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S916

ESTRO 36 2017

_______________________________________________________________________________________________

features in the two CT modalities were compared based

on the intraclass correlation coefficient (ICC1). The

prognostic value of both modalities was assessed using

univariable Cox regression. Additionally, in a previous

analysis we built a local tumor control prognostic model

based on contrast enhanced CT images of 93 patients. It

comprised three radiomic features (HHH large zone high

grey-level emphasis, LLL sum entropy and LLH difference

variance). The performance of this model was

comparatively tested in the two new CT datasets.

Results

118 out of 693 radiomic features showed a good

agreement between native CT and contrast enhanced CT

imaging (ICC>0.8). None of the intensity features was

stable and only 7 of the texture features in the non

transformed map. In the univariable Cox regression 96 and

107 radiomic features in the native and contrast-enhanced

CT images had a significant influence on the local control,

respectively. 62 parameters were prognostic in both

modalities, but only half of them showed a good

agreement between native and contrast enhanced CT

images (ICC>0.8). Two out of the three features of our

previously developed model were stable in respect to the

administration of contrast agent in the CT images

(ICC>0.8). However, our model was only predictive for the

parameter set derived from the contrast enhanced CT

images (CI=0.69, p=0.013). Based on this, patients could

be divided into 2 risk groups (p=0.02, Figure 1).

Figure 1: The patients could be divided into two risk

groups (p=0.02) based on the radiomics of contrast

enhanced CT images and the model derived from our

previous training cohort (contrast enhanced CTs). The

splitting was not significant for radiomics of native CT

images.

Conclusion

Radiomic models can be built on a mixed set of native and

contrast-enhanced CT images but with a reduced number

of suitable radiomic features. A model built exclusively

with contrast enhanced CT images cannot be validated in

a set of native CT Images.

EP-1698 Impact of motion and segmentation on PET

texture features: evaluation with heterogeneous

phantoms.

M. Carles

1,2

, I. Torres-Espallardo

2

, D. Baltas

1

, U. Nestle

1

,

L. Martí-Bonmatí

2

1

University Medical Center, Department of Radiation

Oncology, Freiburg, Germany

2

Hospital Universitario y Politécnico La Fe, Medical

Imaging, Valencia, Spain

Purpose or Objective

A major source of error in quantitative PET/CT of lung

cancer tumors is respiratory motion. Regarding variability

of PET textures features (TF), the impact of respiratory

motion has not been properly studied with experimental

phantoms. The primary aim of this work was to evaluate

the current use of PET texture analysis for heterogeneity

characterization in lesions affected by respiratory motion.

Material and Methods

Twenty-eight heterogeneous lesions were simulated by a

mixture of alginate and 18F- fluoro-2-deoxy-D-glucose

(FDG). Sixteen respiratory patterns were applied. Firstly,

the TF response for different heterogeneous phantoms and

its robustness with respect to the segmentation method

were calculated. Secondly, the variability for TF derived

from PET image with (gated, G-) and without (ungated, U-

) motion compensation was analyzed. Finally, TF

complementarity was assessed.

Results

In the comparison of TF derived from the ideal contour

(VOI_Ideal) with respect to TF derived from 40%-threshold

(VOI_40%) and adaptive-threshold (VOI_COA) PET

contours, 7/8 TF showed strong linear correlation LC

(p<0.001, r>0.75), despite a significant volume

underestimation. Independence on lesion movement (LC

in 100% of the combined pairs of movements, p<0.05) was

obtained for 1/8 TF with U-image (width of the volume-

activity histogram, WH) and 4/8 TF with G-image (WH and

energy ENG, local-homogeneity LH and entropy ENT,

derived from the co-ocurrence matrix). Apart from WH

(r>0.9, p<0.001), no one of these TF has shown LC with

Cmax. Complementarity was observed for the TF pairs:

ENG-LH, CONT-ENT and LH-ENT.

Conclusion

In conclusion, effect of respiratory motion should be taken

into account when heterogeneity of lung cancer is

quantified on PET/CT images. Despite inaccurate volume

delineation, TF derived from 40% and COA contours could

be reliable for their prognostic use. The TF that exhibited

simultaneously added value and independence of lesion

movement were ENG and ENT computed from G-image.

Their use is therefore recommended for heterogeneity

quantification of lesions affected by respiratory motion.

EP-1699 The simulation study of position and biology

of target with PET in high energy X-Ray irradiation

Q. Zhang

1

1

Topgrade Medical - Yiren Hospiatl, Radio- therapy

center, BEIJING, China

Purpose or Objective

To study the possibility of in situ

verification of dose distributions and position in radiation

therapy with PET imaging based on the activity

distribution of

11

C and

15

O produced via photonuclear

reactions in patient irradiated by 45MV X ray from the

LA45 accelerator.

Material and Methods

The method is based on the photonuclear reactions in the

most elemental composition

12

C,

16

O in body tissues

irradiated with high-energy photons with energies up to 45

MeV, resulting primarily in

11

C and

15

O, which are positron

emitting nuclei. The induced positron activity

distributions were obtained with a PET scanner in the

same room of a LA45 accelerator (Top Grade Medical,

Beijing, China). The activity distributions of

11

C and

15

O

were used to verify the dose distributions and position in

tarfet as delivered by the LA45 accelerator.

The experiments were performed with a brain phantom.

Radiation beams were delivered to the phantom according

to realistic radiation therapy treatment plans. The

phantom was immediately transfer to PET anfd was

scanned on the PET after irradiation. The scans were

performed at 20 minutes and 2-5 minutes after irradiation

for

11

C and

15

O, respectively. The interval between the two

scans was 20 minutes. The activity distributions of

11

C and

15

O within the irradiated volume can be separated from

each other because the half-life of

11

C and

15

O is 20