2 nd ANNUAL ARDENT WORKSHOP Quality assessment of

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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, 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 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 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 Tissue-equivalent conductive plastic Vacuum

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. a-source

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 14 -18 October 2013

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. 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 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 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 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 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

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. 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 -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

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 …. . 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

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 ARDENT workshop. Milano 14 -18 October 2013

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 2013

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 2013

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. 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 2013

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 October 2013

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 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 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 < 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 ARDENT workshop. Milano 14 -18 October 2013

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 -18 October 2013

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 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 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 October 2013

BNCT dose components twin TEPC measurements 30

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, NY, 1979 • ICRU Report 36. Microdosimetry. 1983 P. Colautti 2 nd ARDENT workshop. Milano 14 -18 October 2013