Production of bunch doublets for scrubbing of the LHC

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Production of bunch doublets for scrubbing of the LHC J. Esteban Muller (simulations), E. Shaposhnikova 3 December 2013 LBOC Thanks to H. Bartosik, T. Bohl, G. Iadarola, W. Hofle, G. Rumolo For LLRF and ADT compatibility see talks of P. Baudrenghien and G. Kotzian at the last LBOC

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Production of bunch doublets for scrubbing of the LHC . J. Esteban Muller (simulations ), E . Shaposhnikova 3 December 2013 LBOC Thanks to H. Bartosik, T. Bohl, G. Iadarola , W. Hofle, G . Rumolo For LLRF and ADT compatibility see talks - PowerPoint PPT Presentation

Transcript of Production of bunch doublets for scrubbing of the LHC

Page 1: Production of bunch doublets for scrubbing of the LHC

Production of bunch doubletsfor scrubbing of the LHC

J. Esteban Muller (simulations), E. Shaposhnikova3 December 2013 LBOC

Thanks to H. Bartosik, T. Bohl, G. Iadarola, W. Hofle, G. Rumolo

For LLRF and ADT compatibility see talks of P. Baudrenghien and G. Kotzian at the last LBOC

Page 2: Production of bunch doublets for scrubbing of the LHC

Method of bunch splitting into two bunchlets

1. Reduce voltage to minimum possible amplitude (limited by intensity effects) to reduce longitudinal emittance blow-up and uncaptured beam.

2. Jump RF phase by 180 deg (to unstable phase).3. Wait till uncaptured particle will move ½ of RF period and increase

sharply voltage to an amplitude sufficient to recapture particles lost from the bunch center.

Low voltage Jump to unstable phase Wait Voltage increase Buckets are filled

Page 3: Production of bunch doublets for scrubbing of the LHC

Different options for bunch splitting

1) Bunch splitting in the LHC => 2.5 ns doublets2) Bunch splitting in the SPS => 5.0 ns doublets.

The latter can be done ata) injectionb) flat bottomc) flat topd) intermediate flat portion (~200 GeV)

Page 4: Production of bunch doublets for scrubbing of the LHC

Main issues for all options

• Acceleration in the SPS– high intensity required for efficient scrubbing

(>1.5x1011/bunch, 25 ns spacing) 200 MHz beam loading => slow cycle, but still limited

– Beam control of this beam structure• Splitting– longitudinal emittance blow-up – particle losses – beam stability: unstable phase, 800 MHz?– no HW available (even for the tests)

Page 5: Production of bunch doublets for scrubbing of the LHC

Splitting in LHC: preliminary results• Voltage program:

– SPS before extraction: 2 MV– Injection: 3 MV 6 MV

• Emittance blow-up: 0.5-> 1.02 eVs• Particle loss

– During splitting: ~1%– But due to subsequent voltage

reduction during one following injection: ~15%

– 10% total loss measured in SPS at beginning of ramp (1 dip)

=> Voltage program could be optimized to minimize particle loss:- 1st injection: 3 MV 4 MV (~7% losses), 2nd injection: 4MV 5 MV, …=> LLRF probably can reduce voltage only for injecting beam…

Page 6: Production of bunch doublets for scrubbing of the LHC

Splitting in LHC

Advantages• Issues with doublets only in

LHC, at the last stage• Less problems with

injection into LHC• Sufficient RF voltage/bucket

in LHC

Disadvantages• Doublet spacing 2.5 ns is

much less interesting for scrubbing (Giovanni)

• Losses in LHC during splitting

• Losses during RF manipulations with following SPS injections

Page 7: Production of bunch doublets for scrubbing of the LHC

Splitting in SPS: at injection• Voltage program (same as in

measurements) :– at injection:

1 MV 3 MV• Emittance from 0.56 eVs to 0.31

eVs in each bunchlet• Particle loss during splitting ~1% +

6% to satellites

• More losses should be expected during subsequent injections (3 dips more) due to full bucket

• For splitting at the end of flat bottom results will not be so good

Page 8: Production of bunch doublets for scrubbing of the LHC

Splitting in SPS: at injection

Advantages• Long bunches from PS ->

very small emittance blow-up

• Doesn’t require RF phase jump (new HW)

• Already tested in the SPS• Losses at lower energy• Doesn’t need additional flat

top in magnetic cycle

Disadvantages• E-cloud in the SPS • Losses during voltage

reduction during the subsequent PS injections(was not observed?)

Page 9: Production of bunch doublets for scrubbing of the LHC

Splitting in SPS: flat top• Emittance blow-up:

– from 0.5 eVs to 1.76 eVs• Particle loss

– During splitting: ~5%– LHC injection: ~30%

• Voltage program:– During splitting: 2 MV 4MV– Extraction at 7 MV– LHC injection: 6 MV

• Total time needed ~ 0.1 s• LHC buckets filled with this intensity

distribution (3 satellites):3.5% - 43% - 7% - 43% -3.5%

• Triplet in case of lower voltage at extraction in the SPS and less losses

• Very small final intensity

Page 10: Production of bunch doublets for scrubbing of the LHC

Splitting in SPS: flat top

Advantages• Issues with doublets only on

flat top, at the last stage• Less problems with

injection into LHC• Sufficient RF voltage/bucket

in LHC

Disadvantages• Losses at high energy in SPS• Extraction of uncaptured beam

to LHC• Minimum voltage during

splitting limited by beam loading => large emittance blow-up

• Full SPS bucket after splitting => long bunches– Losses at injection into LHC– Satellite bunches in the LHC=> Less favorable scenario

Page 11: Production of bunch doublets for scrubbing of the LHC

Splitting in SPS: flat portion• Voltage program:

– During splitting (200 GeV):1 MV 2MV

– Extraction to LHC: 7 MV– LHC injection: 6 MV

• Emittance blow-up:– from 0.35 eVs to 0.82 eVs

• Particle losses– During splitting ~7 %– LHC injection < 2%

• No satellites in LHC (&SPS)• Total time needed ~ 0.1s + even

slower ramp

Page 12: Production of bunch doublets for scrubbing of the LHC

Power limitation during cycle

• Similar limitations for

0.4 eVs and 0.8 eVs bunches above 300 GeV

• Intensity limited to 1.5x1011/bunch

Page 13: Production of bunch doublets for scrubbing of the LHC

Splitting in SPS: flat portion

Advantages• Emittance blow-up required

for beam stability > 200 GeV• More bucket area available

in the 2nd part of the ramp• Uncaptured beam is not

injected into LHC

Disadvantages• Acceleration of the large

emittance => beam loading limitation to the total intensity

• More complicated magnetic cycle with additional flat portion

• Losses at relatively high energy in SPS

=> Better scenario than splitting at the flat top or LHC injection

Page 14: Production of bunch doublets for scrubbing of the LHC

Conclusion• Main limitations are expected to be from high intensity (beam loading)

and beam losses (full bucket after splitting)• Splitting at SPS injection seems to be the most feasible scenario: minimum

emittance blow-up. Can be used after efficient scrubbing of the SPS (1-2 weeks)?

• Intermediate flat portion seems to be the 2nd interesting option (if splitting at SPS injection is rejected due to e-cloud)

• Need more detailed simulations (no intensity effects included)• Need new hardware • Need to be tested in MDs• Acceleration of high intensity 25 ns beam in the SPS will be itself very

challenging task