ILC Accelerator Activities in North America (cooperation with France)
Presentation at IRFU Linear Collider Days prepared by:
Marc Ross (SLAC) November 29, 2013
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2013 IRFU Linear Collider Days
ILC Accelerator Activities in North America (cooperation with - - PowerPoint PPT Presentation
ILC Accelerator Activities in North America (cooperation with France) Presentation at IRFU Linear Collider Days prepared by: Marc Ross (SLAC) November 29, 2013 2013 IRFU Linear Collider Days 1 Completing the ILC Technical Design Phase
Presentation at IRFU Linear Collider Days prepared by:
Marc Ross (SLAC) November 29, 2013
1
2013 IRFU Linear Collider Days
» R & D to enable Project Proposal and updated Value estimate –
with Cost Containment
» SC RF Technology Transfer
» Consists of two parts: 1) R & D Report and 2) Design Description
» SRF Linac: Fermilab NML, DESY E-XFEL and FLASH, KEK STF » Beam Dynamics: Cornell CesrTA (2008 – 2010) » Beam Tuning: KEK ATF2
» CEBAF Upgrade and E-XFEL
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3 2013 IRFU Linear Collider Days
» R & D to enable Project Proposal and updated Value estimate –
with Cost Containment
» SC RF Technology Transfer
» Consists of two parts: 1) R & D Report and 2) Design Description
» SRF Linac: Fermilab NML, DESY E-XFEL and FLASH, KEK STF » Beam Dynamics: Cornell CesrTA (2008 – 2010) » Beam Tuning: KEK ATF2
» CEBAF Upgrade and E-XFEL
» Development of a strong industrial base
» CEBAF Upgrade and E-XFEL
» SRF Linac: Fermilab NML, DESY E-XFEL and FLASH, KEK STF » Beam Dynamics: Cornell CesrTA (2008 – 2010) » Beam Tuning: KEK ATF2
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By the end of the XFEL Production > 1000 cavities will have been fabricated by industry and processed using the basic TESLA – recipe.
» Two companies
time to construct 4 months; time to test unknown
» (See E. Elsen)
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6 'BB Lunch', M. Ross (SLAC)
7 'BB Lunch', M. Ross (SLAC)
8 'BB Lunch', M. Ross (SLAC)
Slide dated late 09.2013 All C100 cryomodules are now installed (11.2013)
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in late July 2013:
» Shakeup of US accelerator construction projects: » SLAC LCLS-II project redefined » ANL APS upgrade program redefined
» 4 GeV CW SRF Linac-based FEL » Use ILC / XFEL 1.3 GHz technology » Installed in the upstream 1/3 of the SLAC linac housing » (50 year old S-band linac to be completely removed)
» First light end of FY 2019
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2013 IRFU Linear Collider Days
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2013 IRFU Linear Collider Days
CM01 CM2,3 CM04 CM15 CM16 CM35 BC1
270 MeV R56 = -65 mm Ipk = 60 A Lb = 0.40 mm sd = 1.4 %
BC2
1550 MeV R56 = -65 mm Ipk = 1000 A Lb = 0.024 mm sd = 0.50 %
GUN
0.75 MeV
LH
98 MeV R56 = -5 mm Ipk = 12 A Lb = 2.0 mm sd = 0.006 %
L0
j 0 V0 97 MV
L1
j =-26° V0 =235 MV
HL
j =-170° V0 =40 MV
L2
j = -28° V0 = 1448 MV
L3
j = 0 V0 = 2460 MV
LTU
4.0 GeV R56 = 0 Ipk = 1000 A Lb = 0.024 mm sd 0.02 %
100 pC; Machine layout 26SEP2013; Bunch length Lb is FWHM 3.9GHz
Linac V (MV) j (deg) Acc. Grad. (MV/m)
Mod’s No. Cav’s Spare Cav’s Cavities per Amplifier L0 97 * 14.6 1 8 1 1 L1 235
15.1 2 16 1 ? HL
12 12? L2 1448
15.5 12 96 6 32? L3 2460 15.7 20 160 10 32?
* L0 phases: (-40, -52, 0, 0, 0, 13, 33), with cav-2 at 20% of other L0 cav’s.
