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Perspective on the Accelerator Physics Side of EICC LBNL

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Lianc-ring has too much technical challenges, some virtually impossible ... (near impossible) Small bunch number. Long ion bunch, weak FF. High collision frequency ... – PowerPoint PPT presentation

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Title: Perspective on the Accelerator Physics Side of EICC LBNL


1
Perspective on the Accelerator Physics Side of
EICC _at_ LBNL
  • January 16, 2009

2
  • ????,?????
  • ??????,?????
  • ??????,?????
  • ????
  • If you know the enemy and know yourself, you need
    not fear the result of a hundred battles.
  • If you know yourself but not the enemy, for every
    victory gained you will also suffer a defeat.
  • If you know neither the enemy nor yourself, you
    will succumb in every battle.
  • SunTzu

3
Outline
  • ELIC/mEIC
  • eRHIC/MEeIC
  • Others (LeHC and ENC_at_FAIR)
  • Comparisons and assessments
  • Remarks

4
eRHIC Ring-Ring
  • Conceptual design completed
  • Only on2 IP
  • No major RD except electron cooling (also in
    RHIC II)
  • Cost 700M
  • Design suffers low luminosity (lt1033)
  • 165 bunches in RHIC ring? low collision frequency
  • Very long ion bunch? large ß, weak final
    focusing
  • Must redo AGS and RF of RHIC to improve ? too
    high cost

5
eRHIC ERL-Ring
  • Lianc-ring has too much technical challenges,
    some virtually impossible
  • Polarization electron current too high (420mA
    vs. 0.1mA state-of-art)
  • Multi-pass (5x2) high energy ERL
  • linac-ring beam-beam

6
MEeIC Half Way of eRHIC
  • Reduce electron energy from 10 GeV to 2 or 4 GeV
  • Save cost on large ERL and ring for electron
  • Same design, same technologies and same problems

7
MEeIC Luminosity
  • MEeIC luminosity 0.09 to 0.9 (1033 1/s/cm2)
  • How to get this luminosity?
  • ERL for electron beam
  • High polarized electron current, 50 mA vs. 0.1 mA
    state-of-art
  • Large electron beam-beam tune-shift (disruption)
  • Multiple-pass ERL (3x2 passes)
  • Coherent electron cooling for short ion bunch and
    small emittance
  • Proton energy is 250 GeV/u (vs. 11 GeV/u for
    MEIC)
  • Ion bunch length reduces from 20 cm to 5 cm
  • Transverse RMS emittance reduces from 9.4 nm to
    0.94 nm
  • Proton bunch 21011 protons (a factor of 80
    large than MEIC bunch)
  • Averaged charge density is 3.4, 8.5 up to 34
    times than MEIC
  • Technology development cycle
  • Polarized source
  • Coherent electron cooling
  • Electron cooling FEL, great idea but much more
    complex
  • Conventional Electron cooling (1967 Bodlker idea
    ? 1976 Derbenev theory ? 1980? Low energy
    experiement ? 2004 FNAL 8 GeV p- demo)

8
LHeC and ENC_at_FAIR
20140 GeV e 17 TeV p
3 GeV e 15 GeV p
9
ELIC/MEIC vs. eRHIC/MEeIC
10
Personal Reflection
  • eRHIC/MEeIC
  • Not a working design
  • No satisfactory backup plan
  • Good RD progress
  • ELIC/MEIC
  • Good design and schemes
  • Not enough RD progress

11
Suggestions
  • ELIC
  • As is with continue optimization
  • MEIC
  • Next design iteration follows science case
    evolution
  • RD (till next EICC, May 28)
  • Design independent
  • Individual topics
  • IP
  • Polarization (electron/proton)
  • Cooling (coherent/conventional)

12
Lets hear what Slava is going to say?
13
Slavas View of Staging
  • Stage 1 Two warm rings in a 300 m tunnel, crab
    crossing, traveling ion focus.
  • Stage 2 SC ion ring in same tunnel
  • Stage 3 Full size (1.5 to 2.5 km) figure-8
    tunnel with warm electron ring
  • Stage 4 SC ion ring (high energy EIC)

14
Accelerator Physics RD Issues
  • Why we need Figure-8 rings (tunnels)?
  • Acceleration of polarized ions in boosters (small
    SC ring and e-collider ring) and ion collider
    Ring
  • (AGS still struggling the intrinsic spin
    resonances)
  • Longitudinal ion spin (especially deuteron)
  • A modest warm solenoid or SC snake in crossing
    straight is needed to stabilize spin
  • Two SC snakes in arcs (for p and 3He) are needed,
    if to have longitudinal spin at 4 IP. These three
    snakes are ease!
  • Medium energy electron cooling (Fermilab/BINP)
  • Traveling ion focusing
  • Crab crossing
  • Repetition rate synchrotron
  • Synchrotron for electron cooling ring (variable
    electron orbit)
  • Other RD which can lead high luminosity
  • Repetition rate (0.5 to 1.5 GHz)
  • Detector space (4 m to 2 m)
  • Aperture size
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