BEAM INTENSITIES WITH EURISOL M Valentina Ricciardi GSI

BEAM INTENSITIES WITH EURISOL M. Valentina Ricciardi GSI, Darmstadt, Germany

LAYOUT "Blocks of knowledge" to be put together to estimate RIB intensities: 1) Set-up 2) Production cross-sections 3) Production rates 4) Efficiencies 5) Possible combination of ISOL + IN-FLIGHT methods These "blocks of knowledge" are not uncorrelated. How to proceed? 1. We go through each block and see what we know 2. Provide this information to the user in a simple, accessible way (www)

SET-UP Primary beam Standard option: 1 Ge. V protons: ● on direct target (100 k. W) ● on converter target (4 -5 MW) Additional possibilities (compatible with the baseline driver accelerator): ● 2 Ge. V 3 He ● 250 Me. V deuterons ● heavier ions with A/Q = 2 up to 125 Me. V/u Target Direct target § Protons interact directly with the target material Indirect target § Spallation neutron source (most of the heat load) § Production target (few-Me. V neutrons)

PRODUCTION CROSS SECTIONS Which nuclear reactions are of interest assuming the above set-up? Direct-target option Spallation-evaporation with ≤ 1 Ge. V protons Spallation-fission with ≤ 1 Ge. V protons Fission with secondary neutrons Indirect-target option Fission with few-Me. V neutrons

PRODUCTION CROSS SECTIONS Features of spallation reactions Experimental data taken at the FRS at GSI Evaporation residues Fission fragments IMF (intermediatemass fragments) P. Napolitani J. Taieb, M. Bernas, V. Ricciardi § Spallation-evaporation produces nuclides reaching from the projectile to about 10 to 15 elements below (a few of them are neutron-rich, most of them are neutron-deficient) § Spallation-fission (from Th, U) produces neutron-rich nuclides up to Z=65.

PRODUCTION CROSS SECTIONS Experimental data taken at the FRS at GSI Energy dependence B. Fernandez The region on the chart of the nuclides covered by evaporation residues extends with increasing energy available in the system T. Enqvist Useful to: • Fill gaps in target mass T. Enqvist • Enhance the production of IMF

PRODUCTION CROSS SECTIONS Fission. Model Calculation (ABLA) K. H. Schmidt, A. Kelić

PRODUCTION CROSS SECTIONS Spallation. Model Calculation (ABRABLA)

IN-TARGET PRODUCTION (production rates) Additional things enter into the game: a. Target thickness, material b. secondary projectiles (mostly neutrons) c. decay pattern Important: target material should be feasible! U. Köster

IN-TARGET PRODUCTION (production rates) Residue production in thick-spallation targets (D. Ridikas) J. -C. David et al, Internal report DAPNIA-07 -59, June 2007 Experiment: at Dubna, Pohorecki et al, NIMA 2006 660 Me. V p Calculations: MCNPX 2. 5. 0 + CINDER'90 Fission residue: Evaporation residue: 30. 8 cm nat. Pb

IN-TARGET PRODUCTION (production rates) Optimization of in-target yields: Direct targets Courtesy of S. Chabod Case 183 Hg Optimum target: Pb Optimum energy: 1 Ge. V Optimum target length: ~18 cm? (extraction efficiency)

EFFICIENCIES Specific and precise information on the efficiency, nucleus by nucleus (CERN/ISOLDE) On progress In the meantime, profiting of the valuable database(*) of yields at ISOLDE, a work of Lukić gives an Overview on the overall extraction efficiency (GSI) (*) H. -J. Kluge, Isolde users guide, CERN, Geneva, 1986, web: http: //isolde. cern. ch

EFFICIENCIES Correlation of ISOL yields with isotope half-life § Comparison of ISOLDESC yields to in-target production rates § Ratio yield/produced → overall extraction efficiency for the nuclide S. Lukić et al.

EFFICIENCIES Same general behavior found in many cases. S. Lukić et al.

EFFICIENCIES K. H. Schmidt

EFFICIENCIES K. H. Schmidt Can we extract some general tendency from the measured data? . . . work in progress

TWO-STEP REACTION: ISOL + IN-FLIGHT J. Benlliure et al GSI experiment S 294 (November 2006) What is cold fragmentation Participating institutes: Universidad de Santiago de Compostela, Spain Centre d’Etudes Nucleaires Bordeaux. Gradignan, France Warsow University, Poland GSI Darmstadt, Germany VINCA-Institute Belgrade, Serbia Institute of Physics, Bratislava, Slovakia

TWO-STEP REACTION: ISOL + IN-FLIGHT Two-step schemes: fission + cold fragmentation Production of medium-mass neutron-rich nuclei 2. Use cold fragmentation of 132 Sn to produce medium-A neutron-rich nuclei 1. Produce 132 Sn via fission in uranium target

TWO-STEP REACTION: ISOL + IN-FLIGHT Experimental setup at FRS GSI experiment S 294 (November 2006) S 0 -S 2: 238 U(950 A Me. V) + Be 132 Sn B / ~ 3 10 -4 To. F ~ 72 ps L ~ 18 m Z 2 ~ E A/A ~ 1. 3 10 -3 S 2 -S 4: 124 -132 Sn + Be X B / ~ 3 10 -4 To. F ~ 100 ps L ~ 36 m A/A ~ 1 10 -3

TWO-STEP REACTION: ISOL + IN-FLIGHT Fragmentation of 132 Sn (Preliminary results) Fragmentation of 132 Sn on Be D. Perez and D. Dragosavac Preliminary cross sections are available

TWO-STEP REACTION: ISOL + IN-FLIGHT Energy of the post accelerator Charge state can cause impurity

BEAM-INTANSITY DATA-BASE Courtesy of Wojtek Gawlikowicz, Univ. Warsaw http: //www-w 2 k. gsi. de/eurisol-t 11 http: //www. slcj. uw. edu. pl/~wojtek/eurisol_database. php

CONCLUSIONS • Consistent description of nuclide production • Calculations of in-target yields in progress • Study of the extraction efficiencies in progress • Feasibility of the two-step reaction scheme experimentally proven • EURISOL beam-intensities data-base in progress

Beam intensities with EURISOL DS Task 11 Task leader: Karl-Heinz Schmidt, GSI-Darmstadt Participants and contributors: ISOLDE-CERN, CEA/Saclay, University of Jyväskylä, University of Warsaw, Io. P Bratislava, GSI-Darmstadt, University Santiago de Compostella, Khlopin Radium Institute, VINČA-INS Belgrade