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Results:

In the evaluation of sensitivity factor no differences were noted

in the values evaluated with the Petri versus point source; while signifi-

cant differences were noted in the values with and without scatter correction.

The sensitivity factors (with Petri dish and with scatter correction) for Tc99m

and I131 were 71.4 and 26.1 counts/MBq s, respectively. The mean SUV values

measured in homogeneous phantoms were 1.08 (4 it, 10 sub) for Tc99m

and 0.75 (2 it, 10 sub) for I131. Recovery coefficient varied from 0.88

(26.5 mL) to 0.27 (1.15 mL) for Tc99m and from 0.53 (26.5 mL) to 0.10

(1.15 mL) for I131.

Conclusion:

Our results suggest that this method can be applied on clin-

ical SPECT-CT and the use of Q.Metrix software permitted us to work more

precisely and with higher repeatability than manually.

http://dx.doi.org/10.1016/j.ejmp.2016.01.355

C.350

QUANTITATIVE 177LU SPECT IMAGING USING ADVANCED CORRECTION

ALGORITHMS IN NON-REFERENCE GEOMETRY

M. D’Arienzo

* , a , b ,

M.L. Cozzella

a ,

A. Fazio

a ,

M. Cazzato

c ,

S. Ungania

c ,

G. Iaccarin

o c ,

M. D’Andrea

c ,

K. Schmidt

d ,

S. Kimiae

i d ,

L. Strigar

i c .

a

ENEA,

National Institute of Ionizing Radiation Metrology, Rome, Italy;

b

Department

of Anatomical, Histological, Forensic Medicine and Orthopedic Sciences, La

Sapienza University, Rome, Italy;

c

Laboratory of Medical Physics and Expert

Systems, Regina Elena National Cancer Institute, Rome, Italy;

d

ABX-CRO

advanced pharmaceutical services Forschungsgesellschaft m.b.H., Blasewitzer

Straße 78-80 D, 01307 Dresden, Germany

Introduction:

Peptide receptor therapy with 177Lu-labelled somatosta-

tin analogues is a promising tool in the management of patients with

inoperable or metastasised neuroendocrine tumours. The aim of this

work was to perform accurate absolute activity quantification of 177Lu in

challenging anthropomorphic geometry using advanced correction

algorithms.

Materials and Methods:

A cylindrical PMMA insert was manufactured and

fixed into the liver of an anthropomorphic phantom to simulate a hepatic

lesion. Measurements at the 208 keV peak were performed with a Philips

IRIX gamma camera using three tumour to background activity concen-

tration ratios (6:1, 9:1, 14:1). Attenuation correction was performed using

μ-maps derived from CT data and co-registered with SPECT images, while

scatter correction was performed using the transmission-dependent con-

volution subtraction method. Both the scatter function and the scatter

fraction were experimentally determined. SPECT acquisitions were cor-

rected for dead time and septal penetration. Recovery coefficients were

evaluated using a NEMA phantom. Image analysis was performed using the

commercially available QSPECT software.

Results:

For all acquisitions, the recovered total activity was within 12%

of the calibrated activity both in the background region and in the tumour.

Using a 6:1 tumour/background ratio the recovered total activity was within

2% in the tumour and within 5% in the background. Because of partial volume

effects, the ability to recover activity in the NEMA phantom depends on

the ROI size. An ROI size as large as the physical radius of the sphere

+

1 cm

margin provided activity values correct to within a few per cent in spheres

with diameter

>

2.2 cm.

Conclusions:

Accurate activity quantification of 177Lu can be obtained in

the clinical practice if activity measurements are performed with equip-

ment traceable to primary standards, advanced correction algorithms are

used and acquisitions are performed at the 208 keV photopeak.

http://dx.doi.org/10.1016/j.ejmp.2016.01.356

C.351

MICROSPHERES THERAPY OF LIVER TUMORS: CALCULATIONS AND

MEASUREMENTS OF ABSORBED DOSES FOR NON-UNIFORM ACTIVITY

DISTRIBUTIONS VIA 90Y-PET/CT IMAGING

M. D’Arienzo

*

, a , b ,

M.L. Cozzella

a ,

M. Tapner

c ,

E. Spezi

d ,

N. Patterson

e ,

P. Chiaramida

f ,

L. Filippi

g ,

A. Fisher

h ,

T. Paulu

s h ,

O. Bagni

g ,

M. Pimpinella

a ,

A.S. Guerr

a a ,

M. Capogni

a .

