Upgrade of the ALPI postaccelerator M Comunian Outline

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Up‐grade of the ALPI post‐accelerator M. Comunian

Up‐grade of the ALPI post‐accelerator M. Comunian

Outline – Present day stable beam facility Overview. – SPES Global Overview. • Transport

Outline – Present day stable beam facility Overview. – SPES Global Overview. • Transport Line from Target to Charge Breeder. • Transport Line to SPES RFQ. • SPES RFQ as new injector for ALPI. – NEW ALPI layout for SPES.

SC Linac with QWRs (Nb, Nb/Cu) at 4, 5 K in 19 cryostats Veq

SC Linac with QWRs (Nb, Nb/Cu) at 4, 5 K in 19 cryostats Veq ~ 48 Me. V/q, beams from 12 C to 197 Au, injected by Tandem or PIAVE (1994) SC Linac ALPI Hall 3 Supernanogan ECR on 350 k. V platform SC-RFQs and QWRs, Veq ~ 8 MV 12 C – 197 Au (higher q and Ibeam) (2006) PIAVE XTU-Tandem 15 MV Vd. G Tandem (HV Corp), H‐ 100 Mo beams, E = 30 ÷ 1. 5 Me. V/A, CW or pulsed (1984) Halls 1 and 2

Operation with Stable Beams 2006‐ 2013 In 2013 -2015 PIAVE and ALPI operation 50%

Operation with Stable Beams 2006‐ 2013 In 2013 -2015 PIAVE and ALPI operation 50% of the time: contributes to 15% of the residual Budget (spare on electricity bill) and concentrates work force on the SPES project.

Representative Stable Beams Available TANDEM INJECTOR PIAVE INJECTOR Progressive development of new PIAVE beams:

Representative Stable Beams Available TANDEM INJECTOR PIAVE INJECTOR Progressive development of new PIAVE beams: in 2013 Mo and Ca (at least 10 pn. A at the experiment; 48 Ca to be tested for min. consumption); Next: Pb, Dy, Pd

SPES Layout 3° Hall Cyclotron ALPI Existing, minor modifications required Existing, major modifications required

SPES Layout 3° Hall Cyclotron ALPI Existing, minor modifications required Existing, major modifications required New PIAVE • ALPI UPGRADE • • • Resonators: low‐beta upgrade and E‐ Upgrade (+2 high‐b cryostats) New quads with higher gradient (20→ 25 T/m) to optimize T RN Beam Diagnostics Cryogenics and cryostats upgrades Vacuum system replacement New controls (RF, diagnostics, magnets, access, vacuum) NEW INJECTOR AND LINES TANDEM • • • New HEBT to Hall III Charge breeder and dedicated 1+ source MR Mass Spectrometer Transport to ALPI (lenses, bunchers, …) New NC RFQ

SPES Layout: zoom on new building HRMS Target To CB From Cyclotron Wien Filter

SPES Layout: zoom on new building HRMS Target To CB From Cyclotron Wien Filter By-Pass Cooler New EXPERIMENTAL HALL 1+

New experimental halls Target New by‐pass Cyclotron Energy of 1+ Ions From 20 k.

New experimental halls Target New by‐pass Cyclotron Energy of 1+ Ions From 20 k. V to 40 k. V Experimental halls

SPES Layout: zoom on 3° hall EXPERIMENTAL HALLS MRMS To RFQ CB From HRMS

SPES Layout: zoom on 3° hall EXPERIMENTAL HALLS MRMS To RFQ CB From HRMS

SPES Layout: zoom on ALPI New CR 21 CR 22 New HEBT to 3°

SPES Layout: zoom on ALPI New CR 21 CR 22 New HEBT to 3° hall Zoomed in in next slide New RFQ injector New Position for PIAVE QWR

SPES Layout: zoom on ALPI low Beta PIAVE QWRs new position 4 m 2

SPES Layout: zoom on ALPI low Beta PIAVE QWRs new position 4 m 2 new bunchers 3. 5 m 4 new triplets From 3° hall reshaping A new buncher is also needed near the PIAVE SRFQ

Line 1+ layout: short triplets and 60° bypass. HRMS CB By‐pass Periodic line Input

Line 1+ layout: short triplets and 60° bypass. HRMS CB By‐pass Periodic line Input used for 1+ Beam from Target to CB: • Mass 132 A • Voltage 42. 857 k. V (equivalent to A/q=7. 5) • Measured Emittance as simulation input • CEA Trace. Win code • Fields Maps for Electrostatic quads and Wien Filter Halls 1+ 90° analizer dipole

Starting beam from Target Phase: ‐ 180 ; 180 Mass: 132 in a. m.

