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S414

ESTRO 36

_______________________________________________________________________________________________

Purpose or Objective

PBS, recently developed, scans a tumor with very precise

beam of protons that’s accurate within millimeters,

sparing the healthy surrounding tissues. But it is able to

harmful rather than conventional radiotherapy if the beam

is not accurately irradiated as planned. It is very important

to measure beam width and spot center of the proton

pencil beam for the accurate delivery of dose to the target

volume with a good conformity. We have developed the

beam monitoring system using Array of Fiber-Optic

Cerenkov Radiation Sensor (AFCRS), and conducted

feasibility study for proton pencil beam.

Material and Methods

We have developed a fine segmented detector array to

monitor PBS. A prototype beam monitor system using

AFCRS has been developed for real-time display of the

pencil beam status during the PBS mode operation. The x-

y monitoring system with 128 channel readout is mounted

to the snout for the in-situ real time monitoring. Beam

widths and spot centers of various energies are measured.

Two dimensional Gaussian fit is used to analyze the beam

width and the spot center. The ability of this system to

evaluate Lynx system (Scintillator-based sensor with CCD

camera) and EBT3 for PBS was compared.

Results

The measured Gaussian widths using AFCRS changes from

13 to 5 mm for the beam energies from 100 to 226 MeV.

The beam widths of PBS using the AFCRS are well matched

with the data acquired by a Lynx system and EBT 3 film.

In addition, spot centers for 226 Mev PBS beams are also

well matched with RTP system.

Conclusion

The dosimetric performance of the newly developed

system based on AFCRS was comparable to that of the Lynx

system and EBT3 film. Not only measuring the spot profile

but also monitoring dose map by accumulating each spot

measurement will be available.

PO-0781 A characterisation of EBT3 Gafchromic film for

relative and absolute dosimetry

I. Billas

1

, H. Bouchard

2

, A. Subiel

1

, I. Silvestre

1

, S. Duane

1

1

National Physical Laboratory, Radiation Dosimetry,

Middlesex, United Kingdom

2

Université de Montréal, Département de physique,

Montréal, Canada

Purpose or Objective

The aim of this work is to investigate the variation in dose

response of Gafchromic EBT-3 film within each film and

across films from different boxes and lots. In this way the

uncertainty of relative and absolute dosimetry using EBT-

3 film is quantified and its potential for use in small field

and MRI-guided radiotherapy is better understood.

Material and Methods

Sheets of Gafchromic EBT-3 film were uniformly irradiated

in a cobalt-60 beam in increments of 1 Gy up to a

cumulative dose of 10 Gy. Films were scanned repeatedly

before the first irradiation and after each step. Software

for image processing and analysis was implemented in

MATLAB, allowing determination of the correction for

scanner inhomogeneity and calibration of film optical

density (OD) response in terms of absorbed dose to water.

Regions of interest (ROIs) of various sizes were used to

sample image data, quantifying the uncertainty associated

with variations within each film, from film to film within

the same lot, and from lot to lot. 35 sheets of film were

used, taken from 7 boxes across 3 lots. Three channels of

optical density (OD) data were analysed statistically, both

directly as OD and also in the ratios red/blue and

green/blue. Net values were obtained by subtracting pre-

irradiation values, and a normalisation correction factor,

based on large dose saturation values, was applied.

Results

The figure shows the net ratio of OD, green/blue, before

and after applying the normalisation correction, as a

function of dose, for ROIs which are 10 x 10 mm

2

. The

table lists the relative standard deviation of absorbed dose

measurements made using EBT-3 in the present work.

Conclusion

By combining the subtraction of pre-irradiation values,

with a normalisation correction based on large dose

saturation values, it should be possible to reduce the

contribution to measurement uncertainty arising from

intrinsic variations in the characteristics of EBT-3 film to

0.7 % (

k

=1) for doses in the range of up to 5 Gy.

PO-0782 New liquid ionization chamber detector of

high resolution for treatment verification in

Radiotherapy

L. Brualla-Gonzalez

1

, A. Vázquez-Luque

2

, M. Zapata

3,4

,

D.M. González-Castaño

3,5

, V. Luna-Vega

4

, J. Guiu-Souto

4

,

D. Granero

1

, A. Vicedo

1

, M.T. García-Hernández

1

, J.

Roselló

1,6

, M. Pombar

3,4

, F. Gómez

3,7

, J. Pardo-Montero

3,4

1

Hospital General Universitario de Valencia, Servicio de

Radiofísica ERESA, Valencia, Spain

2

Detection And Radiation Technologies SL, Development,

Santiago de Compostela, Spain

3

Instituto de Investigación Sanitaria IDIS, Grupo de Imaxe

Molecular, Santiago de Compostela, Spain

4

Complexo Hospitalario Universitario de Santiago de

Compostela, Servizo de Radiofísica e Protección

Radiolóxica, Santiago de Compostela, Spain

5

Universidade de Santiago de Compostela, Laboratorio

de Física de Partículas RIAIDT, Santiago de Compostela,

Spain

6

Universidad de Valencia, Departamento de Fisiología de

la Facultad de Medicina, Valencia, Spain

7

Universidade de Santiago de Compostela, Departamento

de Física de Partículas, Santiago de Compostela, Spain

Purpose or Objective

In this work we present a new liquid ionization chamber

array prototype for patient treatment verification. The

objective of its design is to offer a high spatial resolution

with 100% fill factor.

Material and Methods

The prototype has 2041 liquid ionization chambers of

2.5x2.5 mm

2

effective area and 0.5 mm thickness. The

detection elements are arranged in a central square grid

of 43x43, covering an area of 107.5x107.5 mm

2

. The

central inline and crossline are extended to 227 mm and

the diagonals to 321 mm. The active medium is liquid

isooctane.

We have studied short- and medium-term stability, dose

rate dependence, depth and field size dependence,

anisotropy and leaf positioning detectability.

We have measured output factors, tongue-and-groove,

garden fence, small field profiles and irregular fields.

Finally we have used it for the verification of patient

treatments.