Author: Koubek, B.
Paper Title Page
MOPAB192 LILac Energy Upgrade to 13 MeV 651
 
  • B. Koubek, S. Altürk, M. Busch, H. Höltermann, J.D. Kaiser, H. Podlech, U. Ratzinger, M. Schuett, M. Schwarz, W. Schweizer, D. Strehl, R. Tiede, C. Trageser
    BEVATECH, Frankfurt, Germany
  • A. Brunzel, P. Nonn, H. Schlarb
    DESY, Hamburg, Germany
  • A.V. Butenko, D.E. Donets, B.V. Golovenskiy, A. Govorov, K.A. Levterov, D.A. Lyuosev, A.A. Martynov, V.A. Monchinsky, D.O. Ponkin, K.V. Shevchenko, I.V. Shirikov, E. Syresin
    JINR, Dubna, Moscow Region, Russia
 
  In the frame of the NICA (Nu­clotron-based Ion Col­lider fA­cil­ity) ion col­lider up­grade a new light ion LINAC for pro­tons and ions will be built in col­lab­o­ra­tion be­tween JINR and BE­VAT­ECH GmbH. While ions with a mass-to-charge ratio up to 3 will be fed into the NU­CLOTRON ring with an en­ergy of 7 MeV/u, pro­tons are sup­posed to be ac­cel­er­ated up to an en­ergy of 13 MeV using a third IH struc­ture. This en­ergy up­grade com­prises a third IH struc­ture, a dual-use De­buncher cav­ity as well as an ex­ten­sion of the LLRF con­trol sys­tem built on Mi­croTCA tech­nol­ogy.  
poster icon Poster MOPAB192 [4.914 MB]  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2021-MOPAB192  
About • paper received ※ 11 May 2021       paper accepted ※ 31 May 2021       issue date ※ 20 August 2021  
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THPAB167 Technical Design of an RFQ Injector for the IsoDAR Cyclotron 4075
 
  • H. Höltermann, D. Koser, B. Koubek, H. Podlech, U. Ratzinger, M. Schuett, M. Syha
    BEVATECH, Frankfurt, Germany
  • J.M. Conrad, J. Smolsky, L.H. Waites, D. Winklehner
    MIT, Cambridge, Massachusetts, USA
 
  For the Iso­DAR (Iso­tope De­cay-At-Rest) ex­per­i­ment, a high in­ten­sity (10 mA CW) pri­mary pro­ton beam is needed. To gen­er­ate this beam, H2+ is ac­cel­er­ated in a cy­clotron and stripped into pro­tons after ex­trac­tion. An RFQ, par­tially em­bed­ded in the cy­clotron yoke, will be used to bunch and ax­i­ally in­ject H2+ ions into the main ac­cel­er­a­tor. The strong RFQ bunch­ing ca­pa­bil­i­ties will be used to op­ti­mize the over­all in­jec­tion ef­fi­ciency. To keep the setup com­pact the dis­tance be­tween the ion source and RFQ can be kept very short as well. In this paper, we de­scribe the tech­ni­cal de­sign of the RFQ. We focus on two crit­i­cal as­pects: 1. The use of a split-coax­ial struc­ture, ne­ces­si­tated by the low fre­quency of 32.8 MHz (match­ing the cy­clotron RF) and the de­sired small tank di­am­e­ter; 2. The high cur­rent, CW op­er­a­tion, re­quir­ing a good cool­ing con­cept for the RFQ tank and vanes.  
poster icon Poster THPAB167 [2.162 MB]  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2021-THPAB167  
About • paper received ※ 14 May 2021       paper accepted ※ 27 July 2021       issue date ※ 21 August 2021  
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