2 nd ANNUAL ARDENT WORKSHOP Quality assessment of
![2 nd ANNUAL ARDENT WORKSHOP Quality assessment of hadrontherapy fields with TEPCs Paolo Colautti, 2 nd ANNUAL ARDENT WORKSHOP Quality assessment of hadrontherapy fields with TEPCs Paolo Colautti,](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-1.jpg)
![The radiation quality concept The radiation field quality is meant as a physical measurable The radiation quality concept The radiation field quality is meant as a physical measurable](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-2.jpg)
![Therapeutic beam constrains Fluence rates Proton continuos beam BNCT facility CNAO protons per spill Therapeutic beam constrains Fluence rates Proton continuos beam BNCT facility CNAO protons per spill](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-3.jpg)
![Energy calibration technique in F ~ 1 cm cylindrical TEPCs Tissue-equivalent conductive plastic Vacuum Energy calibration technique in F ~ 1 cm cylindrical TEPCs Tissue-equivalent conductive plastic Vacuum](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-4.jpg)
![Energy calibration technique in F ~ 1 mm cylindrical TEPCs Cathode H. V. a-source Energy calibration technique in F ~ 1 mm cylindrical TEPCs Cathode H. V. a-source](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-5.jpg)
![Measurements at the Nice therapeutic proton beam P. Colautti 2 nd ARDENT workshop. Milano Measurements at the Nice therapeutic proton beam P. Colautti 2 nd ARDENT workshop. Milano](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-6.jpg)
![Insulator surfaces damage without electric-field tubes 75 µm P. Colautti 2 nd ARDENT workshop. Insulator surfaces damage without electric-field tubes 75 µm P. Colautti 2 nd ARDENT workshop.](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-7.jpg)
![Solution: a cavity inside the insulator to switch off the electronic avalanche 0. 9 Solution: a cavity inside the insulator to switch off the electronic avalanche 0. 9](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-8.jpg)
![Mini TEPC of 2. 7 mm of external diameter P. Colautti 2 nd ARDENT Mini TEPC of 2. 7 mm of external diameter P. Colautti 2 nd ARDENT](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-9.jpg)
![Vacuum and gas flow apparatus Pressure readout Exhaust Membrane pump Turbo pump Solenoid valve Vacuum and gas flow apparatus Pressure readout Exhaust Membrane pump Turbo pump Solenoid valve](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-10.jpg)
![Electronic chain Low LET MCA Low LET amplifier Medium LET MCA Medium LET amplifier Electronic chain Low LET MCA Low LET amplifier Medium LET MCA Medium LET amplifier](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-11.jpg)
![Electronic chain P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013 Electronic chain P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-12.jpg)
![Before measuring: linearity checks Integral linearity High LET P. Colautti 2 nd ARDENT workshop. Before measuring: linearity checks Integral linearity High LET P. Colautti 2 nd ARDENT workshop.](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-13.jpg)
![Initial data from the 3 MCA P. Colautti 2 nd ARDENT workshop. Milano 14 Initial data from the 3 MCA P. Colautti 2 nd ARDENT workshop. Milano 14](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-14.jpg)
![Volt calibration P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013 Volt calibration P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-15.jpg)
![Logaritmic compaction Equal log intervals 1 st 2 nd 1 st log yi …. Logaritmic compaction Equal log intervals 1 st 2 nd 1 st log yi ….](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-16.jpg)
![Sub-spectra junction is not feasible if they do not superimpose P. Colautti 2 nd Sub-spectra junction is not feasible if they do not superimpose P. Colautti 2 nd](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-17.jpg)
![The pulse-height frequency distribution P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October The pulse-height frequency distribution P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-18.jpg)
![The pulse-height weighted distribution P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October The pulse-height weighted distribution P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-19.jpg)
![Lineal energy calibration ICRU 49 data 142 ke. V/µm Calibration factor: 142/475 = 0. Lineal energy calibration ICRU 49 data 142 ke. V/µm Calibration factor: 142/475 = 0.](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-20.jpg)
![∆E calculation in CSDA P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October ∆E calculation in CSDA P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-21.jpg)
