14.20 o8 c gaedtke

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Development and characterisation of a new fibre optic dosimeter C. Gaedtke 1 , G. V. M. Williams 1 , S. G. Raymond 2 , J. Donaldson 3 , L. Greig 3 , and J. Steel 3 Materials: fluoroperovskites Photoluminescence measurements Optically stimulated luminescence Radioluminescence studies Fibre optic dosimeter Characterization of dosimeter 1 SCPS, Victoria University, PO Box 600, Wellington 6140, New Zealand 2 Industrial Research Limited, PO Box 31310, Lower Hutt 5040, New Zealand 3 Blood and Cancer Centre, Wellington Hospital, Private Bag 7902, Wellington, New Zealand

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Research 6: C Gaedtke

Transcript of 14.20 o8 c gaedtke

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Development and characterisation of a new fibre optic dosimeter

C. Gaedtke1, G. V. M. Williams1, S. G. Raymond2, J. Donaldson3, L. Greig3, and J. Steel3

• Materials: fluoroperovskites • Photoluminescence measurements• Optically stimulated luminescence• Radioluminescence studies• Fibre optic dosimeter• Characterization of dosimeter

1 SCPS, Victoria University, PO Box 600, Wellington 6140, New Zealand2 Industrial Research Limited, PO Box 31310, Lower Hutt 5040, New Zealand

3 Blood and Cancer Centre, Wellington Hospital, Private Bag 7902, Wellington, New Zealand

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Materials – Fluoroperovskites • Motivation: Searching for new materials

that have good transparency, high sensitivity, and with a response to radiation that is comparable to that of tissue.

• NaMgF3:Eu2+, NaMgF3:Mn2+, Rb:MgF3:Eu2+, RbCdF3:Mn2+

Zeff = 7.6 for tissue

Zeff = 10.43 for 0.1 % Mn2+ in NaMgF3

Zeff = 12.33 for 0.05 % Eu2+ in NaMgF3

Zeff = 31.5 for 0.2 % Eu2+ in RbMgF3

Zeff characterizes a materials response to low

energy x-rays (α Z4/E3 for photoelectric effect)

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• Transparent polycrystalline samples are made by mixing the starting materials in stoichiometric ratio in a glassy carbon crucible

• samples were heated slightly above the melting temperature and then slow cooling down to below the melting point

Orthorhombic fluoroperovskite structure

Materials – Fluoroperovskites

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Optically stimulated luminescence (OSL) and radioluminescence (RL) measurements

X-irradiation

conduction band

valence band

A+

electronX-rays

A0

(A0)*

hole

F

photostimulated luminescence

photo-stimulation

A0

(A0)*

OSL emissionIrradiation, trapping and RL

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Photoluminescence measurements

8S7/2

6P7/2

6P5/2

4f65d(Eg)

Wav

enum

ber

Q

Eu2+ configurational coordinate diagram in NaMgF3:Eu2+

NaMgF3:Eu2+

PL excitation and emission from NaMgF3: 0.2% Eu2+ bulk material in phosphorescence mode

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Photoluminescence measurements

Eu2+ configurational coordinate diagram in RbMgF3:Eu2+

RbMgF3:Eu2+

PL excitation and emission from RbMgF3: 0.2% Eu2+ in phosphorescence mode

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Photoluminescence measurements

Energy levels of Mn2+ in a crystal field 10Dq

PL excitation and emission in phosphorescence mode

NaMgF3: 1% Mn

RbMgF3: 5% Mn

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Optically stimulated luminescence

OSL measurements of Eu2+ doped samples in phosphorescence mode after 18 hours of irradiation with the 241Am source

RbMgF3: 0.2% Eu2+ NaMgF3: 0.2% Eu2+

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Optically stimulated luminescence

OSL measurements of Eu2+ doped samples in phosphorescence mode after 18 hours of irradiation with the 241Am source

RbMgF3: 5% Mn NaMgF3: 1% Mn

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Radioluminescence

NaMgF3: 1% Mn2+

irradiation over the weekend RbMgF3: 0.2% Mn2+

irradiation overnight

RL measurements of Mn2+ doped bulk materials during irradiation with the 241Am source

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RadioluminescenceRL measurements of Eu2+ doped bulk materials during irradiation with the 241Am source

RbMgF3: 0.2% Eu2+

irradiation overnight NaMgF3: 0.2% Eu2+

irradiation over the weekend

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RadioluminescenceRL measurements of Eu2+ doped nano particles (pressed into small pellets) during irradiation with the 241Am source

NaMgF3: 1% Eu2+

irradiation over the weekend

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Radioluminescence (RL) and optically stimulated luminescence (OSL) measurments

• Real-time radiation dose and dose rate for radiation protection, non-destructive testing, and in medicine for monitoring radiation dose during radiotherapy or for dose verification and validation

• Advantages of OSL dosimeters: • Retains dose information for a long

time• Higher sensitivity than organic

scintillators • Different shape of materials, can be

made as nano particles, bulk transparent polycrystalline materials or 2D sheets

• Can be nearly tissue equivalent

E.G. Yukihara and S.W.S. Mc Keever, „Optically stimulated luminescence (OSL) dosimetry in medicine“, Phys. Med. Biol., 53, R351, (2008)

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Fibre optic dosimeter

Exposure to 10.5 µGy/s 241Am 60 keV γ-rays, then OSL stimulated at 505 nm

We have a patent on the fluoroperovskite materials and a patent application on the device.

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Characterization of the fiber optic dosimeter

• Different fluoroperovskite compounds have been attached to the end of an optical fibre. Tested using the 241Am source at IRL and the linear accelerator at Wellington hospital operating at 6MV

• Second set of measurements involved collaboration with the Wellington Hospital medical physicists

• Can be used in different modes:– Total dose readout: will reset the dosimeter– Latest dose readout: when there is a series of irradiation, readout of each irradiation is

possible– Pulsed dose rate monitoring: IR stimulated pulsed OSL– Continual low dose rate monitoring: RL– Continual high dose monitoring: RL and blue stimulation

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Characterization of the fiber optic dosimeter

Recent RL measurements at Wellington Hospital with the bulk materials

Setup at Wellington Hospital showing the linear accelerator

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Summary

• response to radiation that is comparable to that of tissue• Fluoroperovskites show good PL, OSL and RL response and therefore used

in application • Characterisation in Wellington Hospital showed that bulk materials have a

linear response to dose• Further studies on nano particles as RL signal is dose independent• Characterization of our fluoroperovskites at linear accelerator at

Wellington Hospital