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Table 1 Dosimeter characteristics summary

From: Optical fibre sensors: their role in in vivo dosimetry for prostate cancer radiotherapy

Dosimeter

Advantages

Disadvantages

Characteristics

Thermoluminescence dosimetry (TLD)

Used in Clinical QA dosimetry

Linear from 0.01 Gy to 300 Gy

Can be made small for point dose measurements

Low cost and come in different sizes

Monitors beta, gamma, X-ray and neutron radiations. Corrections for each type are needed

No real time measurement.

Readout time can be consuming

Supralinear from 300 Gy to 1 kGy

TLD devices are re-useable but suffer from sensitivity with repeated use

Dose range: 0.10 mSv–10 Gy

Energy response: Beta (MAX): 0.766 MeV–5 MeV, Photon: 5 keV–6 MeV, Neutron (TLD): Thermal–6 MeV, Neutron (CR39): 200 keV–6 MeV

Plastic Scintillating fibre optic dosimeter

Little energy dependence

Rapid measurement time of around 2 s

Linear from 0.01 Gy to 1 kGy

Small (1 × 1 × 0.2 cm3)

Stable for days

Reusable, re-readable (0.03 % signal loss over 190 readings. Can be optically reset using UV

Supralinear response >2 Gy

Sensitivity to light and temperature during irradiation and readout

Room temperature fading of the OSL signal.

Only two materials are commercially used in OSL

dosimetry:Al2O3:C and BeO

Useful from 0.01 Sv to 100 Sv for X-ray and gamma radiation

Inorganic Scintillating fibre dosimeter

Used in radiotherapy type applications

Can measure small volumes

Long distance transmission,

Immunity to electromagnetic interference

Effects of Cerenkov radiation

Temperature dependent

Used for photon energies above 100 keV

Phosphor coated fibre

Used in radiotherapy and low dose personnel dosimetry applications

Low cost and easy manufacture

High scintillation efficiency

3.23 % variation detected at 90 kV 50 μA

Accuracy of 2 % found under 15 MV 100 MU radiotherapy testing

High radiation exposure (50 Gy to 500 Gy) induces significant permanent attenuation in plastic optical fibres

Range from 50 kV to 15MV X-ray