Starting beam from Target Phase: ‐ 180 ; 180 Mass: 132 in a. m. u. Energy: 42. 8 ke. V Gaussian beam in the orthogonal plane and uniform distributed in the longitudinal phase space.

target room 90 deg room bypass periodic structure charge breeder

target room 90 deg room bypass periodic structure charge breeder

90° dipole resolution • New quad slits L. Bellan

90° dipole resolution • New quad slits L. Bellan

HRMS physics design DM=2. 5 10‐ 5 1. 3 mm 3 o order effects

HRMS physics design DM=2. 5 10‐ 5 1. 3 mm 3 o order effects analysis (LNS‐LNL) Input parameters: Energy= 260 Ke. V D =4 mrad DE= ± 1. 3 e. V Emittance=3 p mm mrad Linear Design Mass resolution: 1/40000 (eng. design: 1/25000) Scaled-up version of CARIBU-HRMS, ANL (USA) Typical voltage fluctuation frequency 200 -300 Hz, <<10 k. Hz Electrostatic Plates to correct the voltage ripple of the H. V. platform 20 cm 10 cm See Talk of A. Russo Plates gap 6 cm, ± 750 V to correct ± 5 V platform ripple

ECR‐type Charge Breeder • CB based on ECR technique • Developed by LPSC (LEA‐COLLIGA

ECR‐type Charge Breeder • CB based on ECR technique • Developed by LPSC (LEA‐COLLIGA coll. ) • Design 2013, construction 2014 130 90 74 90 Mass Range 132 ………. . 81 91 138 134 98 94 99 80 82 92 34 ION Q Xe 20+ (21+) Sn 21+ Sr 14+ Kr 16+(18+) Y 14+ Zn 10+ Ga 11+ Rb 17+ Ar 8+(9+) Efficiency [%] 10, 9 (6, 2) 6 3. 5 12(8, 5) 3. 3 2. 8 2 7. 50 16, 2(11, 5) Year Data Source 2012 (2005) 2005 2013 2002 2013 2012 (2013) A. Galata (M/q)_min 6. 57 6. 19 7 5. 22 6. 43 7. 40 7. 36 5. 29 3. 78 (M/q)_max 6. 90 6. 38 7 5. 88 7. 07 8. 00 7. 45 5. 41 4. 25

SPES Layout 3° Hall ALPI PIAVE TANDEM Transport Line from CB to RFQ: the

SPES Layout 3° Hall ALPI PIAVE TANDEM Transport Line from CB to RFQ: the new ALPI injector Cyclotron

Transport Line to SPES RFQ Mass Separator MRMS CB RFQ Magnetic Line with Magnets

Transport Line to SPES RFQ Mass Separator MRMS CB RFQ Magnetic Line with Magnets and Solenoids Tape System Stable ECR ion source 1+ Stable Source

Beam Optics of Transport line from CB to RFQ MRMS Magnetic Line RFQ Losses

Beam Optics of Transport line from CB to RFQ MRMS Magnetic Line RFQ Losses

New RFQ Injector for ALPI • • Energy 5. 7 –> 727. 3 ke.

New RFQ Injector for ALPI • • Energy 5. 7 –> 727. 3 ke. V/A [β=0. 0395] (A/q=7) Beam transmission >95% elong, RMS, out = 0. 15 ns*ke. V/u. L=695 cm (7 modules) Intervane voltage 63. 8 – 85. 8 k. V RF power (four vanes) 100 k. W. Mechanical design and realization, similar to the Spiral 2 one, takes advantage of IFMIF experience (LNL, INFN_Pd, Bo, To) for up to 1 m. A A. Pisent Parameter (units) Design Value Operational mode Frequency (MHz) Injection Energy (ke. V/u) CW 80. 00 5. 7 (β=0. 0035) Output Energy (ke. V/u) 727 (β=0. 0395) Accelerated beam current ( A) 100 Charge states of accelerated ions (Q/A) 7 – 3 Inter‐vane voltage V (k. V, A/q=7) Vane length L (m) Average radius R 0 (mm) Synchronous phase (deg. ) Focusing strength B Peak field (Kilpatrick units) Transmission (%) 63. 8 – 85. 84 6. 95 5. 33 – 6. 788 ‐ 90 – ‐ 20 4. 7 – 4 1. 74 95 Output Long. RMS emittance (mmmrad) / 0. 055 / 0. 15 / 4. 35 (ke. Vns/u)/(ke. Vdeg/u) Mechanical layout of the RFQ tank module (≈1 m)

ALPI Layout for SPES 3° Hall ALPI PIAVE TANDEM Cyclotron

ALPI Layout for SPES 3° Hall ALPI PIAVE TANDEM Cyclotron

ALPI Upgrade foreseen for SPES • • Upgrade on ALPI Layout. Cryogenics and energy

ALPI Upgrade foreseen for SPES • • Upgrade on ALPI Layout. Cryogenics and energy upgrade. New HEBT to 3° Hall. Future Magnets upgrade, (20 ‐> 25 T/m) Diagnostics upgrade. Vacuum system and controls. New Alignment system for all the elements.

