1. eRHIC design status V.Ptitsyn for the eRHIC design team

2. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 eRHIC Scope Polarized leptons 3-10 Gev ( 20GeV ) Polarized light ions ( 3 He) 167 Gev/u Heavy ions (Au) 50-100 Gev/u Polarized protons 50-250 Gev (25 GeV) Electron accelerator RHIC e-e- e+e+ p 70% beam polarization goal

3. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 ERL-based eRHIC Design  10 GeV electron design energy. Possible upgrade to 20 GeV by doubling main linac length.  5 recirculation passes ( 4 of them in the RHIC tunnel)  Multiple electron-hadron interaction points (IPs) and detectors;  Full polarization transparency at all energies for the electron beam;  Ability to take full advantage of transverse cooling of the hadron beams;  Possible options to include polarized positrons: compact storage ring; compton backscattered; undulator-based. Though at lower luminosity. Four recirculation passes PHENIX STAR e-ion detector eRHIC Main ERL (1.9 GeV) Low energy recirculation pass Beam dump Electron source Possible locations for additional e-ion detectors

4. ERL-based eRHIC Parameters: e-p mode High energy setupLow energy setup pepe Energy, GeV25010503 Number of bunches166 Bunch spacing, ns71 Bunch intensity, 10 11 21.22 Beam current, mA420260420260 Normalized 95% emittance,  mm.mrad 64606570 Rms emittance, nm3.841916.5  *, x/y, cm 26252630 Beam-beam parameters, x/y0.0150.590.0150.47 Rms bunch length, cm201 1 Polarization, %70807080 Peak Luminosity, 1.e33 cm -2 s -1 Aver.Luminosity, 1.e33 cm -2 s -1 2.60.53 0.870.18 Luminosity integral /week, pb -1 530105 If effective high energy transverse cooling becomes possible the proton emittance and electron beam current can be reduced simultaneously, keeping the same luminosity.

5. ERL-based eRHIC Parameters: e-Au mode High energy setupLow energy setup Aue e Energy, GeV10010503 Number of bunches166 Bunch spacing, ns71 Bunch intensity, 10 11 1.11.21.11.2 Beam current, mA180260180260 Normalized 95% emittance,  mm.mrad 2.44602.4270 Rms emittance, nm3.73.87.57.8  *, x/y, cm 26252625 Beam-beam parameters, x/y0.0150.260.0150.43 Rms bunch length, cm201 1 Polarization, %0000 Peak e-nucleon luminosity, 1.e33 cm -2 s -1 Average e-nucleon luminosity, 1.e33 cm -2 s -1 2.91.5 1.00.5 Luminosity integral /week, pb -1 580290

6. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Main R&D Items Electron beam R&D for ERL-based design: –High intensity polarized electron source Development of large cathode guns with existing current densities ~ 50 mA/cm 2 with good cathode lifetime. –Energy recovery technology for high power beams multicavity cryomodule development; high power beam ERL, BNL ERL test facility; loss protection; instabilites. –Development of compact recirculation loop magnets Design, build and test a prototype of a small gap magnet and its vacuum chamber. –Evaluation of electron-ion beam-beam effects, including the kink instability and e- beam disruption Main R&D items for ion beam: –Polarized 3 He production (EBIS) and acceleration –166 bunches General EIC R&D item: –Proof of principle of the coherent electron cooling

7. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Compact linac design Increased number of 700MHz cavities inside one cryostat to 6 cavities. 3 rd harmonic cavities (2 per cryostat) for the momentum spread minimization. Cavity gradient: 19.5 Mev/m; Average acceleration rate: 8.2 MeV/m; Total length of 1.9 GeV linac: 232m (instead of ~360m in the previous design). 6 cav’s DFD 11.9m1m DFFF Evolution of rms beam sizes along the linac on all acceleration passes. Recirc.passes are presented by Unit matrix. Doublet focusing (90º phase advance per cell) Constant quadrupole gradient. E.Pozdeyev’s talk in the Parallel session Compact linac design makes more realistic a design option with linac(s) placed inside the RHIC tunnel rms beam size, mm s (m)

8. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 ERL Test Facility 50 kW 703.75 MHz system Cryo-module SRF cavity 1 MW 703.75 MHz Klystron e - 2.5MeV Laser SC RF Gun e - 2.5 MeV Beam dump e - 15-20 MeV Merger system Return loop test of high current (several hundred mAmps) high brightness ERL operation test of high current beam stability issues 5-cell cavity SRF ERL highly flexible lattice 704 MHz SRF gun test Start of the commissioning in 2009. D.Kayran’s talk at the Parallel session 5 cell SRF cavity arrived in BNL in March 2008.

9. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 eRHIC Recirculation passes  Separate recirculation loops  Small aperture magnets  Low current, low power consumption  Minimized cost 5 mm 10 GeV (20 GeV) 8.1 GeV (16.1 GeV) 6.2 GeV (12.2 GeV) 4.3 GeV (8.3 GeV) Common vacuum chamber Approved LDRD for the compact magnet development

10. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Recirculation Pass Optics Modification The optics based on Flexible Momentum Compaction cell provides achromatic and isochronal transfer through each arc and allows for flexible adjustment of R 56 parameter. More details in V.Ptitsyn’s talk in the Parallel session Other features: -phase trombone (in the straight sections) -path length control (at 12 o’clock region) -initial design for separator/merger

11. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Interaction Region Design Present IR design features:  No crossing angle at the IP  Detector integrated dipole: dipole field superimposed on detector solenoid.  No parasitic collisions.  Round beam collision geometry with matched sizes of electron and ion beams.  Synchrotron radiation emitted by electrons does not hit surfaces in the detector region.  Blue ion ring and electron ring magnets are warm.  First quadrupoles (electron beam) are at 3m from the IP  Yellow ion ring makes 3m vertical excursion. (Blue) ion ring magnets (Red) electron beam magnets (Yellow) ion ring magnets Detector HERA type half quadrupole used for proton beam focusing C.Montag’s talk at the Parallel session

12. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Beam-beam interaction studies Several features of the beam-beam interactions are under consideration: The kink instability is stabilized for design beam intensities by proper choice of the chromaticity. Techniques for compensation of the mismatch caused by the beam-beam are under consideration. Both electron beam disruption and proton beam-beam parameter benefit from lower  * of electrons. More investigations are underway for incoherent proton beam emittance growth in the presence of electron pinch, including the optimal choice of the working point. For details see a presentation in the Parallel session as well as a talk at previous meeting.

13. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Effect of electron pitching on the proton beam The electron beam is focused by strong beam-beam force. That in turn leads to larger proton beam-beam parameter Proper selection of the IP  and  -waist is important to minimize the proton beam-beam parameter e-beam

14. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Polarized Electron Source Design Items -Large area cathodes (diameter > 1cm) -Ring-like cathode, to minimize ion bombardment damage. -Multiple gun approach. RF-combiner. -Active cooling, to accommodate ~100W of heating load from laser power R&D efforts are led by MIT-Bates experts. For recent results see Y.Tsentalovich’s talk

15. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Other design options Under consideration also:  ERL-based design for smaller energy. Electron energy up to 2-3 GeV. Acceleration done by a linac placed in the RHIC tunnel. It can serve as first stage for following higher electron energy machine.  High energy (up to 20-30 GeV) ERL-based design with all accelerating linacs and recirculation passes placed in the RHIC tunnel. Can be elegant and cost saving design solution.  Variation of this design option uses FFAG design of recirculating passses. Further details are in talks by V.N.Litvinenko and D.Trbojevic in Parallel Session.  Ring-ring design option. Backup design solution. See eRHIC ZDR for more details. The peak luminosity is limited to 4*10 32 cm -2 s -1

16. V.Ptitsyn, EIC Collaboration Meeting, 05/19/08 Summary The accelerator design work continues on various aspects of the ERL- based design of eRHIC, which presently aims to provide e-p average luminosity at 10 33 cm -2 s -1 level. Recent advances are done in several design areas, including linac design, recirculating pass optics, studies of beam-beam effects. R&D subjects, such as polarized source development, ERL test facility and compact magnet design, are supported by financing. So, one can expect advances on those directions in coming 2 years. Other design options under consideration: ERL-based designs with linac(s) in the tunnel and the ring-ring design.