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| facilities:irradiation:trentoprotontherapycenter [09:51 30/05/2022] – [Facility] jhulsman | facilities:irradiation:trentoprotontherapycenter [12:08 01/06/2022] (current) – [Beam Parameters] jhulsman | ||
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| ^ Beam Source ^ Particle Type ^ Flux ($cm^{-2} s^{-1}$) ^ Energy ^ Notes ^ | ^ Beam Source ^ Particle Type ^ Flux ($cm^{-2} s^{-1}$) ^ Energy ^ Notes ^ | ||
| - | | Cylotron (operated by [[ https:// | + | | Cylotron (operated by [[ https:// |
| ===== Facility ===== | ===== Facility ===== | ||
| The Trento Proton Therapy Center (TPTC) is a dedicated facility for treating tumors with protons. The facility is equipped with two rooms: i) for patient treatments and ii) for experimental purposes (physics and/or biophysics). | The Trento Proton Therapy Center (TPTC) is a dedicated facility for treating tumors with protons. The facility is equipped with two rooms: i) for patient treatments and ii) for experimental purposes (physics and/or biophysics). | ||
| - | Protons are supplied by a Cyclotron with an energy of 230 MeV. These are then extracted and focused into a graphite-made energy degrader where the proton energy can be decreased to 60 MeV. The beams can then be redirected into the gantry rooms for patient treatment (offset by $30^{o}$ from the beam line) or into the " | + | Protons are supplied by a Cyclotron with an energy of 230 MeV. These are then extracted and focused into a graphite-made energy degrader where the proton energy can be decreased to 70 MeV. The beams can then be redirected into the gantry rooms for patient treatment (offset by $30^{o}$ from the beam line) or into the " |
| - | {{ : | + | {{ : |
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| + | The beam flux and width depend on the proton energy. Their dependency/ | ||
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| + | ^ Energy (MeV) ^ Average $\sigma$ (mm) ^ Flux (p/s) ^ | ||
| + | | 70.2 | 6.92 | $3.8 \times 10^6$ | | ||
| + | | 100 | 5.68 | $1.2 \times 10^7$ | | ||
| + | | 142.9 | 4.56 |$3.6 \times 10^7$ | | ||
| + | | 169.4 | 4.00 |$7.4 \times 10^7$ | | ||
| + | | 202.4 | 3.48 |$1.4 \times 10^8$ | | ||
| + | | 228.2 | 2.73 |$2.3 \times 10^8$ | | ||
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| + | The correlation between beam profile and flux results from the stopping material which lowers the beam energy. | ||
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| + | ===== Irradiation Configuration ===== | ||
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| + | Three beam configurations are possible: | ||
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| + | - small dual ring ==> circumference of ~3 cm radius with flat intensity profile medium beam intensity | ||
| + | - large dual ring ==> circumference of ~8 cm radius with flat intensity profile low beam intensity | ||
| + | - high beam intensity: direct beam irradiation configuration. Irradiation performed with non uniform intensity beam. The gaussian profile of the beam can be tuned changing the beam energy. | ||
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| + | For the **dual ring** configuration, | ||
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| + | In a ** direct proton beam** irradiation the maximum amount of beam can be delivered on the | ||
| + | target. However, the beam transverse intensity distribution is gaussian instead of uniform. | ||
| + | The gaussian' | ||
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| + | ===== Beam Application ===== | ||
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| + | Since the TPTC is a medical facility the beam in the experimental area is available only at the end of medical treatment, that is from ~19.30 up to 22:30 Mon-Fri, 8-13 on Sat. Formal requests should be done through [[https:// | ||