Author: Boine-Frankenheim, O.
Paper Title Page
MOPS053 Electron Cloud Effects in Coasting Heavy-ion Beams* 724
 
  • F.B. Petrov, T. Weiland
    TEMF, TU Darmstadt, Darmstadt, Germany
  • O. Boine-Frankenheim
    GSI, Darmstadt, Germany
 
  Funding: Work supported by BMBF under contract 06DA9022I.
Dur­ing slow ex­trac­tion of in­tense ion beams elec­tron clouds (EC) can ac­cu­mu­late in the cir­cu­lat­ing coast­ing beam and re­duce the ex­trac­tion ef­fi­cien­cy. This is a con­cern for the ex­ist­ing SIS-18 heavy ion syn­chrotron at GSI and for the pro­ject­ed SIS-100 as part of the FAIR pro­ject. For medi­um en­er­gy heavy-ion beams the pro­duc­tion of elec­trons from resid­u­al gas ion­iza­tion is very ef­fec­tive. The elec­tron den­si­ty is lim­it­ed due to Coulomb scat­ter­ing by the beam ions. Above a thresh­old beam in­ten­si­ty the two-stream in­sta­bil­i­ty and the re­sult­ing co­her­ent beam os­cil­la­tions limit the elec­tron den­si­ty. Below this thresh­old the elec­tron cloud can lead to ob­serv­able de­for­ma­tions of the Schot­tky side-bands. To avoid EC build-up one can in­tro­duce a gap in the beam using bar­ri­er rf buck­et. The re­duc­tion of the build-up ef­fi­cien­cy caused by the gap is stud­ied in de­tails based on the so­lu­tion of the Hill's equa­tion for elec­trons. Fi­nal­ly we es­ti­mate the sat­u­ra­tion level for the elec­tron cloud den­si­ty.
 
 
THPS012 Simulation of the Generation and Transport of Laser-Accelerated Ion Beams 3445
 
  • O. Boine-Frankenheim, V. Kornilov
    GSI, Darmstadt, Germany
  • L. Zsolt
    TEMF, TU Darmstadt, Darmstadt, Germany
 
  In the frame­work of the LIGHT pro­ject a ded­i­cat­ed test stand is under prepa­ra­tion at GSI for the trans­port and fo­cus­ing of laser ac­cel­er­at­ed ion beams. The rel­e­vant ac­cel­er­a­tion mech­a­nism for the pa­ram­e­ters achiev­able at the GSI PHE­LIX laser is the TNSA (Tar­get Nor­mal Sheath Ac­cel­er­a­tion). The sub­se­quent evo­lu­tion of the ion beam can be de­scribed rather well by the isother­mal plas­ma ex­pan­sion model. This model as­sumes an ini­tial dense plas­ma layer with a 'hot' elec­tron com­po­nent and 'cold' ions. We will pre­sent 1D and 2D sim­u­la­tion re­sults ob­tained with the VOR­PAL code on the ex­pan­sion of the beam and on the cool­ing down of the neu­tral­iz­ing elec­trons. The elec­trons and their tem­per­a­ture can play an im­por­tant role for the fo­cus­ing of the beam in a solenoid mag­net, as fore­seen in the GSI test stand. We will dis­cuss pos­si­ble con­trolled de-neu­tral­iza­tion schemes using ex­ter­nal mag­net fields.  
 
MOPS052 Analytical and Numerical Calculations of Beam Pipe Impedances at Low Frequencies with Application to Thin SIS100 Pipe 721
 
  • U. Niedermayer, O. Boine-Frankenheim, L. Hänichen
    TEMF, TU Darmstadt, Darmstadt, Germany
 
