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Explore evaluation of isotopes injection techniques like Gasses, Ovens, Sputtering, and Charge Breeding for Pandora project on plasma modeling, beam-plasma interaction, and electron dynamics. Detailed study and conclusions presented at Pandora meeting in Bologna.
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IONIZATIONS TECHNIQUES AND PLASMA MODELING A. Galatà on behalf of the PANDORA collaboration PANDORA meeting, Bologna 31/01/2019
TOPICS • Evaluation of isotopes injection techniques: • Gasses • Ovens • Sputtering • Charge Breeding • Considerations for PANDORA • Plasma modeling • The developed numerical code • Beam-plasma interaction • Electron density and temperature distributions • Conclusions Pandora meeting, Bologna 31/01/2019
GASSES • The simplest method • Easy tunability with precise leak valve • In case of «dangerous» gases a gas recovery system could be necessary • Total efficiency close to 50% • Takes advantage of wall recycling Pandora meeting, Bologna 31/01/2019
OVENS • Limited dimensions (φ~ 1-2 cm) • Mounting can be difficult • Possible failures (avoidable with a proper design) • Depending on the temperature to be reached the design changes • Heating up to a vapor pressure of 10-2 mbar (preparation time) • Efficiency ≤ 30% • Uniform contamination of the plasma chamber • Completely decoupled from the plasma LEGIS ion source @ LNL • Due to thermal inertia cannot be switched off immediately. Pandora meeting, Bologna 31/01/2019
SPUTTERING • Once the optimum position is found material emission is immediate • Total efficiency around 10% • The sputtering voltage can perturb the plasma (coupling with the plasma) • When the sputtering voltage is switched off the emission is stopped • It could be necessary to use different gasses depending on the material to be sputtered • Uniform contamination of the plasma chamber Pandora meeting, Bologna 31/01/2019
CHARGE BREEDING • Physical processes in common with ECR sources • Particles injected as a 1+ beam (Deceleration, possible magnetic reflections) • Coulomb collisions lead to thermalization with plasma ions τCB(half life) VCB = +(V + ΔV) kV E1+=1*V keV plasma ΔV<0 ΔV Efficiency(Intenisty) <q+> (energy) Pandora meeting, Bologna 31/01/2019
CHARGE BREEDING: LAYOUT SPES-CB BEAMLINE ECR-BASED CHARGE BREEDER plasma 1+ SOURCES ABLE TO IONIZE ALMOST ALL THE ELEMENTS. CAN BE CONNECTED TO A PRODUCTION TARGET Electrostatic beamline 1+ beam Magnetic selection Pandora meeting, Bologna 31/01/2019
CHARGE BREEDING: RESULTS HEAVY ELEMENTS SPES-CB ACCEPTANDE TESTS Global capture 90% ΔV=-27 V Xe Cs Global capture 65% ΔV~-5 V FREQUENCY TUNING EFFECT Pandora meeting, Bologna 31/01/2019
CHARGE BREEDING: RESULTS LIGHT ELEMENTS LPSC RESULTS PANDORA EXPERIMENT WITH 7lI AT LPSC (11/2017) Global capture 65% ΔV~-5 V • Superposition with N • Low efficiency (<2% on Li3+) • Hydrogen can induce chemical reactions • Vacuum cleanliness is mandatory • Efficiency measured even with ΔV=0 due to the energy spread Courtesy of J. Angot Improvements due to a modified magnetic structure WITH VERY LIGHT ELEMENTS BEAM MANIPULATION (RFQC) IS MANDATORY.NEXT STEPTEST WITH 9BE IN 2020 Pandora meeting, Bologna 31/01/2019
APPLICATION TO PANDORA PANDORA FULL SCALE PANDORA SMALL SCALE • Necessary for short lived isotopes (high activity) • Solves problem of handling • Setup complex (higher costs) • Wide choice of isotopes to analyze • Allow online production (NB or CB targets for 7Be) • Beam manipulation necessary for 7Be and very light species(RFQC) • Suitable for long lived isotopes (low activity) • Simpler setup • Use of conventional techniques SPES-BC Pandora meeting, Bologna 31/01/2019
NUMERICAL MODELING Pandora meeting, Bologna 31/01/2019
THEORY INTERACTION OF AN ION BEAM WITH A PLASMA plasma • Plasma ions following a M-B distribution • Cumulative small angle collisions dominate • Motion deduced from a “test particle” • Thermal equilibrium reached for any initial distribution Slowing down time τs 90° Diffusion time τD Energy equilibrium time τE Pandora meeting, Bologna 31/01/2019
THE NUMERICAL CODE LANGEVIN EQUATION ΔvLang= v(t+1)-v(t)= - νsv(t)*Tstep+vrand 2 1 Friction: a=- νsv Random vectorvrand Distribution of random kicks 3 // v while 1,2 ⊥ v changeateachiteration Calculated for eachparticle from the F-P eq. Pandora meeting, Bologna 31/01/2019
RESULTS BEAM-PLASMA INTERACTION BALLISTIC OF THE PROCESS BECR nhalo nplasmoid ENERGY RELEASED IN THE PLASMA Pandora meeting, Bologna 31/01/2019
RESULTS BEAM-PLASMA INTERACTION 1+ IONS NOT CAPTURED BY THE PLASMA Rb Na CODE VALIDATED BY A COMPARISON WITH EXPERIMENTAL RESULTS FOR HEAVY AND LIGHT IONS, OBTAINED AT LPSC Pandora meeting, Bologna 31/01/2019
RESULTS ELECTRONS DYNAMICS FINE STRUCTURE OF THE DENSITY DISTRIBUTION TEMPERATURE DISTRIBUTION CLOSE TO THE RESONANCE SURFACE Pandora meeting, Bologna 31/01/2019
RESULTS ELECTRONS DYNAMICS SPATIAL DISTRIBUTION OF DIFFERENT ELECTRONS POPULATIONS Pandora meeting, Bologna 31/01/2019
RESULTS Ar FLUORESCENCE LINES Vs SIMULATED WARM ELECTRONS DISTRIBUTION • Argon ions occupy far-from-poles positions:from comparison to simulations it comes out there warm electrons (having enough energy for ionization and excitation) are placed • Next step: comparison of two frequencies EXP. @ ATOMKI Pandora meeting, Bologna 31/01/2019
CONCLUSIONS • During the feasibility study we covered all the aspects involved in the design of the new facility. • A small version of the facility, with reduced costs, will allow first experiments with low activity isotopes. • The full scale version with online production will increase significantly the number of possible experiments. • The know-how necessary to build and operate the two “versions” of the facility is present at the two Laboratories. • A predictive numerical tool able to completely characterize the plasma is available. SO…….LET’S DO IT! Pandora meeting, Bologna 31/01/2019