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S505

ESTRO 36 2017

_______________________________________________________________________________________________

Conclusion

For brain metastases stereotactic radiotherapy,

Cyberknife with Iris collimator and VersaHD with ExacTrac

both allowed compliance to dosimetric criteria.

Cyberknife provided higher dose gradients than VersaHD

and limited low dose irradiation of healthy tissues. The

agreement between calculated dose and measured dose

was acceptable for both modalities with mean gamma

values lower than 0.5. An investigation will be performed

to evaluate the use of low margins (1 mm) with the

VersaHD / ExacTrac due to the very low geometric

deviations.

PO-0920 Utilizing monte carlo for log file-based

delivery QA

C. Stanhope

1

, D. Drake

1

, M. Alber

2

, M. Sohn

2

, J. Liang

1

, C.

Habib

1

, D. Yan

1

1

Beaumont Health System, Radiation Oncology, Royal

Oak MI, USA

2

Scientific RT, Munich, Germany

Purpose or Objective

The purpose of this study is to (1) investigate the

feasibility of using Elekta’s R3.2 Log File (LF) Convertor as

a standalone technique for patient-specific QA, and (2)

assess Scientific RT’s SciMoCa monte carlo (MC) algorithm

for use in said system.

Material and Methods

Eleven clinical, dual-arc VMAT patients [9 H&N, 2 low dose

rate brain (35MU/min)] previously planned in Pinnacle and

calculated using Adaptive Convolution (CS) were selected

for this study. Arcs were delivered on Sun Nuclear’s

ArcCHECK (AC) phantom and LF recorded. LF were

converted into dicom plan files and calculated using CS

and MC. For MC, all LF samples were reconstructed with

no increase in calculation time. For CS, plans were

reconstructed using 1° control point spacing to decrease

computational cost. Original (Plan), LF, and AC doses

were compared; statistical distributions (mean ± σ) of

percent diode dose error, as well as 1%/1mm gamma pass

rates, were calculated and compared for the five

comparisons C1 to C5 shown in Table 1. A standard 10%

threshold was utilized for both statistical and gamma

analyses. Dosimetric degradation due to increased control

point spacing (1/2/3/4°) was assessed for CS using

1%/1mm gamma criteria for 4 H&N and 1 brain

patient. Delivering a 25x25 arc at various dose rates (35

to 570 MU/min) diode sensitivity dependence on dose rate

was quantified.

Results

In-field diodes under-responded by 1.5±0.4% at 35 MU/min

compared to 570 MU/min. Consequently, the four brain

fields yielded lower Plan-MC pass rates (44±8%). These

arcs were excluded from subsequent gamma

analysis. Pass rates and diode dose errors are shown in

Table 1. Comparing C2 to C1, MC and CS are

compared. MC resulted in decreased σ values for 17/22

arcs (-3.7 ± 6.5%) and increased passing rates for 10/18

beams (0.4 ± 3.2%). Comparing C4 to C2, log file accuracy

is analyzed for MC. LF resulted in lower σ values for 20/22

arcs (-5.4 ± 3.4%) and improved pass rates for 14/18 arcs

(1.1 ± 1.4%). Comparing C5 to C2, LF and AC QA

techniques are compared. The LF technique yielded

decreased σ values for 22/22 arcs (-51 ± 7%) and improved

pass rates for 18/18 fields (9.9 ± 3.8%). The LF technique

also eliminated systematic AC errors; mean dose errors

decreased from 3.2% to 0.1%. For 1/2/3/4° LF-CS control

point spacing, 1%/1mm pass rates were 80.0 ± 5.0%, 78.0

± 4.2%, 74.0 ± 5.1%, and 68.8 ± 5.3%. Plan-CS pass rates

were 80.2 ± 4.0%. Figure 2 plots difference in pass rates

[(LF-CS vs. AC) minus (Plan-CS vs. AC)] as a function of

control point spacing for each arc. Calculation times for

CS and MC were 12s per control point and 3 minutes per

VMAT arc respectively.

Conclusion

MC doses proved more accurate than CS when compared

to AC measurement. LF-MC plans yielded superior

accuracy and shorter calculation times than LF-CS plans.

By cutting out the phantom and comparing LF dose to that

of the original plan, systematic error was eliminated and

random error greatly reduced.

PO-0921 Dose considerations of IGRT using MV

projection and MV CBCT on a prototype linear

accelerator

P. Balter

1

, T. Netherton

1

, Y. Li

1

, P. Nitsch

1

, S. Gao

1

, M.

Muruganandham

1

, S. Shaitelman-

1

, S. Frank

1

, S. Hahn

1

, A.

Klopp

1

, L. Court

1

1

UT MD Anderson Cancer Center Radiation Physics,

Radiation Physics, Houston- TX, USA

Purpose or Objective

The use of the mega-voltage treatment beam for image-

guided patient setup has some potential advantages over

kV imaging, especially reduced equipment and QA

requirements. One of the challenges that MV imaging

introduces is the increase in daily imaging dose. Here we

investigate (1) whether the MV imaging dose can be

correctly calculated and incorporated into the treatment

plan, and (2) the impact of MV imaging dose on the dose

to normal tissues such as the lung and heart.

Material and Methods

MV imaging dose to the lung, heart and other soft tissue

was measured using an ion chamber in anthropomorphic

thorax phantom (CIRS), and compared with dose

calculated in the TPS (Eclipse) for orthogonal MV-MV

imaging fields and MV CBCT images using a prototype

linear accelerator, each with a low-dose and high-quality

mode (total 4 modes). The impact of the imaging