SC Resonator Improvements on ALPI LOW‐BETA UPGRADE

SC Resonator Improvements on ALPI LOW‐BETA UPGRADE

Example of stable beams PA‐beams with SPES configuration A/q Ion 3 4 5 6

Example of stable beams PA‐beams with SPES configuration A/q Ion 3 4 5 6 126 Xx 42 126 Xx 31 126 Xx 25 126 Sn 21 Loss es 20% 16% Max. Gradient 20 T/m 17 T/m 20 T/m Field FD 1 1. 043 T 1. 249 T 1. 4146 T 1. 55 T Final Energy (Me. V/A) 20. 8 16. 3 13. 6 11. 7 Fields CRB 4 ‐ 2. 6 MV/m 2. 5 MV/m 1. 3 MV/m

Emax vs A/q graph (at present…) 30 Emax [Me. V/A] 25 12 C 16

Emax vs A/q graph (at present…) 30 Emax [Me. V/A] 25 12 C 16 O 20 32 S 74 Ge 15 N 48 Ca 92 Zr 64 Zn 15 82 Se 84 Kr 120 Sn 10 20 Ne 36 Ar 5 0 90 Zr 93 Nb 02 03 04 58 Ni 197 Au 100 Mo 132 Xe 05 06 A/q 07 08 09

(and with full E‐Upgrade within SPES…) 30 Emax [Me. V/A] 25 12 C 16

(and with full E‐Upgrade within SPES…) 30 Emax [Me. V/A] 25 12 C 16 O At present With ALPI in SPES configuration 32 S 20 74 Ge 15 N 48 Ca 64 Zn 92 Zr 84 Kr 82 Se 15 120 Sn 90 Zr 93 Nb 197 Au 100 Mo 10 20 Ne 36 Ar 5 0 02 03 04 58 Ni 132 Xe 05 06 A/q 07 08 09

SPES case for A/q=7 • • • Input energy from new RFQ: 91. 6

SPES case for A/q=7 • • • Input energy from new RFQ: 91. 6 Me. V (β=0. 0395) = 0. 727 Me. V/A. Output energy from CR 22: 1297 Me. V (β= 0. 148) around 10 Me. V/A. Input Transverse emittance of 0. 1 mmmrad RMS norm. . Global transmission from CB to Experimental Hall: 0. 95 (RFQ)*0. 95(ALPI)=0. 9=90%. Simulation software: Tracewin with full RF fields Maps for cavities. ALPI Input Phase Space ALPI Output Phase Space

Beam Optics from RFQ to Experimental Hall for A/q=7 Max G=20 T/m RFQ Experimental

Beam Optics from RFQ to Experimental Hall for A/q=7 Max G=20 T/m RFQ Experimental Hall 5% Losses B. Chalykh

Magnets Sensitivity analysis Max G=19 T/m Experimental Hall RFQ In addition, an upgrade on

Magnets Sensitivity analysis Max G=19 T/m Experimental Hall RFQ In addition, an upgrade on RF Control is on‐going (M. Bellato) to improve the phase and amplitude precision of ALPI resonators 15% Losses

Energy from SPES Post‐Accelerator as function of A/q Preliminary results from alpi performances with

Energy from SPES Post‐Accelerator as function of A/q Preliminary results from alpi performances with 2 cavities off (margin), Low Beta=5 MV/m, Medium Beta=4. 3 MV/m, High Beta=5. 5 MV/m

Possible A/q as function of Mass PRELIMINARY RESULTS FROM CB PERFORMANCES

Possible A/q as function of Mass PRELIMINARY RESULTS FROM CB PERFORMANCES

RIB Energy as function of Mass PRELIMINARY RESULTS FROM ALPI and CB PERFORMANCES

RIB Energy as function of Mass PRELIMINARY RESULTS FROM ALPI and CB PERFORMANCES

Summary • Dynamics and Physical design: stabilized design and errors study in progress •

Summary • Dynamics and Physical design: stabilized design and errors study in progress • Engineering design of beam line components and RFQ: starting (HRMS and Beam Cooler in R&D phase, pending their funding) • Charge Breeder: construction to be completed at the end of 2014 • ALPI upgrade (cryogenics, new cryomodules, RF systems, diagnostics, new beam line…): on going. People involved on Physical design: M. Comunian L. Bellan B. Chalykh L. Calabretta A. Russo A. Pisent