a

ENEA, National Institute of Ionizing Radiation

Metrology, Rome, Italy;

b

Department of Anatomical, Histological, Forensic

Medicine and Orthopedic Sciences, La Sapienza University, Rome, Italy;

c

Sirtex,

North Sydney, NSW 2060, Australia;

d

Cardiff University, Cardiff, UK;

e

Department of Medical Physics, Velindre Cancer Centre, Cardiff, UK;

f

GE

Healthcare Medical Systems, Milano, Italy;

g

Nuclear Medicine Department,

Santa Maria Goretti Hospital, Latina, Italy;

h

Philips Technologie GmbH

Innovative Technologies, Research Laboratories, Pauwelsstr. 17, 52074 Aachen,

Germany

Introduction:

In recent years there has been an intensifying debate on the

most accurate dosimetric approach for dosimetry in molecular radiother-

apy. The aim of the present work is to evaluate the absorbed dose to lesions

from 90Y-PET images using different calculation algorithms including: (I)

Direct Monte Carlo (MC) using Raydose; (II) Kernel-convolution using Philips

Stratos; (III) Local deposition; (IV) MCNP, assuming uniform activity dis-

tribution; and (V) MIRD approach. Absorbed doses calculated using MC codes

were compared with those obtained performing measurements with

LiF:Mg,Cu,P TLDs inside a cylindrical phantom filled with a homogenous

90YCl solution.

Materials and Methods:

An anthropomorphic phantom was used in the

present study. A home-made cylindrical PMMA insert was manufactured

and fixed into the liver cavity to simulate a hepatic lesion. Measurements

in anthropomorphic geometry were performed using a GE Discovery ST PET/

CT scanner with a 6:1 tumor to background activity concentration ratio.

The first scan was performed with an activity concentration of 5.5 MBq/

mL for the lesion insert and 0.89 MBq/mL for the liver background. The

anthropomorphic phantom was then acquired at days 4, 5, 6 and 12 down

to an activity concentration of 0.31 MBq/mL for the lesion insert and 50 kBq/

mL for the liver background.

Results:

All dose algorithms provided acceptable results, the worst case

scenario providing an agreement between absorbed dose evaluations within

20%. Measured doses were consistent with absorbed doses calculated using

full MC techniques with an agreement within 3%, well within the stated

uncertainties.

Conclusions:

Although all dose calculation algorithms provided compa-

rable average dose values, heterogeneous activity distributions were obtained

from 90Y-PET data, where a uniform activity distribution was supposed to

be. Additional work is needed toward the development of specific 90Y-

PET reconstruction protocols to allow proper image quantification for

dosimetry.

http://dx.doi.org/10.1016/j.ejmp.2016.01.357

C.352

INTERNAL DOSE ASSESSMENT IN MOLECULAR RADIOTHERAPY: TIME FOR

AN AGREED DOSIMETRY PROTOCOL?

M. D’Arienzo

*

, a , b ,

M. Capogni

a ,

V. Smyth

c ,

M. Cox

c ,

L. Johansson

c ,

A. Fenwick

c ,

J. Solc

d ,

C. Bobin

e ,

H. Rabus

f ,

L. Joulaeizadeh

g .

a

National

Institute of Ionizing Radiation Metrology, ENEA-INMRI, C.R. Casaccia, Rome,

Italy;

b

Department of Anatomical, Histological, Forensic Medicine and

Orthopedic Sciences, La Sapienza University, Rome, Italy;

c

National Physical

Laboratory (NPL), Hampton Road, Teddington, Middlesex, TW11 0LW London,

UK;

d

Czech Metrology Institute (CMI), Inspectorate for Ionising Radiation,

Radiova 1, CZ-102 00 Prague, Czech Republic;

e

Commissariat a l’Energie

Atomique (CEA) Bt 476, Pt Courrier 142, CEA-Saclay, FR-91191 Gif-sur-Yvette

Cedex, Paris, France;

f

Physikalisch-Technische Bundesanstalt (PTB), Bundesallee

100, D-38116 Braunschweig, Germany;

g

VSL, Dutch Metrology Institute,

Thijsseweg 11, P.O. Box 654, NL-2629 JA Delft, The Netherlands

Introduction:

Molecular radiotherapy (MRT) is conventionally pre-

scribed on the basis of administered activity. The major drawback is that

uptake and retention differ appreciably from patient to patient and so the

absorbed dose to the target can vary significantly between patients for the

same administered activity.

Material and Methods:

Despite the growing trend toward developing

patient-specific dosimetry models based on quantitative data, progress in

this area has been hindered by the lack of (a) appropriate standards for cali-

brating the imaging systems and (b) a clinically accepted dosimetry protocol.

Consequently, it is generally accepted that quantitative imaging (QI) and

dosimetry in MRT suffer from considerable inaccuracy.

Results:

By analogy with external beam radiotherapy, the EMRP MetroMRT

project addressed these issues by formulating MRT dosimetry as a mea-

surement chain traceable to primary standards with known uncertainty:

(I) measurement of administered activity, (II) measurement of activity within

e103

Abstracts/Physica Medica 32 (2016) e97–e115