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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


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SLIDE 1

ILC Accelerator Activities in North America (cooperation with France)

Presentation at IRFU Linear Collider Days prepared by:

Marc Ross (SLAC) November 29, 2013

1

2013 IRFU Linear Collider Days

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SLIDE 2
  • TDP Goals:

» R & D to enable Project Proposal and updated Value estimate –

with Cost Containment

» SC RF Technology Transfer

  • development of a strong industrial base
  • Technical Design Report:

» Consists of two parts: 1) R & D Report and 2) Design Description

  • Beam Test Facilities:

» SRF Linac: Fermilab NML, DESY E-XFEL and FLASH, KEK STF » Beam Dynamics: Cornell CesrTA (2008 – 2010) » Beam Tuning: KEK ATF2

  • Production / Industrialization:

» CEBAF Upgrade and E-XFEL

2 2013 IRFU Linear Collider Days

Completing the ILC Technical Design Phase January 2013

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SLIDE 3

3 2013 IRFU Linear Collider Days

Completing the TDP: Outline

  • TDP Goals:

» R & D to enable Project Proposal and updated Value estimate –

with Cost Containment

» SC RF Technology Transfer

  • development of a strong industrial base
  • Technical Design Report:

» Consists of two parts: 1) R & D Report and 2) Design Description

  • Beam Test Facilities:

» SRF Linac: Fermilab NML, DESY E-XFEL and FLASH, KEK STF » Beam Dynamics: Cornell CesrTA (2008 – 2010) » Beam Tuning: KEK ATF2

  • Production / Industrialization:

» CEBAF Upgrade and E-XFEL

Present

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SLIDE 4
  • SC RF Technology Transfer

» Development of a strong industrial base

  • Production / Industrialization:

» CEBAF Upgrade and E-XFEL

  • Beam Test Facilities:

» SRF Linac: Fermilab NML, DESY E-XFEL and FLASH, KEK STF » Beam Dynamics: Cornell CesrTA (2008 – 2010) » Beam Tuning: KEK ATF2

  • US contribution to ‘Linear Collider Collaboration’ (LCC)
  • ‘P5’ prioritization activity

4 2013 IRFU Linear Collider Days

ILC Accelerator Activities: Outline

By the end of the XFEL Production > 1000 cavities will have been fabricated by industry and processed using the basic TESLA – recipe.

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SLIDE 5
  • Cavity production lines fully functioning: 8 cavities / week

» Two companies

  • Cryomodule production:
  • Three pre-series CM (XM-3, XM-2, XM-1) in process; typical

time to construct 4 months; time to test unknown

  • Production series of 81 each started Sep. 02, 2013;
  • One CM / week nominal; one production line (CEA-Saclay)
  • 24 cavities to be used for high – gradient development

» (See E. Elsen)

5 2013 IRFU Linear Collider Days

EU - XFEL

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SLIDE 6

6 'BB Lunch', M. Ross (SLAC)

Jefferson Lab CEBAF 12 GeV Upgrade

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SLIDE 7

7 'BB Lunch', M. Ross (SLAC)

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SLIDE 8

8 'BB Lunch', M. Ross (SLAC)

Slide dated late 09.2013 All C100 cryomodules are now installed (11.2013)

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SLIDE 9

9 'BB Lunch', M. Ross (SLAC)

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  • Following BESAC (Basic Energy Sciences Advisory) report

in late July 2013:

» Shakeup of US accelerator construction projects: » SLAC LCLS-II project redefined » ANL APS upgrade program redefined

  • SLAC Proposal:

» 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

10 2013 IRFU Linear Collider Days

SLAC Proposal:

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SLIDE 11

11

SLAC Director Chi-Chang Kao, 27 September 2013:

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12

Chi-Chang Kao, 27 September 2013:

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LCLS-II and ILC Much LCLS-II construction will be done at Fermilab, using infrastructure intended for ILC 18 CM? (50%) Other CM to be made at JLab (and Cornell) Saclay CM assembly industrial experience unique US team have made ~ two ILC CM. LCLS-II effort will help understand US-domestic technical, cost, and industrialization

