatment planning. All scans were

repeated after disabling the vendor supplied distortion

correction scheme. The phantom was emptied and CT

scanned to provide the reference CP distribution. In-house

MATLAB routines were developed for distortion

assessment. Reference and evaluated CP distributions

were spatially registered and compared to derive 3D

distortion maps. This methodology does not consider

uniform geometric distortion as it cancels out during the

spatial registration step. This results in omitting uniform

susceptibility-induced CP dispositions and thus mainly

takes into account machine-related distortions.

Results

At central slices, around the scanners’ isocenters

minimum distortion was detected even with the correction

algorithms disabled. However, at the edges of the

available space distortion magnitude greatly increases

(figure 1) and efficacy of algorithm becomes paramount.

Maximum detected distortion reaches 3 mm for the

SIEMENS 3.0T scanner but is reduced to less than 1.5 mm

if the correction algorithm is enabled. For the 1.5T

scanners slightly lower corresponding values were

observed.