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S409

ESTRO 36

_______________________________________________________________________________________________

PO-0772 Patient-specific realtime error detection for

VMAT based on transmission detector measurements

M. Pasler

1

, K. Michel

2

, L. Marrazzo

3

, M. Obenland

4

, S.

Pallotta

5

, H. Wirtz

4

, J. Lutterbach

6

1

Lake Constance Radiation Oncology Center, Department

for Medical Physics, Friedrichshafen, Germany

2

Lake Constance Radiation Oncology Center- Martin-

Luther-Universität Halle-Wittenberg, Department for

Medical Physics- Naturwissenschaftliche Fakultät II,

Friedrichshafen, Germany

3

AOU Careggi, Medical Physics Unit, Florence, Italy

4

Lake Constance Radiation Oncology Center, Department

for Medical Physics, Singen, Germany

5

University of Florence- AOU Careggi, Medical Physics

Unit- Department of Biomedical- Experimental and

Clinical Sciences, Florence, Italy

6

Lake Constance Radiation Oncology Center,

Radiooncology, Singen, Germany

Purpose or Objective

To investigate a new transmission detector for online dose

verification. Error detection ability was examined and the

correlation between the changes in detector output signal

with γ passing rate and DVH variations was evaluated.

Material and Methods

The integral quality monitor detector (IQM, iRT Systems

GmbH, Germany) consists of a single large area ionization

chamber which is positioned between the treatment head

and the patient. The ionization chamber has a gradient

along the direction of MLC motion and is thus spatially

sensitive. The detector provides an output for each single

control point (segment-by-segment) and a cumulative

output which is compared with a calculated value.

Signal stability and error detection sensitivity were

investigated. Ten types of errors were induced in clinical

VMAT plans for three treatment sites: head and neck (HN),

prostate (PC) and breast cancer (MC). Treatment plans

were generated with Pinnacle (V.14) for an Elekta synergy

linac (MLCi2). Geometric errors included shifts of one or

both leaf banks for all control points toward (i) and away

(ii) from the central axis of the beam and unidirectional

shifts of both leaf banks (iii) by 1 and 2mm, respectively.

Dosimetric errors were induced by increasing the number

of MUs by 2% and 5%.

Deviations in dose distributions between the original and

error-induced plans were compared in terms of IQM signal

deviation, 2D γ passing rate (2%/2mm and3%/3mm) and

DVH metrics (D

mean

, D

2%

and D

98%

for PTV and OARs).

Results

For segment-by-segment evaluation, calculated and

measured IQM signal differed by 4.7%±5.5%, -2.6%±4.6%

and 4.19%±6.56% for MC, PC und HN plans, respectively.

Concerning the cumulative evaluation, the deviation was

-1.4±0.25%, -6.0±0.3% und -1.47%±0.97%, respectively.

Signal stability for ten successive measurements was

within 0.5% and 2% for the cumulative and the segment-

by-segment analysis.

The IQM system is highly sensitive in detecting geometric

errors down to 1mm MLC bank displacement and

dosimetric errors of 2% if a measured signal is used as

reference. Table 1 reports IQM signal deviations for a

range of introduced errors.

Regarding MLC errors affecting the field size, large

deviations from reference were observed in the IQM

signal, while unidirectional shifts introduced deviations

below detection limit. A similar behavior was observed for

2D γ and DVH parameters. Figure 1 illustrates the

correlation of D

mean

(PTV) and IQM signal deviation,

indicating that clinically relevant errors can be identified.

Conclusion

The deviation between calculated and measured signal is

relatively high, therefore a measurement should be

defined as reference. With this limitation, the system is

not yet capable of treatment plan verification but is a

powerful tool for constancy testing.

The detector provides excellent signal stability and is very

sensitive regarding error detection. The signal deviation

correlates with 2D γ and DVH metric deviations; this

information can be used for identifying action limits for

the IQM.

PO-0773 Three-dimensional radiation dosimetry based

on optically-stimulated luminescence

M. Sadel

1

, E.M. Høye

2

, P. Skyt

2

, L.P. Muren

2

, J.B.B.

Petersen

2

, P. Balling

1

1

Aarhus University, Department of Physics and

Astronomy, Aarhus, Denmark

2

Aarhus University Hospital, Department of Medical

Physic, Aarhus, Denmark

Purpose or Objective

Modern radiotherapy employs complex 3D radiation fields

to deliver therapeutic doses during treatment, and

detailed quality assurance is a prerequisite. Methods

based on luminescent passive detectors, such as optically

stimulated luminescence (OSL), are widely applied,

especially for personal dosimetry and phantom

measurements. Reusability is one advantage of using OSL

for dosimetry; the OSL particles can be reset by

temperature or light-bleaching. Furthermore, the OSL

material used in this study has a wide dynamic range and

linear dose response, and the dosimeter matrix consists of

a flexible material that can be cast into anthropomorphic