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Results:

Image noise decreased (up to 50% as compared to FBP) when in-

creasing the percentage of ASIR reconstruction (behavior more relevant for

higher spatial frequencies). Only for low tube load (

<

56 mAs) and lower

contrast objects (with respect to phantom background – i.e. PMP, Delrin,

LDPE and Polystyrene) acquisitions, MTF analysis showed that, increasing

the ASIR percentage, the reconstructed images were characterized by an

appreciable reduction in spatial resolution, when compared to FBP-

reconstructed images.

Conclusion:

When compared to FBP, ASIR allows a relevant noise reduc-

tion without appreciably affecting image quality, except for very low dose

and contrast acquisitions.

http://dx.doi.org/10.1016/j.ejmp.2016.01.244

B.240

DOSIMETRIC AND QUALITATIVE EVALUATION OF CT LONGITUDINAL

AUTOMATIC TUBE CURRENT MODULATION USING IN-HOUSE PHANTOMS

D. Becci

*

, L. Gentile, W. Sartor.

Medical Physics Unit, ASL CN1, Cuneo, Italy

Introduction:

We have developed three different phantom designs to

perform several test methods for the purpose to study automatic tube

current modulation (ATCM) in CT.

Materials and Methods:

The Z-axis dose modulation (Z-DOM without

ACS) present in the routine chest scan protocol of a Philips Brilliance 16

CT scanner was investigated. The first phantom used in this study, Adapted

Body Phantom (ABP), was obtained adapting a standard compact body/

head phantom pulling out half of the head module. ABP presents three

sections: hole, body and head respectively. The second, Recycled Step

Phantom (RSP), comprises three circular sections of different dimensions.

SP has a hole in the center to allow for the insertion of a pencil dose

probe. The third, Funnel Filled Phantom (FFP), was manufactured by filling

a large plastic funnel with water, which was then hermetically sealed.

Point dose measurements were performed for ABP and RSP at the center

in each one of the three different sections that compose both phantoms

using RTI CT Dose Profiler. The dose saving (DSV) was evaluated, with

and without Z-DOM comparing with the same values extracted from

Dicom header. ABP, RSP and FFP were scanned for measurements of noise

(SD of CT number).

Results:

Maximum DSV for ABP, RSP and FFP was respectively 29%, 41% (cal-

culated) and 58% (extracted). The mean noise within images using Z-DOM

is worse than those without. ABP and RSP present a different average noise

among sections changing with set mAs/slice. These differences are less no-

ticeable when we consider total average noise. Also the system almost seems

not to reduce mAs/slice in the Hole section with respect to the Body section

in the ABP. In FFP however the noise remains constant with mAs/slice

set.

Conclusions:

The system shows a real reduction in dose while maintain-

ing an adequate image quality. It seems less adequate in saving dose in

hollow regions scanned.

http://dx.doi.org/10.1016/j.ejmp.2016.01.245

B.241

MONITORING OF DATA OF EXPOSURE OF COMPUTED TOMOGRAPHY

EXAMINATIONS BY ANALYSIS OF RADIATION DOSE STRUCTURED

REPORTS

G. Belli

* , a ,

F. D’Eli

a b ,

A.M. Cimmino

a ,

A.S. Curion

a ,

C. Gasperi

a ,

F. Zenone

a ,

C. Ciccotosto

b .

a

U.O.C. Fisica Sanitaria, AUSL8, Arezzo, Italy;

b

U.O.C.

Radiodiagnostica, AUSL8, Arezzo, Italy

Introduction:

The statistical analysis of the data of exposure is needed to

choose the best strategy to optimize the dose administered to patients.

We present goals that can be achieved with software developed in

house for monitoring the radiation dose indexes in computed tomogra-

phy studies.

Materials and Methods:

In our hospital, 6 MSCT scanners (1

×

64,32,4, 2

×

16 slices) send the Radiation Dose Structured Report (RDSR) together with

images to the PACS.

A program, developed in C

++

, is used for automatic retrieval of the RDSR

on a daily basis, and possibly of a previous period.

Exposure data as kVp, mA, rotation time, beamwidth, pitch, CTDIvol, partial/

cumulative DLP and other descriptive parameters of the studies are

automatically extracted from the RDSR and finally stored in a relational da-

tabase of doses or exported as CSV/HTML formats.

