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Feng Zhou Thank Brachmann, Decker, Ding, Huang, Loos, Raubenheimer, Turner et al for the contributions March 6, 2013 Recent LCLS injector studies & plans

Recent LCLS injector studies & plans

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Recent LCLS injector studies & plans. Feng Zhou Thank Brachmann, Decker, Ding, Huang, Loos, Raubenheimer, Turner et al for the contributions March 6, 2013. C ontents. Collimator as an aperture to reduce emittance New applications of a collimator located in BCs: - PowerPoint PPT Presentation

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Page 1: Recent LCLS injector studies & plans

Feng Zhou

Thank Brachmann, Decker, Ding, Huang, Loos, Raubenheimer, Turner et al for the contributions

March 6, 2013

Recent LCLS injector studies & plans

Page 2: Recent LCLS injector studies & plans

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Contents

• Collimator as an aperture to reduce emittance• New applications of a collimator located in BCs:

- For slice emittance measurements- Trace back OTR2 emittance issue- Shorter x-ray FEL production (planning)

• Thoughts of future R&D programs at ASTA and LCLS injector

Page 3: Recent LCLS injector studies & plans

Collimator used to reduce emittance

• Placed collimator in a non-dispersion area: to collimate beam size

• Expected 40% emittance reduction with one circular collimator

• Collimator wakefield is of the major concern

40% reduction

Page 4: Recent LCLS injector studies & plans

Observed wake effect for a smaller gap

x~250um (Aug2, 2012)x~130um (Sep26, 2012)

• Analytical shows circular collimator has much lower wake effect than the flat one (Bane/Stupakov)

• Wake simulation for flat and circular collimator is underway (Li/Xiao)

• Design/fabricate a

circular collimator and test it at the LCLS injector CY14 IF simulations confirm the circular one to be good.

Page 5: Recent LCLS injector studies & plans

Collimator used to measure slice emittance

Chirp

ed

beam

Chirped beam length 11mm

Page 6: Recent LCLS injector studies & plans

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BC1 emittance vs. collimator gap

• Evaluate side effects: space charge (x/y), collimator wakefield (x, y?), CSR and dispersion (x)

• Model/data show negligible collimator wake effect (Bane)

• Y-data/model show negligible space charge effect

• X-dispersion slightly leaks out

• Can y-emittance represent BC1 slice emittance?

Page 7: Recent LCLS injector studies & plans

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Dependence of X-band cavity offset?

• Slice emittance is independence of X-band cavity transverse offset – easier to understand.

Page 8: Recent LCLS injector studies & plans

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BC1 slice x/y emittances (150pC)

• BC1 slice y-emittance is ~0.45um with routine laser profile. • BC1 slice x-emittance is slightly larger due to the leaked-out

dispersion• How to compare with LCLS injector OTR2 emittance?

Page 9: Recent LCLS injector studies & plans

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OTR2/WS2 emittance comparison (150pC)

• During routine operation, what is the LCLS injector realistic emittance?

• OTR2 vs. WS2, LH chicane ON vs. OFF

Page 10: Recent LCLS injector studies & plans

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Area counts comparison (OTR2/WS2)

• Obviously, notable lights from the LH chicane are added to the OTR2 profile, which make OTR2 emittance data deviate from the reality.

Page 11: Recent LCLS injector studies & plans

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OTR2 slice emittance comparisons

• OTR2 slice emittance with chicane-off is similar to BC1 slice emittance – data from routine operation (150pC)

Page 12: Recent LCLS injector studies & plans

12Deep Science Mining for Matter

During our taking data

More typical laser for operations

Page 13: Recent LCLS injector studies & plans

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Discussions on OTR2/BC1 emittances

• OTR2 emittance with LH chicane-on under-estimates the injector emittance:

- Additional lights from the LH chicane modify the OTR2 beam profiles - OTR2 with LH chicane-on may not provide absolute emittance value, but the

emittance trend

• Bunch length with LH chicane-on is 10% shorter than chicane-off – probably the additional lights impact the data.

• With a routine laser profile, slice emittance at OTR2/WS2 and BC1 is ~0.45um for 150pC;

- Plan to measure 250pC.

• BC1 collimator used to measure slice emittance has been validated – the technique is reliable to measure slice beam.

• BC2 slice emittance measurements (planning)

Page 14: Recent LCLS injector studies & plans

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Shorter x-ray FEL production (planning)

ftx

FWHMxt ,

Rms beam size at the collimator

Final bunch length after the chicane (collimator out)

Collimator gap

• To compare with slotted foil (BC2): better or cleaner FEL background? Plan to do MD.

• Lanfa helps us to check simulations

Page 15: Recent LCLS injector studies & plans

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Possible to reduce LCLS emittance

• Lengthen laser pulse to reduce space charge and use smaller laser size: improved slice emittance but projected emittance may be slightly worse (RF emittance).

• September 2011 data: different laser pulse length (2.4-4.4ps) but with same laser size on the cathode (250pC) September 2011 data

Page 16: Recent LCLS injector studies & plans

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Further test at LCLS injector with longer laser pulse (CY14)

Projected emittance

• Simulations show that slice emittance is reduced by 30% with 7ps laser pulse with laser size of 0.8mm, against current 3ps with optimum 1mm of laser size (250pC) – may be tested CY14

simulations

Page 17: Recent LCLS injector studies & plans

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Thoughts of ASTA R&D programs

1. Robust laser cleaning (very near-term, CY13)

2. Upgrade RF gun & laser for 360Hz operations - Address gun heating issues for 360Hz- Upgrade laser for 360Hz operation, and MOD/klystron

3. Develop a load-lock system and higher QE (>5%) cathodes (e.g., Cs2Te):

- May reduce thermal emittance to zero- Operate cathode with 360Hz and/or multi-bunch operations - Significantly simplify laser systems (remove 4-pass MPA)- Greatly improve laser profiles thus the emittance and µBI- Great benefit for FACET-II 3-5nC RF gun operation

They are fully aligned with future LCLS demands