![Maximum ∆E-lost calculation in CSDA P. Colautti 2 nd ARDENT workshop. Milano 14 -18 Maximum ∆E-lost calculation in CSDA P. Colautti 2 nd ARDENT workshop. Milano 14 -18](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-22.jpg)
![Lineal-energy dose distribution Blue points are used to linearly extrapolate the frequency yvalues down Lineal-energy dose distribution Blue points are used to linearly extrapolate the frequency yvalues down](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-23.jpg)
![Weighting the dose distribution with a biological-significant function The weight is 1 for y-values Weighting the dose distribution with a biological-significant function The weight is 1 for y-values](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-24.jpg)
![Splitting the dose spectrum in its neutron and gamma components P. Colautti 2 nd Splitting the dose spectrum in its neutron and gamma components P. Colautti 2 nd](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-25.jpg)
![Quality of the conjunctive-melanoma proton-therapeutic beam P. Colautti 2 nd ARDENT workshop. Milano 14 Quality of the conjunctive-melanoma proton-therapeutic beam P. Colautti 2 nd ARDENT workshop. Milano 14](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-26.jpg)
![The therapeutic beam quality Iso effective-dose map Iso RBEµ map P. Colautti 2 nd The therapeutic beam quality Iso effective-dose map Iso RBEµ map P. Colautti 2 nd](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-27.jpg)
![Two mini TEPCs for quality measurements of BNCT radiation fields P. Colautti 2 nd Two mini TEPCs for quality measurements of BNCT radiation fields P. Colautti 2 nd](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-28.jpg)
![The twin TEPC for BNCT P. Colautti 2 nd ARDENT workshop. Milano 14 -18 The twin TEPC for BNCT P. Colautti 2 nd ARDENT workshop. Milano 14 -18](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-29.jpg)
![BNCT dose components twin TEPC measurements 30 BNCT dose components twin TEPC measurements 30](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-30.jpg)
![Suggested lectures • Glenn F. Knoll. Radiation Detection and Measurements. John Wiley & Sons, Suggested lectures • Glenn F. Knoll. Radiation Detection and Measurements. John Wiley & Sons,](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-31.jpg)
- Slides: 31
![2 nd ANNUAL ARDENT WORKSHOP Quality assessment of hadrontherapy fields with TEPCs Paolo Colautti 2 nd ANNUAL ARDENT WORKSHOP Quality assessment of hadrontherapy fields with TEPCs Paolo Colautti,](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-1.jpg)
2 nd ANNUAL ARDENT WORKSHOP Quality assessment of hadrontherapy fields with TEPCs Paolo Colautti, INFN 2 nd Annual ARDENT Workshop, Milano, 14 -18 October 2013
![The radiation quality concept The radiation field quality is meant as a physical measurable The radiation quality concept The radiation field quality is meant as a physical measurable](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-2.jpg)
The radiation quality concept The radiation field quality is meant as a physical measurable quantity, which is significant for primary effects on a biological system We define the measured y-spectrum in 12 µm sites as the radiation-field microdosimetric quality Some detectors measure only , which is used as quality mark of the radiation field. The couple of values and is a better quality mark of the radiation field. RBEµ, the microdosimetric assessment of RBE, can be an accurate quality mark for a given biological end-point. P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Therapeutic beam constrains Fluence rates Proton continuos beam BNCT facility CNAO protons per spill Therapeutic beam constrains Fluence rates Proton continuos beam BNCT facility CNAO protons per spill](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-3.jpg)
Therapeutic beam constrains Fluence rates Proton continuos beam BNCT facility CNAO protons per spill CNAO carbon ions per spill 1 cm TEPC ought to measure at counting rates bigger than 106 s-1 1 mm TEPC will measure at counting rates bigger than 104 s-1 P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Energy calibration technique in F 1 cm cylindrical TEPCs Tissueequivalent conductive plastic Vacuum Energy calibration technique in F ~ 1 cm cylindrical TEPCs Tissue-equivalent conductive plastic Vacuum](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-4.jpg)
Energy calibration technique in F ~ 1 cm cylindrical TEPCs Tissue-equivalent conductive plastic Vacuum tide Al cylinder P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Energy calibration technique in F 1 mm cylindrical TEPCs Cathode H V asource Energy calibration technique in F ~ 1 mm cylindrical TEPCs Cathode H. V. a-source](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-5.jpg)
