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S403

ESTRO 36

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Conclusion

Rare-earth doped scintillating silica, thanks to their high

light yield and favorable spectral properties, offer a true

alternative to perform optical fiber dosimetry, in different

clinical and preclinical conditions, eliminating in a reliable

and robust way the influence of the stem effect, without

the need of complex and time-consuming calibrations.

PO-0763 Characterizing the response of Gafchromic

EBT3 film in a 1.5 T magnetic field

Y. Roed

1,2

, H. Lee

2

, L. Pinsky

1

, G. Ibbott

2

1

University of Houston, Physics, Houston, USA

2

The University of Texas MD Anderson Cancer Center,

Radiation Physics, Houston, USA

Purpose or Objective

To assess the influence of a magnetic field (B-field) on the

response of radiochromic film. Irradiation at different

orientations of the film with respect to the B-field was

assessed as well as different durations of exposure of the

films to the B-field.

Material and Methods

EBT3 films were placed at 5 cm depth in an acrylic

phantom and irradiated to 2, 4, and 8 Gy using a cobalt

source while exposed to the B-field from an

electromagnet. The film surfaces were perpendicular to

the incident beam while a reference film edge was

oriented either parallel (RE0) or perpendicular (RE90) to

the B-field. Two B-field strengths of B = 0 T and B = 1.5 T

were used. All films were exposed to the B-field for 7 min.

A subsequent set of films was irradiated to 4 Gy using the

same setup and B = 1.5 T field strength. The films were

exposed to the B-field for 6, 10, or 30 minutes.

All films were scanned with an Epson 10000 XL flatbed

scanner prior to and 24 hours after irradiation, first with

the reference edge parallel (PA) to the scan direction and

then perpendicular (PA90).

Red channel pre- and post-scans were analyzed with

ImageJ software. Percent differences (%diff) with respect

to B = 0 T were calculated for PA and PA90 films. %diff

between PA and PA90 were also determined.

Results

All films exhibited an under-response at each dose level

when compared to irradiation at B = 0 T. Less than -2.0 %

difference was determined in the PA scan direction at all

dose levels for both orientations in the B-field (solid and

dashed black in Figure 1). The under-response increased

with increasing dose for RE90 films scanned in PA90

direction (dashed grey in Figure 1). For RE0 the maximum

%diff was -1.1 % (solid grey in Figure 1).

The %diff in scan direction increased with increasing dose

from 11.0 % to 12.4 % in RE0 orientation and from 9.6 % to

11.1 % in RE90 orientation.

Table 1 shows that increasing the time the films remained

in the B-field resulted in less than 1.0 % over-response for

6 and 30 min and -0.9 % under-response for 7 and 10 min.

The %diff in scan direction was about 12 % for all times.

Conclusion

Radiochromic films can measure doses delivered by a

magnetic resonance-image guided radiotherapy treatment

unit and can be considered for quality assurance of MR-

guided treatment units. The duration of exposure to the

B-field did not affect the response of the film and neither

did the orientation of the reference edge as all

determined %diff were less than the uncertainty of film

measurements. However, the orientation of the reference

edge with respect to scan orientation did have a

significant effect on the response of the film. Maintaining

consistent orientation of films both during the irradiation

in a B-field and also on the flatbed scanner still remains

essential to acquire results with the lowest %diff.

PO-0764 A study of Tandem systems incorporating

three thermoluminescent dosimetry materials.

V. Nelson

1

1

Macarthur Cancer Therapy Centre, Medical Physics,

Campbelltown, Australia

Purpose or Objective

Tandem systems, incorporating a pair of TL materials,

have been shown to be very useful for the determination

of effective energy in radiation beams with unknown

radiation energy spectrum. Tandem curves in all these

tandem systems exhibits maximum TL response ratio

between 40-50 keV and similar TL response ratios on

either side of this energy (E

max

), making it difficult to

determine if the effective energy is less than or greater

than the E

max

(Fig.1(a)). However, if a third TL material,

with energy dependent TL response different to the other

two materials, is included in the tandem, two tandem

curves can be obtained. If these two tandem curves

significantly differ from each other, the effective energy

of the radiation beam can be identified as either less than

or greater than E

max

, Fig. 1(b), hence improving the

dosimetry in this energy range. The aim of this work was

to test a number of different TL materials and find a TL

material which fulfils this criteria.