beam driven plasma-wakefield linear collider: pwfa-lc j.p delahaye / slac on behalf of j.p. e. adli,...
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Beam Driven Plasma-Wakefield Linear Collider:PWFA-LC
J.P Delahaye / SLAC
On behalf of
J.P. E. Adli, S.J. Gessner, M.J. Hogan, T.O. Raubenheimer (SLAC),
P.Muggli (MPI), C.Lindstrom (Oslo University), A. Seryi (Adams Inst.)
W. An, C. Joshi, W. Mori (UCLA)
Co authors of:
SLAC Pub 13766 (2009)
Snowmass 2013 (arXiv:1308.1145)
IPAC13 (MOPWO011)
IPAC14 (THPRI013)
2Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
Drive beam generation & distribution derived from
CLIC (CTF3 validation)
Pulsed main beam: 125b * 4ns * 100Hz
Effective accelerating gradient dominated by inter-
plasma cell (100m)
• 25 GeV/100m = 250 MeV/m
Cost and power consumption dominated by turn
arounds (40 at 1TeV)
• Every plasma cell (25 GeV acceleration)
Short interval (4ns) between bunches in plasma
• Plasma relaxation?
Original concept of a beam driven PWFA-LCCounter-propagating drive beam (a la CLIC)
SLAC Pub 13723 & 13766 (2009)
J.P.Delahaye
3Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
Plasma cell(as optimized by E.Adli: arXiv:1308.1145)
J.P.Delahaye
hdrive to plasma ~ 76%, hplasma to main ~ 66%hdrive to main > 50%
Single bunch process
Main bunch:1E10 charges (1.6 nC), 20 mm bunch length
Drive bunch:2E10 charges (3.2 nC), 25 GeV
Plasma cell:Plasma cell 3.3 m long with 2x1016/cm3 density Transformer ratio: 1, 7.6 GV/m accelerating field 25 GeV acceleration gain per plasma cell.
4Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
Co-linear beam driven PWFA Linear Collider : Single bunch: continuous operation, high repetition (10 kHz)
SLAC-PUB-15426 (arXiv:1308.1145) IPAC13 & IPAC14
J.P.Delahaye
Long interval between pulses in plasma (100 ms)
Effective feedback at IP by high repetition rate
Large geometric acceleration: 25GeV/30m=833MeV/m
Efficient drive beam acceleration by SCRF
recirculating linac (continuous operation)
No turn around
Drive & main bunches synchronisation by magnetic chicane (2ns=60cm) at each plasma cell
5Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
Major beam parameters covering a wide energy range
J.P.Delahaye
6Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
PWFA extending high energy frontierwith potential of considerable cost & power savings
J.P.Delahaye
PWFA
PWFA
7Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
Pulsed mode bunch train collisions (a la ILC)
J.P.Delahaye
230 to 600 mApulsed drive linac
feasibility?(NC fully loaded orSC RF low frequency)
Similar bunch structure and beam parameters as the ILC
8Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
An alternative ILC upgrade by PWFAfrom 250GeV to 1 TeV and beyond?
J.P.Delahaye
ILC TeVupgrade
One possible scenario could be:1) Build & operate the ILC as presently proposed up to 250 GeV (125 GeV/beam): total extension 21km 2) Develop the PFWA technology in the meantime (up to 2025?) 3) When ILC upgrade requested by Physics (say up to 1 TeV), decide for ILC or PWFA technology:4) Do not extend the ILC tunnel but remove latest 500m of ILC linac (beam energy reduced by 12.5 GeV)5) Install a bunch length compressor and 16 plasma cells in latest part of each linac in the same tunnel for a 375+12.5 GeV PWFA beam acceleration (465m)6) Reuse the return loop of the ILC main beam as return loop of the PWFA drive beam
500 m
9Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
ILC afterburner from 500 GeV to 1 TeV by PWFA An efficient TeV-LC without drive beam generation
J.P.Delahaye
ILC acceleration till 500 GeV
Each 250 GeV ILC bunch split:- one drive bunch(2/3 charge)- one main bunch(1/3 charge)
PWFA till 1 TeV: Drive bunch provides 50% energy to main bunch thus doubles main beam energy
No drive beam generation and distributionNo extra power and length
Low luminosity per bunchdue to low charge butcompensated by stronger horizontal focusing and higher repetition frequency
18 TeV
1 TeV
500 GeV
320 m
11 km
10PWFA-LC, Sept 23, 2014
“Artistic” view of the inter-plasma cell layout
J.P.Delahaye
Realistic design of main beam inter-cell
by C.Lindstrom (next)
Drive beam line
Main beam line
PWFA-LC, Jan 20, 2015
Extraction of last drive beam bunch from the drive beam pulse by state of the art
Kickers (developed for ILC Damping Ring) with a rise time of 2ns
• Minimum interval between bunches of 2ns at 25 GeV
• Drive bunches synchronisation by magnetic chicane with 60cm delay
• 4 SC bending magnets 7.5 T, 2m long (280mrad) for each plasma cell
Shorter rise time with RF transverse deflectors
• Bunch interval a fraction of wavelength (ex with 4 bunches)
• Works only for a limited number of bunches
• 4 bunches powering 4 plasma cells
• Corresponding to a collider of 200 GeV c.m.