Energy calibration technique in F ~ 1 mm cylindrical TEPCs Cathode H. V. a-source Gas OUT a-source Guard tubes H. V. Gas IN Anode pulse P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Measurements at the Nice therapeutic proton beam P Colautti 2 nd ARDENT workshop Milano Measurements at the Nice therapeutic proton beam P. Colautti 2 nd ARDENT workshop. Milano](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-6.jpg)
Measurements at the Nice therapeutic proton beam P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Insulator surfaces damage without electricfield tubes 75 µm P Colautti 2 nd ARDENT workshop Insulator surfaces damage without electric-field tubes 75 µm P. Colautti 2 nd ARDENT workshop.](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-7.jpg)
Insulator surfaces damage without electric-field tubes 75 µm P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Solution a cavity inside the insulator to switch off the electronic avalanche 0 9 Solution: a cavity inside the insulator to switch off the electronic avalanche 0. 9](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-8.jpg)
Solution: a cavity inside the insulator to switch off the electronic avalanche 0. 9 mm 0. 150 mm 0. 200 mm P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Mini TEPC of 2 7 mm of external diameter P Colautti 2 nd ARDENT Mini TEPC of 2. 7 mm of external diameter P. Colautti 2 nd ARDENT](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-9.jpg)
Mini TEPC of 2. 7 mm of external diameter P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Vacuum and gas flow apparatus Pressure readout Exhaust Membrane pump Turbo pump Solenoid valve Vacuum and gas flow apparatus Pressure readout Exhaust Membrane pump Turbo pump Solenoid valve](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-10.jpg)
Vacuum and gas flow apparatus Pressure readout Exhaust Membrane pump Turbo pump Solenoid valve MFC controller MFC Gas P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Electronic chain Low LET MCA Low LET amplifier Medium LET MCA Medium LET amplifier Electronic chain Low LET MCA Low LET amplifier Medium LET MCA Medium LET amplifier](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-11.jpg)
Electronic chain Low LET MCA Low LET amplifier Medium LET MCA Medium LET amplifier High LET MCA High LET amplifier +18/-6 volt Pulser HVanode HVcathode P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Electronic chain P Colautti 2 nd ARDENT workshop Milano 14 18 October 2013 Electronic chain P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-12.jpg)
Electronic chain P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Before measuring linearity checks Integral linearity High LET P Colautti 2 nd ARDENT workshop Before measuring: linearity checks Integral linearity High LET P. Colautti 2 nd ARDENT workshop.](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-13.jpg)
Before measuring: linearity checks Integral linearity High LET P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Initial data from the 3 MCA P Colautti 2 nd ARDENT workshop Milano 14 Initial data from the 3 MCA P. Colautti 2 nd ARDENT workshop. Milano 14](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-14.jpg)
Initial data from the 3 MCA P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Volt calibration P Colautti 2 nd ARDENT workshop Milano 14 18 October 2013 Volt calibration P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-15.jpg)
Volt calibration P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Logaritmic compaction Equal log intervals 1 st 2 nd 1 st log yi Logaritmic compaction Equal log intervals 1 st 2 nd 1 st log yi ….](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-16.jpg)
Logaritmic compaction Equal log intervals 1 st 2 nd 1 st log yi …. . Bth log yi+1 Example: B = 60 First decade y 1 = 1. 0391, y 2 = 1. 0798, y 3 …. Δ 1 = 0. 04065 Second decade y 1 = 10. 0391, y 2 = 10. 0798, y 3 …. Δ 1 = 0. 4065 Original counts Count density in compacted intervals P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Subspectra junction is not feasible if they do not superimpose P Colautti 2 nd Sub-spectra junction is not feasible if they do not superimpose P. Colautti 2 nd](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-17.jpg)
Sub-spectra junction is not feasible if they do not superimpose P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![The pulseheight frequency distribution P Colautti 2 nd ARDENT workshop Milano 14 18 October The pulse-height frequency distribution P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-18.jpg)
