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Estimation of technical treatment accuracy in fractionated stereotactic radiosurgery

Published online by Cambridge University Press:  29 April 2019

Raj Kishor Bisht*
Affiliation:
Gamma Knife Unit, Department of Neurosurgery, All India Institute of Medical Sciences, New Delhi 110 029, India
Gopishankar Natanasabapathi
Affiliation:
Gamma Knife Unit, Department of Neurosurgery, All India Institute of Medical Sciences, New Delhi 110 029, India
Shashank Sharad Kale
Affiliation:
Gamma Knife Unit, Department of Neurosurgery, All India Institute of Medical Sciences, New Delhi 110 029, India
*
Author for correspondence: Raj Kishor Bisht, Gamma Knife Unit, Department of Neurosurgery, All India Institute of Medical Sciences, New Delhi 110 029, India. Tel: +91 11 26594588. Fax: +91 11 26588927. E-mail: raaj_bisht@rediffmail.com
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Abstract

Aim:

The purpose of this study was to estimate technical treatment accuracy in fractionated stereotactic radiosurgery (fSRS) using the Extend™ system (ES) of Gamma Knife (GK).

Methods and materials:

The fSRS with GK relies on a re-locatable ES where the reference treatment position is estimated using repositioning check tool (RCT). A patient surveillance unit (PSU) monitors the head and neck movement of the patient during treatment and imaging. The quality assurance test of RCT was performed to evaluate a standard error (SE) associated with a measurement tool called digital probe. A ‘4-mm collimator shot’ dose plan for a head–neck phantom was investigated using EBT3 films. CT and MR distortion measurement studies were combined to evaluate SEimaging. The combined uncertainty from all measurements was evaluated using statistical methods, and the resultant treatment accuracy was investigated for the ES.

Results:

Four sets of RCT measurements and 20 observations of associated digital probe showed SERCT of ±0·0186 mm and SEdigital probe of ±0·0002 mm. The mean positional shift of 0·2752 mm (σ = 0·0696 mm) was observed for 20 treatment settings of the phantom. The differences between radiological and predefined isocentres were 0·4650 and 0·4270 mm for two independent experiments. SEimaging and SEdiode  tool were evaluated as ±0·1055 and ±0·0096 mm, respectively. An expanded uncertainty of ±0·2371 mm (at 95% confidence level) was observed with our system.

Conclusions:

The combined result of the positional shift and expanded uncertainty showed close agreement with film investigations.

Information

Type
Original Article
Copyright
© Cambridge University Press 2019 
Figure 0

Figure 1. (a) Mini CT phantom and (b) acquired CT imaging response.

Figure 1

Figure 2. (a) Metal dot marker in the central plane, (b) film positioning with orientation marking, (c) central pin prick on the film for mechanical mean, (d) film adaptor positioning in dosimetric space of the phantom and (e) CT imaging response with metal dot marker.

Figure 2

Table 1. Distance between the dots on MR imaging, MR distortion phantom study

Figure 3

Table 2. Metal marker separation in mini CT phantom for linear distortion

Figure 4

Figure 3. The response of EBT3 films when exposed in head–neck phantom; radiological isocentre precision check with a single 4-mm collimator shot plan for two independent experiments (a) and (b). (a) Experiment 1 and (b) Experiment 2.

Figure 5

Figure 4. (a,b) Density profiles in X-axis and Y-axis and (c,d) density profiles in coronal and sagittal planes using EBT3 films for experiment 1.

Figure 6

Table 3. Calculation of δ with head–neck phantom, where δx, δy and δz are positional shifts along the x, y and z axes, δ1 and δ2 are combined positional shifts along three major axes obtained from film set 1 and film set 2

Figure 7

Table 4. Statistical evaluation of uncertainties, where n is the number of measurements, σ is standard deviation and SE is the standard error