  The pro­ject­ed fast ramped syn­chrotron SIS100 for FAIR uses an el­lip­ti­cal stain­less steel beam pipe of 0.3 mm thick­ness. The low­est co­her­ent be­ta­tron side­bands reach down to 100 kHz which de­mands ac­cu­rate impedance cal­cu­la­tions in the low fre­quen­cy (LF) regime. For these fre­quen­cies, i.e. skin depth greater than wall thick­ness, struc­tures be­hind the pipe may con­tribute to the impedance. Due to the ex­treme­ly large wake length nu­mer­i­cal meth­ods in the time do­main are not ap­pli­ca­ble. The lon­gi­tu­di­nal and trans­verse impedance of the thin SIS100 beam pipe in­clud­ing struc­tures be­hind the pipe are ob­tained nu­mer­i­cal­ly by a method using power loss in the fre­quen­cy do­main. We com­pare dif­fer­ent an­a­lyt­i­cal mod­els for sim­pli­fied pipe struc­tures to the nu­mer­i­cal re­sults. The dc and ul­tra-rel­a­tivis­tic lim­its are in­ves­ti­gat­ed. The in­ter­pre­ta­tion of bench mea­sure­ments in the LF regime is dis­cussed.  
 
WEPC094 Energy Loss and Longitudinal Wakefield of Relativistic Short Ion Bunches in Electron Clouds 2229
 
  • F. Yaman, O. Boine-Frankenheim, E. Gjonaj, T. Weiland
    TEMF, TU Darmstadt, Darmstadt, Germany
  • G. Rumolo
    CERN, Geneva, Switzerland
 
  Funding: Work supported by BMBF under contract 06DA9022I
The aim of our study is the nu­mer­i­cal com­pu­ta­tion of the wake­field, impedance and en­er­gy loss for an en­er­get­ic, short (< 10 ns) ion bunch pen­e­trat­ing an elec­tron cloud plas­ma re­sid­ing in the beam pipe. We use a 3-D self-con­sis­tent and high­er order PIC code based on the full-wave so­lu­tion of the Maxwell equa­tions in the time do­main. In our sim­u­la­tions we ob­serve the in­duced den­si­ty os­cil­la­tions in the elec­tron cloud in the lon­gi­tu­di­nal as well as in the trans­verse di­rec­tions. A spe­cial nu­mer­i­cal pro­ce­dure is ap­plied to com­pute the lon­gi­tu­di­nal wake po­ten­tial and the broad­band cou­pling impedance due to the beam-elec­tron cloud in­ter­ac­tion. The code is ap­plied to the case of the CERN SPS and the pro­ject­ed SIS-100 at GSI. The ef­fects of the beam pipe, elec­tron den­si­ty, bunch in­ten­si­ty and ex­ter­nal mag­net­ic dipole fields are stud­ied. The re­sults are com­pared to an­a­lyt­i­cal and nu­mer­i­cal mod­els of re­duced com­plex­i­ty.
 
 
THPS001 Experimental Studies of Beam Loss during Low Energy Operation with Electron Cooled Heavy Ions in the ESR 3424
 
  • P.A. Görgen, O. Boine-Frankenheim
    TEMF, TU Darmstadt, Darmstadt, Germany
  • S. Appel, C. Dimopoulou, S.A. Litvinov, M. Steck
    GSI, Darmstadt, Germany
 
  At the ESR at GSI elec­tron cooled heavy ion beams are de­cel­er­at­ed to 4 MeV/u and ex­tract­ed for the HI­TRAP ex­per­i­ment. We will re­port about cool­ing equi­lib­ri­um mea­sure­ments at 4 and 30 MeV/u for Ar18+ coast­ing beams. We com­pare the equi­lib­ri­um beam pa­ram­e­ters with re­sults from beam dy­nam­ics sim­u­la­tions using the BE­TA­COOL code and an an­a­lyt­ic model of re­duced com­plex­i­ty. The time slot in which HI­TRAP ac­cepts beam is 2μs long. For op­ti­mum ef­fi­cien­cy the beam has to be bunched to this length be­fore ex­trac­tion. The ob­tained bunch pro­files are com­pared to lon­gi­tu­di­nal beam dy­nam­ics sim­u­la­tions. Our mea­sure­ments show that at both en­er­gies bunch­ing leads to se­vere beam loss. The es­ti­mat­ed trans­verse space charge tune shifts dur­ing the rf bunch­ing in­di­cate that res­o­nance cross­ing might be re­spon­si­ble for the ob­served the beam loss. The in­flu­ence of the tune shift will be fur­ther eval­u­at­ed through res­o­nance mea­sure­ments.