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Conclusion:

For some isotopes the knowledge of the calibrator behavior

with different geometry is essential to evaluate accurately the activity value.

With 123I the measure is significantly affected by composition and thick-

ness of container; with 90Y the volume correction is essential.

http://dx.doi.org/10.1016/j.ejmp.2016.01.341

C.336

PERFORMANCE CHARACTERISTICS OF BIOGRAPH MCT TOF-PET/CT

SCANNER

I. Bonetti

* , a ,

G. Sceni

b ,

E. Cefalì

b ,

S. Morano

c ,

V. Scaffidi

c ,

M. Guerrisi

d .

a

Section of Medical Physics, School of Medical Physics – University of Rome

Tor Vergata – Faculty of Medicine, Roma, Italy;

b

Department of Medica Physics,

A.O. Bianche Melacrino Morelli, Reggio Calabria, Italy;

c

Department of Nuclear

Medicine, A.O. Bianche Melacrino Morelli, Reggio Calabria, Italy;

d

Section of

Medical Physics, Department of Biomedicine and Prevention, University of Rome

Tor Vergata-Faculty of Medicine, Roma, Italy

Introduction:

The aim of this work is to characterize the physical

properties of the Biograph mCT – TOF PET/CT scanner recently

installed at Nuclear Medicine Department in Ospedali Riuniti Reggio

Calabria.

Materials and Methods:

The Biograph mCT scanner combines a 64-slice

CT scanner (Siemens SomatomDefinition AS) with an LSO PET scanner which

incorporates Time of Flight (TOF) reconstruction and has TrueV Option. The

PET component is configured with 32,448 LSO crystals arranged in 4 rings

of 48 detector blocks in a matrix 13

×

13 of 4 mm

×

4 mm

×

20 mm. This

configuration covers an axial field-of-view (FOV) of 21.8 cm correspond-

ing to 109 image planes with a slice thickness of 2 mm. Performance

characteristics of PET component have been evaluated according to NEMA

NU-2 2007 standards by means of Siemens NEMA kit (NEMA PET Self-

Test-mCT) provided with the scanner.

Results:

Preliminary data analysis confirms that the values of measured

major machine parameters (sensitivity, spatial resolution stability, count

rate performance, scatter fraction, image quality) are in agreement with

manufacturer specification.

Conclusions:

In this work we have assessed the performance character-

istics of Biograph mCT PET/CT scanner according to NEMA NU-2 2007

standard test.

Preliminary results confirm the good performance of the system in agree-

ment with recent publications on similar devices.

http://dx.doi.org/10.1016/j.ejmp.2016.01.342

C.337

AUTOMATIC GTV CONTOURING APPLYING ANOMALY DETECTION

ALGORITHM ON DYNAMIC FDG PET IMAGES

C. Bracco

* , a ,

F. Verdoj

a b ,

M. Grangett

o b ,

A. Di Dia

a ,

M. Racca

c ,

T. Varett

o c ,

M. Stas

i a .

a

Medical Physics Department, Candiolo Cancer Institute – FPO- IRCCS,

Candiolo, Italy;

b

Computer Science Department, University of Turin, Turin, Italy;

c

Nuclear Medicine Department, Candiolo Cancer Institute – FPO- IRCCS,

Candiolo, Italy

Introduction:

The aim of this work is to show the results of GTV auto-

matic segmentation based on dynamic PET acquisition. With respect to

single voxel segmentation the temporal information is used to improve

quality of GTV delineation. The segmentation algorithm proposed ex-

ploits the theoretic assumption that FDG uptake over time in cancer cells

is very different from the one in normal tissues and therefore in this

study anomaly detection is used to look for tumor peculiar-anomalous

TACs.

Material and Methods:

For each patient two list mode datasets of images

were acquired. The first one scan (basal) was acquired one hour after FDG

injection and reconstructed as static frame. The last one (delayed) was ac-

quired half one hour after the first scan and reconstructed as dynamic scan.

