Status & Plans for the TRIUMF ISAC Facility

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Status & Plans for the TRIUMF ISAC Facility P.W. Schmor APAC 07, Jan 29-Feb 2 Indore, India

TRIUMF ISAC

Schematic Layout of TRIUMF/ISAC with H- Driver, ISOL Production & Post Accelerators ISAC-II High Energy Experiments ISAC-I High Energy Experiments Driver: Cyclotron H - 500 MeV 100 µa Laser Beams for Resonant Laser Ion Source CSB Low Energy Experiments

Schematic of the ISAC Facility At TRIUMF

BL2A is ISAC beam line

ISOL Method, RIB Yield The yield depends on the following parameters: Y = Φ σ χ ε ε ε, R E i Φ = Proton beam intensity, σ = Cross section, χ = Target thickness, ε = Effusion efficiency, R ε = Diffusion efficiency, E ε = Ionization efficiency. i

30Na 20000 18000 16000 14000 30Na Yield vs Current Detector (CPS) 12000 10000 8000 6000 4000 50 μa Protons Yield Ratemeter 74Rb 2000 0 0 10 20 30 40 50 60 Driver (microamperes) 30Na Measured Yield at 8 pi 74Rb Yield vs Current 6000 5000 Detector (CPS) 4000 3000 2000 1000 RIB Yields are non linear wrt Driver Current 0 0 5 10 15 20 25 Driver (microamperes) Measured Yield at 8pi

ISAC RIB since 1998 Mainly using surface ion source Be, Al, Ga, Ag with TRILIS

Ion Source Operation

Target is made of a 19 mm diameter Ta tube 20 cm long. The transfer tube is EB welded perpendicular to the oven tube. The target material is stacked into the Ta tube. The transfer tube is used for the SIS and LIS. ISAC Target & Thermal Ion Source Target Oven Transfer tube & Hot Surface Ion Source

2500 TFin(K) T FP(K) TBLOCK (K) 0 sheat shields Combined High Power Target Heating (4) High Power Target Normal target design with fins on the target container. 2000 Temperature ( K ) 1500 1000 Ionizer 500 0 0 5 10 15 20 Input Power ( kwatts ) P. Bricault et al., EMIS XIV, Nucl. Instr. Meth.

Initially pressed pellets of oxide material and refractory metal foils were used. The oxides have very low thermal conductivity and the proton beam intensity was restricted to about 5 µa. With carbide compounds higher currents were possible. We were limited to 20 µa on SiC. Currently the carbides are bound onto a graphite foil to remove the heat load more effectively & 70 μa is possible. The same technique with Nb5Si3 on Nb foils is being tested. Refractory foils operated at 50 kw Target Materials Ta Foils SiC on Graphite foil

FEBIAD Operational for 6 weeks at high power Coil Target Cathode Extraction Transfer Tube Anode, GRID Repeller

Resonant Laser ionization 9-14 Be 35μA p + on Ta target on-line dev / yield run (05/2006) Each element has specific atomic levels, The beam purity depends on the number of resonant step one uses, Rydberg or autoionization level probed to improve the Li ioniziation efficiency from a thermal surface ionization source

MISTIC-ECR Ion Source Operational on Ion Source Test Stand

ISAC Accelerators

ISAC-I Accelerator OLIS Stable beams LEBT All-electrostatic (2 kev/u) 11.8 MHz multi-harmonic prebuncher 35 MHz cw RFQ E=2 153 kev/u A/q<=30 MEBT Stripping foil 35 MHz rebuncher 105 MHz cw Variable Energy DTL E=0.15-1.8 MeV/u A/Q<=6 HEBT Diagnostic section 11.8/35 MHz rebunchers

ISAC 35MHz Split-ring RFQ Accelerates ions with A/q<=30 from 2 kev/u to 150 kev/u ISAC 106MHz Separated Function DTL Accelerates ions with A/q<=6 to final energies fully variable from 0.15<E<1.8 MeV/u

ISAC-II (Phase I - Medium Beta Section) Commissioned in 2006 E=4.5 MeV/u A/q=6 S0

ISAC-II Cryogenics Accelerator Vault Refrigerator Room Compressor Room Buffer Tank

2x2x1m stainless steel box vacuum vessel Medium Beta Cryomodule LN2 cooled copper sheet used as thermal shield Mu metal between vacuum tank and LN2 shield Cold mass suspended from lid on three adjustable support pillars Four cavities Ep=30MV/m One SC solenoid @ 9T V eff =4.3MV Single vacuum for thermal insulation and rf Lid Assembly in Assembly Frame

