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Items: 6

1.
Figure 1

Figure 1. From: In vivo real-time rectal wall dosimetry for prostate radiotherapy.

MOSFET detectors placed in the outer lumen of the RadiaDyne rectal balloon

Nicholas Hardcastle, et al. Phys Med Biol. ;55(13):3859-3871.
2.
Figure 6

Figure 6. From: In vivo real-time rectal wall dosimetry for prostate radiotherapy.

A field-by-field comparison of the RTPS calculated and MOSFET measured anterior rectal wall dose for the 3DCRT and IMRT deliveries

Nicholas Hardcastle, et al. Phys Med Biol. ;55(13):3859-3871.
3.
Figure 3

Figure 3. From: In vivo real-time rectal wall dosimetry for prostate radiotherapy.

Angular dependence of the dual MOSFET detector for (a) azimuth and (b) polar axes. The error bars represent two standard deviations of the mean of three measurements.

Nicholas Hardcastle, et al. Phys Med Biol. ;55(13):3859-3871.
4.
Figure 5

Figure 5. From: In vivo real-time rectal wall dosimetry for prostate radiotherapy.

Real-time measured anterior rectal wall dose for (a) 3DCRT plan and (b) IMRT plan. The error bars are the 95% confidence interval of the average of three measurements.

Nicholas Hardcastle, et al. Phys Med Biol. ;55(13):3859-3871.
5.
Figure 2

Figure 2. From: In vivo real-time rectal wall dosimetry for prostate radiotherapy.

(a) Custom made phantom to house the rectal balloon (b) Balloon phantom placed inside the I'mRT phantom and (c) CT slice of the phantom showing the dual MOSFET location relative to the hypothetical prostate (inner contour) and PTV (outer contour)

Nicholas Hardcastle, et al. Phys Med Biol. ;55(13):3859-3871.
6.
Figure 4

Figure 4. From: In vivo real-time rectal wall dosimetry for prostate radiotherapy.

Dual MOSFET dose relative to Ion Chamber measured dose at the centre of the I'mRT phantom for a range of beam angles. The error bars are two standard deviations of the average of three measurements.

Nicholas Hardcastle, et al. Phys Med Biol. ;55(13):3859-3871.

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