First, controls on the accuracy and consistency of the acquisition settings

in relation to the examination protocols are performed.

Then, the statistical analysis of radiation dose indexes for the most common

examinations it is performed.

For both steps, SQL queries are executed on database.

Results:

They have been retrieved more than 85,000 RDSRs.

Accuracy/consistency tests:

CT 64 slices: beam collimation resulted wrong for all spiral acquisitions;

mA and CTDIvol were recorded erroneously for a study by a factor ten

compared to the true values retrieved from the images.

The cross-analysis between Study Description (SD), Target and IEC CTDI

phantom showed a mismatch for about 20% of the anatomical regions

scanned relying on the exclusive use of the SD.

Optimization of the image–quality dose ratio by changing noise-related ac-

quisition parameters:Analysis of RDSR showed a reduction for CTDI-DLP

(75thpercentiles) of 18%–11% for chest/mdc, 20%–13% for abdomen/mdc.

Conclusions:

Software that allows executing queries on aggregate data from

RDSR can be a useful tool to monitor acquisition protocols and dose index

involved in radiological examinations.

http://dx.doi.org/10.1016/j.ejmp.2016.01.246

B.242

A NOVEL IMAGEJ MACRO FOR CATPHAN LOW CONTRAST MODULE

ANALYSIS: PRELIMINARY RESULTS

M. Biondi

* , a ,

A. Bogi

a ,

L.N. Mazzoni

a ,

E. Vanz

i a ,

G.M. Belmont

e a ,

G. De Ott

o a ,

R. Martini

b ,

S.F. Carbone

c ,

L. Guerrini

a ,

A.E. La Rocca

a ,

D. Guerrieri

c ,

A. Guasti

d ,

F. Banci Buonamici

a .

a

Department of Medical Physics, University

Hospital of Siena, Siena, Italy;

b

Department of Medical, Surgical and

Neurosciences, University of Siena, Siena, Italy;

c

Department of Diagnostic

Imaging, University Hospital of Siena, Siena, Italy;

d

Department of Medical

Physics, U.S.L. 7, Siena, Italy

Introduction:

In the last decades the number CT scans performed per year

has dramatically increased, so that protocol optimization, preferably based

on objective methods for image analysis, is nowadays mandatory. While

for high contrast resolution evaluation MTF could be used, there is not a

commonly accepted method for low contrast resolution evaluation. Catphan

phantoms are widely used in CT quality assurance. In this work an ImageJ

macro for CTP515 low contrast insert quantitative analysis has been

developed.

Material and Methods:

CTP515 module contains 3 groups (contrast level

0.3%, 0.5% and 1%) of 9 cylindrical rods with diameters between 2 and

15 mm. Images were acquired with a CT scanner (GE, Discovery 750 CT),

varying tube voltage (kV

=

100, 120, 140) and noise index (NI

=

8, 12). Each

image was first filtered with the human visual-response function peaked

at four cycles per degree. Choosing a “signal known exactly/background

known exactly” approach ROIs was placed automatically. Test statistics

related to signal and to background were build using 69 images, than a dis-

crimination index d’ related to PC in a 2-AFC was calculated for each detail.

Minimum detectable detail size (MDDS) for each contrast level was evalu-

ated with a fit to the PC values obtained using 75% as threshold. Finally 3

readers scored each image so that macro results could be compared to

human perception.

Results:

Macro results showed that image quality is correlated more with

NI than to kV value. MDDS for automated method were 1.65 mm (1%),

3.4 mm (0.5%) and 4 mm (0.3%). Human observer study showed inter-

reader variability and similar trends were found: MDDS were 3 mm (1%),

5 mm (0.5%) and 7 mm (0.3%).

Conclusions:

The proposed ImageJ macro can be used for low contrast ob-

jective analysis in CT. Thanks to the ease of use and to the wide spread of

Catphan phantom it could be an useful tool in optimization works. Further

works on error estimation and on correlation with human observer results

are needed.

http://dx.doi.org/10.1016/j.ejmp.2016.01.247

e72

Abstracts/Physica Medica 32 (2016) e71–e96