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S792

ESTRO 36

_______________________________________________________________________________________________

tests makes it difficult to implement and results out of

tolerance are often left unexplained. Experimental

designs are a robust statistical method which minimizes

the number of tests to be performed and provides a

statistical analysis of the results. They were used to

compare computed and measured doses for several

algorithms.

Material and Methods

Tests were chosen using a Taguchi table L36 (2

11

x3

12

) to

enable the quantification of the influence of each

parameter. Five algorithms were studied: the AAA (version

11, Varian) is used in clinical routine and the collapsed-

cone convolution-superposition (CCCS) algorithm (version

1.5, Mobius Medical Systems) is used as a secondary dose

calculation plan check. The AcurosXB (AXB) algorithm

(version 11, Varian) was also investigated as well the

pencil beam (PB) and Monte Carlo (MC) algorithms

available on Iplan (version 4.5, Brainlab). Absorbed dose

was first calculated in water for 72 beams with varying

parameters: energy, MLC, depth, wedge angle, wedge

jaw, X, Y

1

and Y

2

dimensions. Computations were then

conducted for 72 beams in a CIRS Thorax phantom with

varying parameters: energy, wedge angle, wedge jaw, X

and Y dimensions, medium and gantry angle. Calculated

doses were compared to measurements conducted on a

Novalis TrueBeam STx (Varian) with a CC04 ionisation

chamber (IBA).

Results

In water, all algorithms gave a mean difference between

computed and measured doses centred on zero (within the

uncertainty). No studied parameter led to statistically

significant deviation. In the thorax phantom, the mean

difference between computed and measured doses was -

0.7 ± 1.1 % for AAA, -1.4 ± 1.4 % for CCCS, -2.5 ± 1.0 % for

AXB, 2.3 ± 2.2 % for PB and 0.3 ± 1.9 for MC. For AAA and

CCCS, calculations in bone medium led to a statistically

significant underestimation of the computed dose while

the other parameters had no influence on the results. For

MC, calculated dose was overestimated for gantry angle of

225° which was attributed to the modelization of the

treatment table by the TPS.

Conclusion

Experimental designs were used as a statistical method to

validate the AAA, CCCS and MC algorithms. The PB

algorithm was rejected for clinical use because it

overestimates the dose in heterogeneous medium. Results

showed that the AXB algorithm systematically

underestimates the dose in heterogeneous medium which

could be linked to the dose to water - dose to medium

conversion as referred in the literature. Further

investigation is needed before its implementation in

clinical routine, especially for modulated beams. The tests

described by the experimental designs were also used to

define the tolerance levels of the secondary plan check

software and are now part of the ongoing quality

assurance of the TPS

.

EP-1482 Signal Prediction for an On-line Delivery

Verification System

R. Heaton

1

, M. Farrokhkish

1

, G. Wilson

1

, B. Norrlinger

1

,

D.A. Jaffray

1

, M.K. Islam

1

1

Princess Margaret Cancer Centre University Health

Network, Radiation Physics, Toronto, Canada

Purpose or Objective

Dynamic radiation delivery techniques like VMAT

introduce challenges in treatment verification. Complex

treatments, as well as hypofraction and adaptive radiation

therapy, require new verification approaches to ensure

safe delivered. One approach is the introduction of

entrance fluence monitoring device, like the Integral

Quality Monitoring (IQM) System (iRT Germany), which

provides a spatially encoded dose area product signal as a

unique delivery fingerprint. Complementary to this

measurement is the signal calculation based on the

treatment plan. This work describes the calculation for

the IQM system and examines the impact of selected

components on clinical fields.

Material and Methods

The calculation models the spatial response of the IQM

chamber and the fluence transmitted through the

individual collimating elements. The chamber response is

modelled as a 2D map. The fluence from the machine is

divided into 2 components: a point source at the target

and an extended source at the flattening filter, referred

to as the primary and extended source, respectively. The

primary source is characterized by a radial intensity

profile and is attenuated through the jaws and multileaf

collimator. Transmission is calculated for a 2D array

matching the chamber response map, and area averaged

fluence is calculated for moving collimating elements

during beam delivery. The extended source is modeled as

a Gaussian distributed source with a Compton angular

intensity distribution. The contribution of the Gaussian

source to each element in the fluence array is raytraced

through the collimation to obtain the area averaged

fluence. An element-wise multiplication of the chamber

response map with the primary and extended source

fluence is summed to generate the predicted signal,

modified by factors reflecting the chamber volume, the

intensity of the primary and extended sources and change

in machine output with field aperture. The model has

been implemented for Varian and Elekta treatment units,

with calculations and measurements compared for

clinically relevant fields.

Results

Parameters for the model were determined from a series

of rectangular field measurements with the IQM chamber

combined with ion chamber measurements. Iterative

optimization of parameter values to match rectangular

field IQM measurement were performed. Similar

techniques were used to extract normalization

parameters.

The agreement between the calculated and measured

signals on a Varian TrueBeam unit for over 300 different

IMRT field segments from Prostate and Head & Neck plans

show 99% of segments agree within ±5%; 95% within ±3%.

Similar results were seen for an Elekta Agility unit in a

sample of over 400 different IMRT field segments, with

97% of segments agreeing within ±5% and 91% within

±3%.

Conclusion

A 2-source calculation model has been implemented for an

area-fluence monitor designed for on-line patient QA.

EP-1483 Pre-Treatment QA of MLC plans on a

CyberKnife M6 using a liquid ion chamber array.

L. Masi

1

, R. Doro

1

, O. Blanck

2

, S. Calusi

3

, I. Bonucci

4

, S.

Cipressi

4

, V. Di Cataldo

4

, L. Livi

5

1

IFCA, Medical Physics, Firenze, Italy

2

Saphir Radiosurgery Center, Medical Physics, Frankfurt/

Gustrow, Germany

3

University of Florence, Department of Clinical and

Experimental Biomedical Sciences "Mario Serio", Firenze,

Italy

4

IFCA, Radiation Oncology, Firenze, Italy

5

Azienda Ospedaliera Universitaria Careggi,

Radiotherapy Unit, Firenze, Italy

Purpose or Objective

CyberKnife MLC plans require accurate patient-specific

QA. The purpose of this study is to validate the use of a

liquid ion chamber array for Delivery Quality Assurance

(DQA) of robotic MLC plans, using several test scenarios

and routine patient plans and comparing results to film

dosimetry.