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S180

ESTRO 36 2017

_______________________________________________________________________________________________

We conducted the neutron measurement under the

collaboration with National Institute of Standards and

Technology (NIST). We employed Bubble detectors (BTI,

Canada) to measure the neutron dose and energy

spectrum with good spatial resolution. The detectors

provide six energy thresholds from 10 keV to 10 MeV

allowing to validate dose and the neutron energy

spectrum. To simulate neutron scatter, a polyethylene

cylindrical phantom was milled and the bubble detectors

were placed inside. The phantom was then irradiated with

a Californium-252 neutron source to simulate the

secondary neutrons. We also simulated the experiment in

TOPAS to compute the neutron dose and energy spectrum

for comparison (Figure 1).

Results

The measured spectrum was unfolded and shows to be in

good agreement with the simulation. On average, the

percent difference in the spectrum was less than 31%

(Graph 1) and the percent difference of dose was under

23%. The agreement was best at the neutron energies 10

keV – 100 keV (19 %) and worst at 2.5-10 MeV (91 %). Better

statistics are needed for the higher energy spectrum

region. We plan to conduct the measurement three times

to minimize statistical errors and plan to extend the

validation to anthropomorphic physical phantoms.

Conclusion

We validated the dose and energy spectrum of scattered

neutrons computed from TOPAS Monte Carlo code by the

measurements using Bubble Detector. We plan to utilize

TOPAS dose calculation system coupled with patient-

specific proton therapy data for normal dose calculations

to support epidemiological studies of proton therapy

patients.

Proffered Papers: Treatment planning applications

OC-0345 Comparing cranio spinal irradiation planning

for photon and proton techniques at 15 European

centers

E. Seravalli

1

, M. Bosman

2

, G. Smyth

3

, C. Alapetite

4

, M.

Christiaens

5

, L. Gandola

6

, B. Hoeben

7

, G. Horan

8

, E.

Koutsouveli

9

, M. Kusters

10

, Y. Lassen

11

, S. Losa

4

, H.

Magelssen

12

, T. Marchant

13

, H. Mandeville

3

, F.

Oldenburger

14

, L. Padovani

15

, C. Paraskevopoulou

16

, B.

Rombi

17

, J. Visser

14

, G. Whitfield

13

, M. Schwarz

17

, A.

Vestergaard

18

, G.O. Janssens

19

1

UMC Utrecht, Department of Radiation Oncology,

Utrecht, The Netherlands

2

University Medical Center Utrecht, Radiotherapy,

Utrecht, The Netherlands

3

The Royal Marsden NHS Foundation Trust, Radiation

Oncology, Sutton, United Kingdom

4

Institute Curie, Radiation oncology, Paris, France

5

West German Proton Therapy Center Essen, Clinic for

Particle Therapy, Essen, Germany

6

Instituto nazionale dei tumori, radiation oncology,

Milano, Italy

7

Radboud university medical center, Department of

Radiation Oncology, Nijmegen, The Netherlands

8

Addenbrooke's Hospital, Radiation Oncology,

Cambridge, United Kingdom

9

Hygeia Hospital, Medical physics department, Athens,

Greece

10

Radboud university medical center, radiation oncology,

Nijmegen, The Netherlands

11

Aarhus University Hospital, radiation oncology, Aarhus,

Denmark

12

Oslo University Hospital, Radiation oncology, Oslo,

Norway

13

The Christie NHS Foundation Trust, Radiation oncology,

Manchester, United Kingdom

14

AMC, radiation oncology, Amsterdam, The Netherlands

15

Timone hospital, radiation oncology, Marseille, France

16

Hygeia Hospital, MEidcal Physics, Athens, Greece

17

Santa Chiara Hospital, Proton therapy Center, Trento,

Italy

18

Aarhus University Hospital, Medical Physics, Aarhus,

Denmark

19

University Medical Center Utrecht, Radiation Oncology,

Utrecht, The Netherlands

Purpose or Objective

The craniospinal irradiation (CSI) is challenging due to the

long target volume and the need of field junctions. The

conventional 3D-CRT technique (two lateral opposed

cranial fields matched to a posterior field) is still widely

adopted. Modern techniques (MT) like IMRT, VMAT,

Tomotherapy and proton pencil beam (PBS) are used in a

limited number of centres.

A multicentre dosimetric analysis of five techniques for CSI

is performed using the same patient, set of delineations

and dose prescription. We aimed to address two questions:

Is the use of 3D-CRT still justifiable in the modern

radiotherapy era? Is one technique superior?

Material and Methods

One 14 year-old patient with medulloblastoma underwent

a CT-simulation in supine position. The CTV and OARs were

delineated in one centre. A margin for PTV was added to

CTV: 5 mm around the brain and spinal levels C1-L2, 8 mm

for levels L3-S3. Fifteen SIOP-E linked institutes, applying

3D-CRT, IMRT, VMAT, Tomotherapy, or PBS (three centres

per technique), were asked to return the best plan

applicable for their technique: high weighting for PTV

coverage (at least 95% of PTV should receive 95% of the

prescribed dose) and low weighting for OAR sparing. Plans

for a prescription dose of 36 Gy were compared within and

between techniques, using a number of dose metrics:

Paddick conformity (range 0-1, with 1 being highly

conformal), and heterogeneity (range 0-1, with 1 being

highly heterogeneous) indices for brain and spine PTVs,

OAR mean doses and non-PTV integral doses.

Results

Conformity- (range 0.75-0.90) and homogeneity (range

0.06-0.08) indices of brain PTV were similar among all

techniques. However for the spinal PTV inferior indices

(CI: 0.30 vs 0.61 HI: 0.18 vs 0.08) are observed for 3D-CRT

with respect to modern techniques (Figure 1). Compared

to more advanced photon techniques, 3D-CRT increased

mean dose to the heart (13Gy vs 8Gy), thyroid (28Gy vs

15Gy), and pancreas (17Gy vs 12Gy) but decreased dose to

both kidneys (4Gy vs 6Gy) and lungs (6Gy vs 8Gy) (Figure

2). PBS reduced the mean dose to the OARs compared to

all photon techniques: a decrease of more than 10Gy was

found for parotid glands, thyroid and pancreas; between

5-10Gy for lenses, submandibular glands, larynx, heart,