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Indian Activities under IIFC Pitamber Singh Head, Ion Accelerator - PowerPoint PPT Presentation

Indian Activities under IIFC Pitamber Singh Head, Ion Accelerator Development Division Bhabha Atomic Research Centre, Mumbai Presentation on behalf of 1. Bhabha Atomic Research Centre, Mumbai 2. Raja Ramanna Centre for Advanced Technology,


  1. Indian Activities under IIFC Pitamber Singh Head, Ion Accelerator Development Division Bhabha Atomic Research Centre, Mumbai Presentation on behalf of 1. Bhabha Atomic Research Centre, Mumbai 2. Raja Ramanna Centre for Advanced Technology, Indore 3. Variable Energy Cyclotron Centre, Kolkata 4. Inter University Accelerator Centre, New Delhi 5. Fermilab, USA June 3, 2014

  2. DAE Accelerator Development Program DAE laboratories have proposed (XII and XIII Plans) • Physics Studies and Enabling Technology Development for Ion Accelerators ( BARC) (Approved by AEC) • High Energy Proton LINAC Based Spallation Neutron Source ( RRCAT ) 1 GeV BARC RRCAT

  3. Project at Fermilab • Fermilab has proposed the construction of a High Intensity Superconducting Proton Accelerator (HISPA) (aka PIP-II) Phase I: PIP-II

  4. Indi dian an Institutions tutions and Fermi milab lab Collabo boratio ration • The collaboration signed MOU to collaborate on – High Intensity Superconducting Proton Accelerator for the respective domestic programs • Concept of “Total Project Collaboration” on Accelerator Feb 10, 2009

  5. Tec echni hnical cal wor ork k un under er MO MOU 1. Fermilab, RRCAT, BARC, IUAC and VECC Collaboration on ILC Main Linac SRF Accelerator Technology R&D” (October 2, 2007) 2. SLAC, RRCAT, BARC, IUAC and VECC Collaboration on ILC RF Power Sources and Beam Dump Design R&D” (December 3, 2007) 3. Fermilab and Indian Accelerator Laboratories Collaboration on High Intensity Proton Accelerator and SRF Infrastructure Development” (February 10, 2009) 4. Fermilab and Indian Accelerator Laboratories Collaboration on RF Power (325 MHz) Development for High Intensity Proton Accelerator ” (August 22, 2011 5. Collaboration on RF Power (650 MHz) Development for High Intensity Proton Accelerator ” (Aug 22,2011) 6. Collaboration on Instrumentation and Control for High Intensity Proton Accelerator ” (Aug 22, 2011) 7. Collaboration on Accelerator Physics issues for High Intensity Proton Accelerator ” ( Aug 22, 2011) Aug 22, 2011

  6. DOE OE-DAE DAE Imp mplementi lementing ng Agreeme reement nt Discovery Science: The United States’ Department of Energy and India’s Department of Atomic Energy signed an Implementing Agreement on Discovery Science that provides the framework for India’s participation in the next generation particle accelerator facility at Fermilab. Project Annex 1 for HISPA Collaboration awaits final signature

  7. Frequency: 325 and 650 MHz Scheme for the 1 GeV High Intensity Superconducting Proton Accelerator HWR, Elliptical RFQ Elliptical IS MEBT LEBT SSR Cavities Cavities ~150 MeV 1 GeV 200 MeV ~3 MeV 50 keV • We will go in steps but the initial design needs to be done for 30 mA • 1 st Phase will be similar to PIP-II

  8. Layout La out of of BARC RC Li Lina nac 5 cell elliptic HWR/ SSR0 RFQ IS SSR1 SSR2 Cavity 3 MeV ~10 MeV ~50 MeV ~200 MeV 1 GeV SSR0 & HWR cavities have been optimized to minimize peak fields. Parameters HWR SSR0 Units  G 0.11 0.11 Frequency 162.5 325 MHz E pk /E 0 5.15 5.78 B pk /E 0 6.44 6.53 mT/(MV/ m) Height (H) 860 399.4 mm HWR SSR0 Spoke radius 80 45 mm Halo Parameter in the SC Linac Sectio Caviti Energy @ ns es end (MeV) SSR0 13 10.0843 SSR1 25 50.0197 SSR2 49 201.774 A baseline beam dynamics Beam profile in the SC Linac Emittance evolution in the SC Linac design for the SC linac has Input emittance Output emittances been done for 30 mA H + In x and y = 0.22 pi mm mrad In x and y = 0.2360 pi mm mrad beam upto 200 MeV. In z = 0.3004 pi mm mrad In z = 0.3197 pi mm mrad

  9. RFQ FQ for or 200 00 Me MeV Li Lina nac Requirement:  Good beam quality (Longitudinal emittance small)  Maximize the Transmission Results: Energy : 3 MeV Length of RFQ : 3.8 m Transmission : 99.85 % Accelerated : 99.44 % (3 ± 0.105 MeV) RMS emittance at exit of RFQ: O/P Trans emitt: 0.02 cm-mrad O/P Long emitt: 0.03 cm-mrad

