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2012 Student Practice in JINR Fields of Research 9.oct.2012. Radioactive ion beam facilities. How does they work ?. I. Sivacek flerovlab.jinr.ru. How to prepare secondary beams ?. Efficiency and selectivity. ISOL systems has advantage in better selectivity - PowerPoint PPT Presentation
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Radioactive ion beam facilities
How does they work ?
2012 Student Practice in JINR Fields of Research 9.oct.2012
I. Sivacek flerovlab.jinr.ru
How to prepare secondary beams ?
Efficiency and selectivity
• ISOL systems has advantage in better selectivity
• Fragment separators have more intensive secondary beams
• Every process has it’s own efficiencyξ = ξDiff ・ ξIon ・ ξSep
I2 = σ Nt Φ ξ
EFFICIENCY IS CRUCIALProper choice of equipment for each experiment is needed !
Secondary beams preparation
• In-flight (10 - 1000 MeV/u, thin target)– Projectile fragmentation (scattering to small
angles, few nucleons lost)• Heavy projectile on light target -> n-rich, mid A• Light projectile on heavy target -> n-def., low A
– Fusion• Cold – 1n channel (GSI Darmstadt)• Hot – 3n, 4n with double-magic 48Ca (JINR Dubna)
• Isotopes with τ ~ μs• Significant emittance
Secondary beams preparation
• ISOL (any target, any projectile)– Fragmentation (protons, heavy ions)– Fission (neutrons, heavy ions)• Variety of mid-A isotopes (light and heavy fragment)
– Spallation (protons)• n-deficient, close to β-stability line
– Fusion (heavy ions)• n-def,. far from β-stability, ~ 5 MeV/u projectiles, selective
• τ > ms• High selectivity, better emittance, up to 60 keV
Thermalization of reaction products
• Thick hot target (ISOLDE) *converter – high Z (W, Ta)
• Hot catcher (MASHA)– Fast release, high diffusion and effusion efficiency (low
effusion materials Ti, V, Zr, Nb, Mo, Hf, Ta, W – ideal for construction materials – Ta heater at MASHA catcher)
• Gas catcher (Gas cell for thermalization of reaction products)
*IGISOL
Target-catcher system is usually not selective
&
MASHA hot catcher
Heavy ionbeam
Target
Hot catcher(graphite)
1TO12, 114
ECR
Heater
Separating foil
4-sector diaphragm for beam diagnostic
2 μm Ti foil
Ion source• IGISOL (ions are evacuated in 1+ or 2+ state)
– Charge state: evacuation time, He purity, e - ion density in gas cell, chemical properties
• Impact ionization (elements Wi > 7 eV)
– Energetic electrons hit neutral atom in el. field• Thermoionization/surface ionizations– X+ (Wi < 7 eV); X- (EA > 1,5 eV) *catcher heater materials
• Laser resonance ionization• Electron cyclotron resonance
Not very selective
Very fast method
Very selective (alkali metals, halogens)
VERY selective
Not very selective, great efficiency
Laser ionization
• Isobaricaly and isomericaly pure secondary beams
• Pulse laser – tunable wavelength
• Competitive de-excitation
• Non resonant high power laser ionization for highly charged ion beams
Electron cyclotron resonance
• Plasma including all electrons and ions• Magnetic field keeps plasma volume• Resonance frequency 2πf = ω = e.B/m for electron
mass m, elementary charge e and magnetic field strength B = 0,0875 T
• 2,45 GHz microwave power – electrons gain energy in resonance
• Impact ionization• C, N, O: ~ 50%; Xe: ~ 90% (only volatile elements)
ECR ion source scheme
Working gas (He)Reaction products
1+ reaction products,1+ working gas
40 kV acceleration
Mass separation• Fragment separators (in-flight)– Light fragments q = Z– Heavy fragments q ≤ Z -> degraders
• Mass separators (ISOL)– Dipole magnet (magnets, or combination with TOF)– The higher angle – the better resolution
Ion optics• Dipole magnets – mass analysis
• Quadrupole lenses – focusation– linear corrections of beam-shape– dispersion changes– linear or 3D ion traps (*mass analysis)
– HF quadrupoles - beam cooling• Sextupoles– 2nd order (nonlinear) corrections of beam spot– wobbler
Detection systems
• Position-sensitive spectrometric “stop detectors”• Time-of-flight systems• Faraday cups for beam diagnostic
• Post acceleration– Linac– Tandem accelerators– Cyclotrones (also used as very precise mass separators)
QUESTIONS !Now is the right time for