Single Cavity Performance Summary Ep@7W Ep, MV/m 1.00E+10 1.00E+09 1.00E+08 50 40 30 20 10 0 Prototype EZ 01 EZ 02 EZ 03 EZ 04 EZ 05 EZ 06 EZ 07 EZ 08 EZ 09 EZ 10 Qo vs Ea from single cavity tests ISAC-II specifications: Ea=6MV/m P=7W Cavity EZ11 EZ 12 EZ 13 EZ 14 EZ 15 EZ 16 EZ 17 EZ 18 EZ 19 EZ 20 Prototype #1 #2 #3 #4 #5 #6 #7 #8 #9 #10 #11 #12 #13 #14 #15 #16 #17 #18 #19 #20 7W Cavities tested initially in single cavity cryostat Average peak surface field at operating power of 7W is now Ep=38MV/m corresponding to a voltage gain of 1.4MV/cavity and a magnetic field of Bp=75mT and a gradient Ea=7.5MV/m 1.00E+07 0 2 4 6 8 10 12 Ea, MV/m

LINAC Commissioning Floor Layout Diagnostic box Cryomodule TOF detector SCB1 SCB2 SCB3 SCB4 SCB5 Si detector PS Rack Buncher Level 1 power supply room ISAC Beam Beam optics Commissioning Configuration

Energy Measurement Time of Flight (TOF) Medium Beta 9.07m TOF1 TOF2 85nsec

Milestone: Acceleration April 8, 2006 12C3+ Acceleration - May 2, 2006 1 OFF SCB1 SCB1-2 SCB1-3 0.8 SCB1-4 Distribution (AU) 0.6 0.4 SCB1-5 SCB4 SCB3 SCB2 SCB1 Off SCB5 0.2 0 1 2 3 4 5 6 7 E (MeV/u) Energy after each cryomodule for C12(3+) with an injection energy of 1.5Mev/U.

Beam Profile of full energy beam

Acceleration Summary E (MeV/u) 12 10 8 6 4 2 4He2+ 4He1+ 22Ne4+ Commissioning beams A/q=5.5 (22Ne4+) A/q=4 (40Ca10+, 20Ne5+, 12C3+, 4He1+) A/q=2 (4He2+) E (MeV/u) 0 0 2 4 6 8 10 12 14 16 18 20 12 10 8 6 4 2 0 Cavity Energy history during acceleration. 1 2 3 4 5 6 7 8 A/q Expected E final for 6MV/m and actual E final Performance Power @ 7W/cavity Design gradient is 6MV/m Average gradient is 7.2MV/m Final energy is 10.8, 6.8 and 5.5MeV/u for A/q=2, 4, 5.5 respectively Transmission >90%

January 05, 2007 First RIB in ISAC II

Near Term Plans for ISAC I & II Install ISAC II experimental stations & Beamlines TIGRESS, EMMA, Heracles,.. Operation with Actinide Targets Initial tests in 2007 Obtain fission produced neutron rich isotopes Completion of ISAC II Accelerators High Beta cavities planned for 2009 To reach design energy of 6.5 MeV/u for all masses Installation of Charge State Booster in 2008 Heavier masses can be accelerated

Stage 1-2009 E=6.5MeV/u A/q=7 S0 CSB

ISAC Future Plans Beyond ISAC II

ISAC Future Plan The TRIUMF cyclotron driver could provide another proton beam (~ 200-400 µa ) from a presently unused beam line (BL4AN) to new target stations, These target stations would then provide a place to perform systematic development of exotic beams, Ion Source development, Characterization of new targets An additional Radioactive Nuclear Beam could be simultaneously accelerated from these new target stations for experiment

Proposed New Driver Beam New Targets & Simultaneous Post Acceleration

Summary Target & Ion Sources ISAC operates at 100 µa (50 kw) Composite carbide targets on graphite foils operate at the same powers as refractory foils Surface, FEBIAD & resonant laser ion sources are in operation ECR ion source is in testing stage Actinide target capability is planned ISAC II Stage 0 of ISAC II accelerators (medium beta) has operated with RIB First experiment took data in Jan. 2007 (MAYA) using 11 Li A further 20MV of acceleration being prepared for 2009 Concepts are being developed for a dedicated target testing facility & for simultaneous multi user capability