The pulse-height frequency distribution P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![The pulseheight weighted distribution P Colautti 2 nd ARDENT workshop Milano 14 18 October The pulse-height weighted distribution P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-19.jpg)
The pulse-height weighted distribution P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Lineal energy calibration ICRU 49 data 142 ke Vµm Calibration factor 142475 0 Lineal energy calibration ICRU 49 data 142 ke. V/µm Calibration factor: 142/475 = 0.](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-20.jpg)
Lineal energy calibration ICRU 49 data 142 ke. V/µm Calibration factor: 142/475 = 0. 299 P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![E calculation in CSDA P Colautti 2 nd ARDENT workshop Milano 14 18 October ∆E calculation in CSDA P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-21.jpg)
∆E calculation in CSDA P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Maximum Elost calculation in CSDA P Colautti 2 nd ARDENT workshop Milano 14 18 Maximum ∆E-lost calculation in CSDA P. Colautti 2 nd ARDENT workshop. Milano 14 -18](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-22.jpg)
Maximum ∆E-lost calculation in CSDA P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Linealenergy dose distribution Blue points are used to linearly extrapolate the frequency yvalues down Lineal-energy dose distribution Blue points are used to linearly extrapolate the frequency yvalues down](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-23.jpg)
Lineal-energy dose distribution Blue points are used to linearly extrapolate the frequency yvalues down to 0. 01 ke. V/µm Fractional part of the visual area is the fractional contribution to the absorbed dose by the corresponding y -events P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Weighting the dose distribution with a biologicalsignificant function The weight is 1 for yvalues Weighting the dose distribution with a biological-significant function The weight is 1 for y-values](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-24.jpg)
Weighting the dose distribution with a biological-significant function The weight is 1 for y-values < 10 ke. V/µm The weight is < 1 for y-values ≈> 200 ke. V/µm Fractional part of the visual area is the fractional contribution to the effective-dose of corresponding yevents P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Splitting the dose spectrum in its neutron and gamma components P Colautti 2 nd Splitting the dose spectrum in its neutron and gamma components P. Colautti 2 nd](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-25.jpg)
Splitting the dose spectrum in its neutron and gamma components P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Quality of the conjunctivemelanoma protontherapeutic beam P Colautti 2 nd ARDENT workshop Milano 14 Quality of the conjunctive-melanoma proton-therapeutic beam P. Colautti 2 nd ARDENT workshop. Milano 14](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-26.jpg)
Quality of the conjunctive-melanoma proton-therapeutic beam P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![The therapeutic beam quality Iso effectivedose map Iso RBEµ map P Colautti 2 nd The therapeutic beam quality Iso effective-dose map Iso RBEµ map P. Colautti 2 nd](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-27.jpg)
The therapeutic beam quality Iso effective-dose map Iso RBEµ map P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![Two mini TEPCs for quality measurements of BNCT radiation fields P Colautti 2 nd Two mini TEPCs for quality measurements of BNCT radiation fields P. Colautti 2 nd](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-28.jpg)
Two mini TEPCs for quality measurements of BNCT radiation fields P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![The twin TEPC for BNCT P Colautti 2 nd ARDENT workshop Milano 14 18 The twin TEPC for BNCT P. Colautti 2 nd ARDENT workshop. Milano 14 -18](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-29.jpg)
The twin TEPC for BNCT P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
![BNCT dose components twin TEPC measurements 30 BNCT dose components twin TEPC measurements 30](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-30.jpg)
BNCT dose components twin TEPC measurements 30
![Suggested lectures Glenn F Knoll Radiation Detection and Measurements John Wiley Sons Suggested lectures • Glenn F. Knoll. Radiation Detection and Measurements. John Wiley & Sons,](https://slidetodoc.com/presentation_image_h/1c078ab7d8de7048603d3911d255449e/image-31.jpg)
Suggested lectures • Glenn F. Knoll. Radiation Detection and Measurements. John Wiley & Sons, NY, 1979 • ICRU Report 36. Microdosimetry. 1983 P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013
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