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RF Parameters:

2013 IRFU Linear Collider Days

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RF Parameters (2)

2013 IRFU Linear Collider Days

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LCLS-II - Linac and Compressor Layout for 4 GeV

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)

  • No. Cryo

Mod’s No. Cav’s Spare Cav’s Cavities per Amplifier L0 97 * 14.6 1 8 1 1 L1 235

  • 26

15.1 2 16 1 ? HL

  • 40
  • 170
  • 3 (3.9GHz)

12 12? L2 1448

  • 28

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

2013 IRFU Linear Collider Days 16

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17

First 800 m of SLAC linac (1964):

Marc Ross, SLAC LCLS-II September 6, 2013

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SLIDE 18

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ILC R & D initiative: Power Coupler development Mandated by PAC (12.2012) technical review Common activity with Orsay /LAL Issues:

  • Cost
  • Copper coating / flaking
  • Complex Assembly
  • Plug-compatibility
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SLIDE 19

TTF3/XFEL coupler STF-2 coupler

TDR coupler

(1) Deep Technical Review of Input Couplers

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SLIDE 20

ILC specification

  • Power requirements

– 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

  • Q-ext

– 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

  • Antenna alignment:

– 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

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SLIDE 21
  • Cryogenic loss:

– Coupler contribution to cryogenic losses at 2K is ~5%. = not critical. – Major contribution from coupler is 70K

  • Conditioning time

– Both designs are ok – The nominal conditioning time of < 50h is achieved/demonstrated.

  • Multipacting

– DESY and SLAC simulations, tests and operation show no problem with TTF3 – STF2 will be simulated, tests show no problem

  • One vs. two windows

– 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

  • Compatibility

– 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)

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SLIDE 22
  • Cost

– 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

Recommendation:

  • STF2 coupler has to demonstrate stable long time (>6 month) beam operation

in a CM (TTF3 coupler has a long history in FLASH)

  • The ILC management recommend an adapted STF2 design with 40mm cavity
  • flange. In this case more development steps have to follow in order to realize

the compatible design. The new design has to be proven with beam operation.

  • The concept of plug compatibility has to be further developed in view of a

spare part concept. We recommend spare modules, not individual parts.

  • An industrial study of mass production for both designs is recommended
  • Industrial study of STF2 for design optimization and cost reduction is

recommended.

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SLIDE 23

ATF2 Program Status

Glen White, SLAC January 2013

2013 IRFU Linear Collider Days 23

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SLIDE 24

Detector measures

signal Modulation Depth “M”

N + N -

[rad]

[rad]

2013 IRFU Linear Collider Days

measurable range

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

13/05/29 24

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SLIDE 25

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

13/05/29 25

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174 deg. 30 deg. 2 - 8 deg

Crossing angle continuously adjustable by prism

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Vertical table

1.7 (H) x 1.6 (V) m

  • Interferometer
  • Phase control (piezo stage)

path for each θ mode (auto-stages + mirror actuators )

beam pipe Laser transported to IP

  • ptical

delay half mirror

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SLIDE 27

transverse :laser wire scan precise position alignment by remote control

2013 IRFU Linear Collider Days

Role of IPBSM in Beam Tuning

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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

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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

M = 0.52 ± 0.02 (stat)

σy = 166.2 ± 6.7 (stat) [nm]

  • 2 - 8 ° mode: clear contrast (Mmeas ~0.9)
  • Prepared 174 deg mode commissioning
  • Suppress systematic errors
  • Higher laser path stability / reliability
  • High M measured at 30 ° mode
  • Contribute with stable operation to

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”

preliminary preliminary

* IPBSM systematic errors uncorrected ** under low e beam intensity (〜 1E9 e / bunch)

10 x βx* , 1 x βy*

By IPBSM group@KEK

13/05/29 28

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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

preliminary

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

M 〜 0.306 ± 0.043 (RMS)

correspond to σy 〜 65 nm

Best record

from Okugi-san’s Fri

  • peration meeting slides
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The Reality… May 2 week Cont. Run

  • Summary of all scans during 2 week ops period

– Summary plot courtesy of Edu.

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