  10. Desi sign gn and nd Development elopment of of Foc ocus using ing le lens nses es for or ME MEBT BT Stages of Development work at BARC: 1. Electromagnetic design of Quadrupole Focussing Magnets and dipole correctors 2. Engineering design 3. Development drawings 4. Fabrication and Geometrical inspection 5. Magnetic measurements (integral fields) 6. Quality checks and traveller 7. Qualification tests with H + beam at 2.5 MeV Current Status: - A prototype of Quad F and dipole corrector has been developed and qualified for its magnetic, electric, thermal design & for beam focusing. - The prototype magnets are planned to be shipped to Fermilab for detailed magnetic measurements and integration with PXIE beam line. Fabrication of triplet and doublet frames with Dipole corrector has been initiated at BARC. Table1: Deliverables for PXIE MEBT/HEBT transverse focusing lattice with their optics requirements S. Type Qty. Integrated Gradie ient / Field ld homogeneit ity y in Longit itudin inal l no no integrated field ld GFR of 23 mm space 1 Quadrupole F (QF) 18 1.5 T 1% 100mm 2 Quadrupole D (QD) 16 0.85 T 1% 50mm 3 H/V Dipole 15 2.1 mT*m 5% 55mm corrector(DC)

  11. Devel elopme pment nt of Quad adrupol upole e - F F Magnet et Therm rmal Quali lificatio ion Electroma omagne gnetic ic Analy lysis is Yoke Developmen opment Electromagnetic design and analysis Thermal qualification with embedded RTD The Quadrupole magnet yoke using TOSCA sensors SN Particular Values 1. Current 9.98 A 0.73 Ω 2. Initial Resistance 0.055 Ω 3. Increase in Resistance 4. Temperature coefficient 0.003862 K -1 of Resistivity 5. Temperature Rise 19.40 °C Results of heat run tests Quad. Pole profile – dimensional accuracy Quadrupole-F magnet assembly 30 µm

  12. De Desi sign & De Devel elopme ment nt Di Dipol ole e co corrector ectors Electroma omagne gnetic ic Analy lysis is Magne netic ic Qualifica icatio ion Therm rmal Quali lificatio ion Magnetic measurement with Hall Electromagnetic design and analysis Thermal qualification with embedded sensors at BARC using TOSCA RTD sensors 50 120 Measured B-field Temperature in 0C 45 Surface Temperature of coil at 100 Simulated B-field Design Excitation level of 4A 40 B-Field(Gauss) 80 35 60 30 40 Ambient 25 20 20 0 100 200 300 400 0 Time Elapsed in seconds -400 -200 0 200 400 Axial Distance in mm Magnetic field measurement along axial Fabrication and assembly of dipole Results of thermal run test length of magnet corrector

  13. Qualification lification of dipole ole correc rrectors tors with h prot oton on beam m at FOTI TIA A facil cility, ity, BARC Sr. no Beam Parameter Value 1. Beam H + 2. Beam energy 2.5 MeV 3. Beam Current 10nA 4. Beam size 3 mm 5. Target distance 1 meter Particle trajectory simulations Steering of beam - analytical vs. measured Dipole corrector magnet assembly installed in FOTIA beam line

  14. Magneti gnetic c Measur asurements ements and beam m lin ine e Qualif lifica icatio tion of Quad d F Quad-F with ements surements on of Q tion Quad-F assembly installed in FOTIA beam line Magnetic measurement set-up comprising of 2.5 MeV H+ beam Induction coil, flip coil and Hall probe at etic measu icati BARC ifica y of Beam line Qualif y of magnetic Focusing snap shots at different currents, Beam focuses as current of Quad increases, and it tends to de-focus when focused beyond focal point Magnetic field and its higher order ary multipoles measured using induction coil mmar magnetometer Parameter Simulated Achieved Unit Summ ary Summar Input MMF 1500 1500 AT ∫G.dl 1.533 1.59 Tesla Beam snap shot Beam snap shots kmax Magnetic 8.91 8.95 (Quadrupole off) (Quadrupole on) Flux/pole

  15. Sin ingle le Spoke oke Reso sonator nator at IUAC AC • IUA UAC C is i s involved olved in th the e fabricat rication ion of tw two TEM-cl class ass 325 MHz, β =0.22, 22, Single gle Spoke ke Reson Resonat ator ors • Apart t from m th this, s, IUA UAC C & RRCAT T are re collab abor orati ating ng to build TM-clas lass s Single gle & Multi ti-ce cell l caviti ties es operati ating ng at t 1.3 GHz and 650 MHz. Sin ingle gle Cell ll 650 MHz, , β =0.9 9 Cavi vity ty • 5-Ce Cell 1.3 GHz Niobium m Cavi avity ty • In th the last t few months ths substanti ntial al amount t of e effort t has been devoted ed for r completin ting g th the tw two Spoke ke assemblies lies and subsequentl uently y att ttachin ing g th them to th the Outer r Shells ls.

  16. The Single Spoke Assembly In the last few months two Spoke assemblies have been completed and subsequently attached to the Outer Shells. Before electro-polishing After electro-polishing

  17. Sh Shel ell + Sp Spoke e Assem embly Recently the Spoke assemblies were successfully attached to the Outer Shells.

  18. Next xt Ste tep p for or SSR1 The next step is to tune the resonators and attach the End Walls to the Outer Shells. All the four End Wall assemblies are ready. All the 4 End Walls (left), and electropolished RF side of an End Wall (right).

  19. Me Measur asurem ements ents SSR1 R1 The Spoke + Shell assemblies and the End Wall assemblies are being readied now for frequency tuning.

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