Solution target for cyclotron production of radiometals
US-2017221594-A1 · Aug 3, 2017 · US
US10049778B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10049778-B2 |
| Application number | US-201314428552-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 11, 2013 |
| Priority date | Sep 14, 2012 |
| Publication date | Aug 14, 2018 |
| Grant date | Aug 14, 2018 |
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The invention relates to an arrangement for producing a proton beam. This arrangement is characterized in that it is constituted by a laser driven accelerator of protons adapted to produce a beam of relativistic protons of 0.5 GeV to 1 GeV with a current in the order of tens of mA, such as a current of 20 mA. The invention can be used for transmutating nuclear waste.
Opening claim text (preview).
The invention claimed is: 1. An arrangement for producing a proton beam of relativistic protons of 0.5 GeV to 1 GeV of energy, the arrangement comprising: a proton target, and a laser source focused on the proton target, configured to produce a beam of short pulses at an intensity greater than 10 23 W/cm 2 , the laser source comprising: an ultrashort pulse laser pulse oscillator for producing pulses, and a coherent amplification network system comprising a series of successive amplifier stages, each amplifier stage comprising: a bundle of single mode fiber amplifiers for amplifying the pulses produced by the laser pulse oscillator, each fiber amplifier comprising a plurality of optical fibers, the optical fibers being spaced from one another, and a cooling medium flowing between the fibers, wherein a bundle of one of the successive amplifier stages comprises optical fibers obtained by splitting of optical fibers of a preceding stage, the coherent amplification network system further comprising a downward end portion comprising a last amplifier stage comprising: an amplifying fiber section having optical fibers separated from each other to allow cooling of the optical fibers, and an output bundle section comprising a transport fiber section of a smaller diameter than the amplifying fiber section, comprising optical fibers of a loss lower than that of optical fibers of the amplifying fiber section. 2. The arrangement for producing a proton beam according to claim 1 , wherein the current is about 20 mA. 3. The arrangement for producing a proton beam according to claim 1 , wherein the current is about tens of mA. 4. The arrangement according to claim 1 , wherein a duration of each laser pulse is about 30 femtoseconds. 5. The arrangement according to claim 1 , wherein an average power is about 20 MW. 6. The arrangement according to claim 1 , wherein the proton target is a solid target formed by a film of a substance. 7. The arrangement according to claim 1 , wherein the laser pulse oscillator has a repetition rate of about 10 KHz. 8. An installation for transmutation of nuclear waste, comprising an arrangement for producing a proton beam according to claim 1 , and a spallation target irradiated by the beam of relativistic protons for producing neutrons of 0.5 GeV to 1 GeV of energy by spallation, said neutrons being directed towards the nuclear waste to be transmuted. 9. The installation according to claim 8 , wherein the spallation target is a liquid target. 10. The installation according to claim 9 , wherein the spallation target comprises an entrance window of high-stress steel and a cylindrical tube filled by a liquid of Pb—Bi alloy, wherein said liquid alloy flows and circulates in a dedicated hydraulic circuit to cool the installation. 11. The installation according to claim 8 , wherein a duration of each laser pulse is about 30 femtoseconds. 12. The installation according to claim 8 , wherein an average power is about 20 MW. 13. A method for transmutating nuclear waste, comprising: producing a proton beam, using an arrangement according to claim 1 , irradiating a spallation target with said proton beam so that neutrons of 0.5 GeV to 1 GeV are spallated from said spallation target, directing said neutrons spallated from said spallation target towards said nuclear waste so as to transmute said nuclear waste.
Generating neutron beams (targets for producing nuclear reactions H05H6/00; neutron sources G21G4/02) · CPC title
Parallel arrangements · CPC title
by neutron irradiation · CPC title
Methods or devices for acceleration of charged particles not otherwise provided for {, e.g. wakefield accelerators} · CPC title
by bombardment with electrically charged particles (irradiation devices G21K5/00) · CPC title
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