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S442

ESTRO 36 2017

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PO-0830 Quantification of density and tissue changes

in pencil beam scanning proton treatment.

F. Van den Heuvel

1

, F. Fiorini

1

, B. George

1

1

University of Oxford, CRUK/MRC Oxford Institute for

Radiation Oncology, Oxford, United Kingdom

Purpose or Objective

Proton pencil beam scanning (PBS) is becoming the

methodology of choice to deliver proton therapy in many

cases. Several authors have reported discrepancies

between the dose distributions generated by commercial

planning systems, using analytical models, compared to

those using stochastic methods. The differences are

greatest in areas with extensive tissue inhomogeneities.

In analytically based commercial planning systems,

inhomogeneities are taken into account using a water

equivalent path length (WEPL) scaling. In this work we

quantify and investigate the impact of different densities

and tissue on the dose deposition characteristics of a

proton pencil beam.

Material and Methods

A single pencil beam with nominal energy 226 MeV from

an IBA-facility is modeled in homogenous cubic 40x40x40

cm3 phantom using FLUKA. The pencil beam’s dose

deposition is uniquely characterised using a stable

distribution parameterisation, yielding three parameters α

(halo or tail describing parameter), γ (scale parameter)

and ID (integral dose) as a function of depth in the

phantom. Changes of the parameters with changing

densities are investigated and the WEPL technique is

assessed. In addition, the behaviour of the parameters in

a selection of relevant tissues is evaluated.

In addition we investigated different specific media having

different atomic properties and show that an effective

density representation is can be used for these.

Results

The parameters α (Fig 1) describing the scattered

radiation and ID (not shown) clearly scale with the density

of the material. The scaling parameter γ shows a more

complicated behaviour. Indeed, this work shows that an

effective density can be calculated which has the form of

ρ_eff = 1-(1-ρ)/2

Figure 2 shows the difference between both curves. Note

that the maximum of the curves follows the WEPL rule as

they are linked to the position of the bragg peak.

Conclusion

Simple WEPL scaling used in analytical dose calculations

may not correctly model the physical properties of a

proton pencil beam. A more complex scaling framework

that separates the halo and scale parameters could

provide a more accurate representation of dose deposition

from a proton pencil beam. In further work (not shown)

we also show that tissue specific (i.e. stopping power

differences) properties can be handled by using effective

densities.

PO-0831 Multi isocentric 4-pi volumetric modulated arc

therapy approach for head and neck cancer

S. Subramanian

1

, S. Chilukuri

1

, V. Subramani

2

, M.

Kathirvel

1

, G. Arun

1

, S.T. Swamy

1

, K. Subramanian

1

, A.

Fogliata

3

, L. Cozzi

3

1

Yashoda Super Specialty Hospital, Radiation Oncology,

Hyderabad, India

2

All India Institute of Medical Sciences, Radiation