Includes 2-km RW wake
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Marc Ross, SLAC LCLS-II September 6, 2013
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TDR coupler
– We recommend to match the coupler to 30 MV/m for reduced filling time and smaller Qext range – Max coupler power at operation 450 kW (for 8.8 mA, 10Hz, Eacc=31.5 MV/m ±20%) – RF processing to at least four times max input power ~ 1.8 MW up to 500 us at test stand TW – Surface field not a problem for both designs, i.e. 40mm and 60mm are both ok – Should check flattop regulation at 25 MV/m and Qext ~ 1e7 (LFD) – TW testing on test stand up to 1.8MW has to be done for both: TTF3 and STF2
– Variable coupling is needed, remote operation – QL tuning range: 2-7x106 is needed, but we recommend 1-10 x 106 – 1-10∙106 is achieved with TTF3 – STF2 has to be improved
– Design should be +-2mm
– For TTF3 coupler the most sensitive parameter is a horizontal antenna shift/tilt. 3mm shift change QL by ~20%. Vertical tolerances are relaxed. – For STF-2 coupler this is not issue, mechanical design guarantee small shift. – TTF3 has to be improved
– Coupler contribution to cryogenic losses at 2K is ~5%. = not critical. – Major contribution from coupler is 70K
– Both designs are ok – The nominal conditioning time of < 50h is achieved/demonstrated.
– DESY and SLAC simulations, tests and operation show no problem with TTF3 – STF2 will be simulated, tests show no problem
– Many single window coupler are successful under operation – The single window would need to seal-off the cavity before the cavity-string installation into the cryomodule. – Single window coupler for ILC would need complete new development and test program of coupler (and module) – But it could be a significant cost saving
– Cavity and attached parts (power coupler, tuner, HOM coupler, feedthroughs, He vessel, thermal connections, magnetic shield…) are tuned/balanced, it is not easy to exchange only parts of this composition – STF2 coupler design does not fit in the compatibility requirements of the TDR (40mm cavity coupler flange)
– CPI: STF2 price is 1.9 higher – Toshiba: STF2 slightly lower price – RI: about same price – Industrial study of STF2 for design optimization and cost reduction is recommended – The TTF3 coupler mass fabrication has to be investigated
in a CM (TTF3 coupler has a long history in FLASH)
the compatible design. The new design has to be proven with beam operation.
spare part concept. We recommend spare modules, not individual parts.
recommended.
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signal Modulation Depth “M”
[rad]
[rad]
2013 IRFU Linear Collider Days
determined by fringe pitch depend on crossing angle θ (and λ )
N: no. of Compton photons Convolution between e- beam profile and fringe intensity
) 2 / sin( 2
y
k d
M d k N N N N
y y y
) cos( ln 2 2 ) ( 2 exp ) cos(
2
s s M
Focused Beam : large M Dilluted Beam : small M
Small σy Large σy
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Crossing angle θ 174° 30° 8° 2°
Fringe pitch
266 nm 1.03 μm 3.81 μm 15.2 μm Lower limit 20 nm 80 nm 350 nm 1.2 μm Upper limit 110 nm 400 nm 1.4 μm 6 μm
) 2 / sin( 2
y
k d
M d
y
) cos( ln 2 2 s
Measures σy* = 20 nm 〜few μm with < 10% resolution
Expected Performance
select appropriate mode according to beam focusing
2013 IRFU Linear Collider Days
σy and M for each θ mode
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174 deg. 30 deg. 2 - 8 deg
Crossing angle continuously adjustable by prism
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1.7 (H) x 1.6 (V) m
path for each θ mode (auto-stages + mirror actuators )
beam pipe Laser transported to IP
delay half mirror
transverse :laser wire scan precise position alignment by remote control
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beforehand …. Construct & confirm laser paths, timing alignment Longitudinal:z scan After all preparations ………. continuously measure σy using fringe scans Feed back to multi-knob tuning laser spot size σt,laser = 15 – 20 μm
12/20 :
1st success in M detection at 174 deg mode
Beam time status in 2012
stable measurements of M 〜 0.55 Feb; 30 deg mode commissioned ( 1st M detection on 2/17)
2013 IRFU Linear Collider Days
σy = 166.2 ± 6.7 (stat) [nm]
ATF2 beam focusing / tuning study
(10 x bx*, 3 x by* optics)
Spring run Major optics reform of 2012 summer Winter run Last 2 days in Dec run Measured many times M = 0.15 – 0.25 (correspond to σy 〜 70 – 82 nm)
Large step towards achieving ATF2 ‘s goal !!
error studies ongoing aimed at deriving “true beamsize”
* IPBSM systematic errors uncorrected ** under low e beam intensity (〜 1E9 e / bunch)
By IPBSM group@KEK
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measured M over continuous reiteration of linear /nonlinear@ tuning knobs @ 174 ° mode
Beam time status in 2013 Spring
2013 IRFU Linear Collider Days
dedicated data for error studies under analysis ex) consecutive 10 fringe scans
Time passed measure M vs time after all conditions optimized
preliminary
Stable IPBSM performance major role in beam tuning
10 x bx*, 1 x by*
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174 ° mode ”consistency scan” moving towards goal of σy = 37 nm : higher IPBSM precision and stability
& looser current limits of normal / skew sextupoles current
correspond to σy 〜 65 nm
Best record
from Okugi-san’s Fri
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