Total body irradiation—an attachment free sweeping beam technique
Härtl et al. Radiation Oncology (2016) 11:81
DOI 10.1186/s13014-016-0658-y
RESEARCH
Open Access
Total body irradiation—an attachment free
sweeping beam technique
Petra M. Härtl†, Marius Treutwein*† , Matthias G. Hautmann, Manuel März, Fabian Pohl, Oliver Kölbl
and Barbara Dobler
Abstract
Introduction: A sweeping beam technique for total body irradiation in standard treatment rooms and for standard
linear accelerators (linacs) is introduced, which does not require any accessory attached to the linac. Lung shielding
is facilitated to reduce the risk of pulmonary toxicity. Additionally, the applicability of a commercial radiotherapy
planning system (RTPS) is examined.
Material and Methods: The patient is positioned on a low couch on the floor, the longitudinal axis of the body in
the rotational plane of the linac. Eight arc fields and five additional fixed beams are applied to the patient in supine
and prone position respectively. The dose distributions were measured in a solid water phantom and in an
Alderson phantom. Diode detectors were calibrated for in-vivo dosimetry. The RTPS Oncentra was employed for
calculations of the dose distribution.
Results: For the cranial 120 cm the longitudinal dose profile in a slab phantom measured with ionization chamber
varies between 94 and 107 % of the prescription dose. These values were confirmed by film measurements and
RTPS calculations. The transmittance of the lung shields has been determined as a function of the thickness of the
absorber material. Measurements in an Alderson phantom and in-vivo dosimetry of the first patients match the
calculated dose.
Discussion and conclusion: A treatment technique with clinically good dose distributions has been introduced,
which can be applied with each standard linac and in standard treatment rooms. Dose calculations were performed
with a commercial RTPS and should enable individual dose optimization.
Keywords: Total body irradiation, Sweeping beam technique, Lung shielding, Dosimetry, 3D treatment planning
Background
Total body irradiation (TBI) plays a prominent role especially in the myeloablative conditioning prior to
hematopoietic stem cell transplantation [1]. Many different schemes regarding the total dose, the fractionation
and the dose rate are reported [2, 3]. However, 12 Gy in 6
fractions on 3 days is a very common myeloablative condition scheme [3, 4]. From 1995 to 2013 at our department
different schemes have been applied [5] using a sweeping
beam technique as described by Müller [6]. This technique not only used a gravity oriented shaped filter to
* Correspondence:
†
Equal contributors
Department of Radiotherapy, Regensburg University Medical Center,
Regensburg, Germany
compensate the effects of inverse square variation of the
fluence with distance as it has later been investigated by
Chui et al. [7], but also allowed the application of a set of
lung shields close to the collimator.
The aim of this study was to establish a treatment procedure with similar parameters, when the linacs which
had been employed for this sweeping beam technique
had to be replaced [8, 9]. No accessory should be attached directly to the machine to avoid a certification
process for in-house developed equipment [10]. Lung
shielding should be facilitated to reduce the pulmonary
toxicity [2, 11] as it was possible with the former technique. Abandoning of the gravity oriented accessory was
a precondition to enable the calculation of the dose distribution with a commercial RTPS in clinical routine
[12]. Although the application of a commercial RTPS is
© 2016 The Author(s). Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0
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Härtl et al. Radiation Oncology (2016) 11:81
still quite uncommon in TBI with Linacs, as the technical conditions cannot be modelled for many of the applied techniques, single cases have been reported earlier
[12–15]. In the recent years further adaptions of RTPS
for TBI have been presented [16, 17].
This study presents the measurements required for the
introduction of the new technique and the results of the
in-vivo dosimetry of the first plans.
Methods
Linac, couch and patient positioning
Two linacs of type Elekta Synergy™ with Agility™ head
(Elekta Ltd., Crawley, UK) and photon energies of 6 and
15 MV and electron energies of 6, 8, 10, 12 and 15 MeV
were used for this study. Both linacs have been matched
[18] and conform the requirement of a back-up concept,
guaranteeing the completion of the treatment in time in
case of machine breakdown [11, 19].
The patient is positioned on a low couch on the floor
in supine and prone position, the longitudinal axis in the
rotation plane of the gantry (Fig. 1). The positioning is
supported by a soft mask allowing free air flow in the
prone direction. The couch top is located 117.5 cm
below the isocenter. A plate of Makrolon® polycarbonate
of 10 mm thickness is placed on a stand above the patient to reduce the buildup effect in the patient [11]. The
distance between the couch and the polycarbonate plate
is 33 cm. The plate also serves as tray for the lung
shields. The top of the patient’s head is always 60 cm
from the vertical isocenter plane and is represented by
the longitudinal position l = 0 cm. The dose reference
point was defined on the vertical axis through the isocenter in the middle of the diameter of the patient or
phantom at l = 60 cm. In most cases this is close to the
umbilical transverse plane as a quite common reference
Page 2 of 8
point [19–21]. The position of the feet depends on the
patient’s body length.
The low diameter in the cervical region is partially
compensated in prone and supine positioning by a bolus
of plastic modelling mass.
Treatment fields
The photon beam energy chosen for TBI is 6 MV as rather common [11]. The main dose contribution is given
by rotational fields (arcs) alternating from 310° to 70°
clockwise and reverse. A collimator angle of 90° ensures
a constant field width of 10 cm at the isocenter in the
sweeping direction limited by the solid jaws. The multileaf collimator is set to an opening of 40 cm to exceed
the couch width. A number of eight arcs per patient
position and a dose rate of 300 monitor units (MU) per
minute has been chosen to achieve a low mean lung
dose rate [21] which has been discussed as a parameter
to reduce pulmonary toxicity [20, 22–24]. For the compensation of the effects of inverse square variation of the
fluence with distance, additional fi (...truncated)