• Bunch interval = RF deflector period/4
Interval between drive bunches and magnetic chicane?
J.P.Delahaye
Pi/2 phase advance
1
RF deflector
RF deflector
Septum3 2 1
1
2
3Pi/2 phase advance
24 4 34
12Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
Combination of RF transverse deflectors at various frequencies for increasing the number of drive bunches
J.P.Delahaye
13PWFA-LC, March 10, 2015J.P.Delahaye
Alternative multilines drive beam distribution(Carl Lindstrom)
14PWFA-LC, March 10, 2015J.P.Delahaye
Alternative multilines drive beam distribution(Carl Lindstrom)
PWFA-LC, Jan 20, 2015
Drive bunch interval of (1.5E9*4)-1 = 0.167ns or 5cm
• Compatible with efficient drive beam generation by SC
recirculating linac equipped with 1.5 GHz SC RF cavities
and multiplication frequency by a factor 4 (a la CLIC)
• Reasonable drive beam intensity of 19.4 Amp during pulse
Reasonable magnetic chicane with for each cell:
• 4 magnets 2.4m long and 2 T with 50 mrad deflection
Transverse deflectors
(2 of each kind for each cell)
Tentative sketch
Drive beam and chicanes
J.P.Delahaye
30MV with TCAV(1m) @12GHz
(MV)
PWFA-LC, Jan 20, 2015
1.2 TeV acceleration based on co-propagating drive beam
scheme with magnetic chicanes:
• One beam turn-around for every additional 1.2 TeV c.m.
• Number of turn-arounds reduced by a factor 48 in respect with
counter-propagating drive beam scheme
A hybrid schemeCo & Counter-propagating drive beam
J.P.Delahaye
17PWFA-LC, March 10, 2015
Rough cost estimation of various options of drive beam distribution of a 3 TeV collider
J.P.Delahaye
Common assumption: drive beam made of bunches with 5cm interval
18PWFA-LC, March 10, 2015
Drive beam generation and distributionSingle-bunch main beam no accumulation with compression(Hybrid 3 TeV LC made of 500 GeV sectors powered by 20 bunches each)
J.P.Delahaye
667ps = 20cm
5 bunches, 4.85A
3.33ns = 1m
0 to 0.5 TeV 0.5 to 1.0 TeV 1.0 to 1.5 TeV
1.5GHz Drive Linac
953m 1649m 2128m
10 kHz kicker
Main beam10kHz 100ms =30km 100ms =30km
Drive beam 1.26 MHz 24% duty factor
SC option compatible with drive beam pulsed operation?
1906m = 6.35ms 3298m = 11.0ms
167ps = 5cm
20 bunches, 19.4A
3.33ns = 1m X4 multiplication
1906/4=476.5mcircumference
238m = 793ns 2*4*3 =24 trains of 5 bunches, 7110m = 23.70ms
100ms =30km
19Beam driven PWFA @ FACET-II Science Workshop (Oct 14, 2015)
ConclusionsPWFA a very promising technology:
Attractive schemes possibly extending LC reach in multi-TeV range
Potential of considerable savings (Cost & Power):
• High accelerating fields: effective 833 MeV/m (10*CLIC)
• Excellent power efficiency (Wall-plug to beam ~ 20% = 2*CLIC)
Great flexibility of time interval
Continuous or pulsed mode of operation
An alternative for ILC energy upgrade?
Many challenges still to be addressed
Adaptation to e+ acceleration (tentatively assumed similar to e-) !
Beam quality preservation, efficiency, etc…
High energy applications heavily rely on multi-stages
Inter-space plasma cell design critical (main & drive beam lines)
Short(er) matching section from plasma to plasma (larger effective gradient)
Magnetic chicanes detailed design including CSR (short bunches)
Most appropriate drive beam generation & distribution?
Major issues should be addressed in FACET-II Two stages system test in FACET-II (phase 4)?
Optics corrections, tolerances, etc….
J.P.Delahaye