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S681

ESTRO 36

_______________________________________________________________________________________________

energy of the Cobalt source compared to those of clinical

X-ray beam lead to increase of the surface dose.

A previous study (SIMBAD 01) investigated the feasibility

of comparative planning among different radiotherapy

technologies (i.e: IMRT vs VMAT vs MRI-

60

Co) optimizing for

target coverage and organs at risk sparing. Hardware and

software implementation on MRIdian will be completed at

our institution within February 2017. Experimental

measurements are planned when the system will become

clinically operative. Aim of the present analysis is to

quantify the dose delivered to subcutaneous tissues in the

SIMBAD 01 planning conditions (without specific

optimization for subcutaneous tissues).

Material and Methods

Ten patients affected by locally advanced rectal cancer

(LARC) were included in this study. For each patient a

VMAT RapidArc, a 5-beams sliding window IMRT and one

MRIdian treatment plan were performed.

All treatment plans were calculated according to the

Quality Assurance protocols adopted in our Institution: the

PTV1 was represented by tumor and corresponding

mesorectum; the PTV2 by mesorectum in toto and pelvic

nodes. Isotropic 0.7 cm margins were added to PTVs. The

total prescribed dose for PTV1 was 55 Gy and 45 Gy for

PTV2 through Simultaneous Integrated Boost.

All plans were optimized for PTV coverage and sparing of

bowel bag and bladder.PTV coverage was evaluated by

calculating the V95 and V105 values. For bowel bag V45

and for bladder the mean dose was considered.

The presence of magnetic field has been taken into

account during MRIdian MRI-

60

Co planning procedures..

The evaluation of subcutaneous skin dose was obtained

calculating the median dose in a 5 mm wide ring dummy

structure contoured 3 to 8 mm far from body surface.

The first 3 mm from body surface were not taken into

account to avoid inconsistencies related to uncertainties

in dose calculation at air-body interface due to different

dose calculation algorithms (AAA Collapse Cone for VMAT

and IMRT treatments, Montecarlo for MRIdian TPS).

Results

All plans optimized for this study satisfied the constraints

on PTV coverage and organs at risk sparing. Dosimetric

values obtained in this planning comparison are listed in

table 1.

The median skin dose resulted higher using the MRIdian

system (1.97 Gy against 1 Gy for IMRT and 0.98 Gy for

VMAT)

Conclusion

A subcutaneous skin dose increase is observed with the

employment of MRI-

60

Co RT when compared to LINAC

treatment planning, even if still in clinically acceptable

constraints. Considering and contouring such a structure

seems useful. Specific study will be performed to define

how reducing dose to subcutaneous tissues by optimizing

for

such

structures.

EP-1267 In silico Evaluation of the impact of Magnetic

Field on dose distribution using of MRIdian MRI- 60Co

D. Cusumano

1

, L. Boldrini

2

, L. Azario

3

, S. Teodoli

1

, M.

Balducci

4

, G.C. Mattiucci

4

, S. Chiesa

2

, G. Chiloiro

2

, N.

Dinapoli

2

, M.A. Gambacorta

4

, C. Masciocchi

5

, D. Piccari

6

,

M. Rapisarda

6

, M.V. Antonelli

6

, M. Ferro

2

, E. Placidi

1

, A.

Piermattei

3

, F. Cellini

2

, V. Valentini

4

1

Fondazione Policlinico A. Gemelli, UOC Fisica Sanitaria -

Gemelli ART - Radiation Oncology, Rome, Italy

2

Fondazione Policlinico A. Gemelli, Gemelli ART -

Radiation Oncology, Rome, Italy

3

Università Cattolica del Sacro Cuore, Rome, Italy

4

Università Cattolica del Sacro Cuore, Gemelli ART -

Radiation Oncology, Rome, Italy

5

Fondazione Policlinico A. Gemelli, KBO Labs - Gemelli

ART - Radiation Oncology, Rome, Italy

6

Fondazione Policlinico A. Gemelli, TSRM - Gemelli ART -

Radiation Oncology, Rome, Italy

Purpose or Objective

The MRIdian MRI

60

Co radiotherapy system (ViewRay,

Oakwood, Ohio) combines an open split-solenoid MRI

scanner equipped for parallel imaging and three

60

Co

gamma-ray sources.

The quantification of dose distribution perturbations due

to the presence of 0.35 T magnetic field represents an

issue.

The MRIdian TPS is equipped by two Montecarlo based

algorithms to calculate the dose distribution: the first one

has faster calculation time; and does not account for the

presence of magnetic field (B

off

). The second one has

slower calculation time; and takes into account for the

presence of magnetic field (B

on

). Hardware and software

implementation on MRIdian will be completed at our

institution within February 2017. Experimental

measurements are planned when the system will become

clinically operative.

Aim of this study was to compare the two algorithms in

order to evaluate which could be more accurate in an

in

silico

treatment planning study designed for locally

advanced rectal cancer (LARC).

Material and Methods

This study includes 7 cases of patients affected by LARC.

For each patient of the study two plans were developed.

Same priority values for the optimization were applied.

The calculation of dose distribution was performed using

the two different algorithms object of this study (B

off

and

B

on

).

Plans were performed in IMRT modality, adopting same

beams geometry consisting in one pseudo-arc composed

by three beam triplets.

The treatment plans were optimized according to usual

Quality Assurance protocols adopted in our Institution for

Linac IMRT treatments: the PTV1 was represented by

tumor and corresponding mesorectum; the PTV2 by

mesorectum in toto and pelvic nodes. Isotropic 0.7 cm

margins were added to PTVs. The total prescribed dose for

PTV1 was 55 Gy and 45 Gy for PTV2 through Simultaneous

Integrated Boost.

All plans were optimized for PTV coverage and sparing of

bowel bag and bladder. For PTVs coverage V95 and V105

were considered. For bowel bag V45 and for bladder the

mean dose were considered, respectively. Plans were

normalized at target median.

Results

Table 1 summarizes the median values for PTV coverage

and organs at risk sparing obtained in the two cases. No

significant differences have been reported between the

two algorithms.