Two delayed scans were registered to the basal scan. A modified version

of the RX Detector was used. RX Detector usually works in RGB, but in this

study its use on TACs has been explored passing the three grayscale images

in place of the three channels of RGB. The resulting single image, which

actually is a matrix of Mahalanobis distances, presents values that are very

high for voxels whose TAC has anomalous temporal behavior. Finally, thresh-

old segmentation is performed on the distance matrix. On a dataset of 10

patients segmentation techniques present in the literature working on single

PET scan have been implemented as well as segmentation techniques based

on RX Detector output.

Results:

Spatial overlap index (SOI) was used as metric to evaluate the seg-

mentation accuracy. All of the segmentation algorithms implemented on

RXD output show better SOI (0.507

±

0.158) than algorithm based on SUV,

i.e. Brambilla, SOI 0.278

±

0.236. A manual contour drawn by experienced

Nuclear Physician was the reference.

Conclusion:

Although a small dataset, the segmentation of dynamic PET

images based on RXD output seems to be promising.

http://dx.doi.org/10.1016/j.ejmp.2016.01.343

C.338

BREATHING MOTION CORRECTION IN DOSIMETRY OF LIVER LESION

BASED ON 90Y-PET/CT IMAGING

G. Iaccarino, A. Cacciatore

*

, S. Ungania, M. Cazzato, M. D’Andrea,

L. Strigari.

Istituto Nazionale Tumori Regina Elena, Roma, Italy

Introduction:

A degrading factor in quantitative PET imaging is internal

organ motion due to respiration which is a primary cause of image blur-

ring. The aim of this work was to investigate a method to correct PET images

for breathing artifacts in order to improve the dosimetry of liver

radioembolization with 90Y microspheres.

Materials and Method:

PET/CT images were acquired in list mode

modality (LM) with an acquisition time of 30 minutes due to the low

branching ratio of 90Y. The breath curve was constantly monitored

by an external monitor system. The respiratory signal was generated

from a small load cell placed in an elastic belt which was fastened just

below the diaphragm on the patient’s abdomen. The trigger signal sent

by the device to the PET was used to perform the synchronization of

the LM and the respiratory curve. Using a Matlab script, the LM file

was split into sub-files, each corresponding to a different breath ampli-

tude. Images corresponding to each breath amplitude were recon-

structed correcting for scatter, attenuation and system resolution. All

images were finally co-registered to the end-exhale position at which the

CT scan was acquired. Dose distribution was then calculated by convolv-

ing the activity distribution with a Monte Carlo 90Y-kernel. Different volumes

of interest were contoured by gradient and threshold methods and dose

volume histograms were calculated with and without breathing

correction.

Results:

Depending on lesion size and breathing amplitude, the correc-

tion incremented both mean and maximum doses. In the most dramatic

case a patient with an amplitude of about 3.2 cm and a lesion size of 2.7 cm

showed a difference of about 50% in mean dose estimation.

Conclusion:

Our study shows that taking into account organ motion

is mandatory for an accurate dose evaluation. In particular absence of

breathing correction always causes dose underestimation. The magni-

tude of correction strongly depends on lesion size and respiratory

amplitude.

http://dx.doi.org/10.1016/j.ejmp.2016.01.344

C.339

THE IMPACT OF EANM (2013) FORMALISM FOR RADIOIODINE DOSIMETRY

IN HYPERTHYROIDISM DISEASE: A COMPARATIVE EVALUATION OF

THERAPEUTIC ACTIVITY

M. Cacciatori

* , a ,

G. Frigerio

a ,

M. Duchini

a ,

A. Bresolin

b ,

A. Ostinelli

a .

a

Department of Medical Physics, Sant’Anna Hospital, Como, Italy;

b

Physics

Department, University of Milan, Milano, Italy

Introduction:

The treatment of choice in most of hyperthyroidism cases

is the radioiodine therapy. An accurate assessment of the pathological

volume and an individual dosimetry procedure implementation prior to

therapy are mandatory by Council Directive 97/43/Euratom. The aim of this

study is to assess the differences arising in the 131I therapeutic activity

depending on whether the SIE-AIMN-AIFM (2005) or EANM (2013) for-

malism is used.

e99

Abstracts/Physica Medica 32 (2016) e97–e115