Beam losses through the cycle
- G. Papotti,
- A. Gorzawski, M. Hostettler, R. Schmidt
LHC Beam Operation workshop - Evian 2012
Beam losses through the cycle G. Papotti, A. Gorzawski, M. - - PowerPoint PPT Presentation
LHC Beam Operation workshop - Evian 2012 Beam losses through the cycle G. Papotti, A. Gorzawski, M. Hostettler, R. Schmidt outline motivation 2011 vs 2012, PM browser module beam losses per beam mode capture, ramp, flat top,
LHC Beam Operation workshop - Evian 2012
– 2011 vs 2012, PM browser module
– capture, ramp, flat top, squeeze, …
– thanks to A. Gorzawski for a lot of data, analysis and plots
– appetizers on instabilities – bunch-by-bunch losses in stable beams and burn off
– give only overview of the year, no details on fill to fill differences – injection not treated
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– e.g. LHC3, 72 bunches
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– 0.45 TeV to 0.5 TeV – 0.5 TeV to 4 TeV
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2011 ¡ 2012 ¡
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– based on sliding window (e.g. 5s, 20s, 80s)
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P = n2 − n1 t2 − t1 E1e11p@ 4TeV
2 ¡ 1 ¡
– beam 1: ~96.2% – beam 2: ~95.3%
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– from end of injection to start of stable beams
– second not so much
– enhanced satellites? (Q20? batch-by-batch blow-up was often off) energy ¡matching ¡
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MD3 ¡
– when had the higher losses at capture? – Q20 and smaller emittances?
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TS3 ¡
– ramp function: 770s long
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– slightly worsened after octupole polarity change
MO ¡polarity ¡change ¡
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– very reproducible for beam 1, but at different times – at precise times for beam 2 MO ¡polarity ¡change ¡
19 Dec 2012 16 giulia.papotti@cern.ch 930s (sq. function = 925s long) 820s (β*~0.8-0.7m) 420s (β*~3m)
– very reproducible losses and max power loss
split ¡coll ¡beam ¡process ¡
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– shift crews used to say: “b2 loses earlier in cycle, b1 loses at start of stable beams” split ¡coll ¡beam ¡process ¡
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– preliminary analysis, more time required
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?. ¡Q’/MO ¡reducAon ¡incorporated ¡ in ¡collapse ¡funcAon ¡ 1 ¡ ? ¡ 2 ¡ ? ¡ 3 ¡ 3 ¡ 1 ¡
not ¡bunch-‑by-‑bunch! ¡
500 1000 1500 2000 2500 3000 3500 2 2.5 3 3.5 4 Bunch number Lumi Emittance [um] 2500 2600 2700 2800 2900 3000 3100 3200 3300 3400 200 400 600 800 1000 Fill number Blownup bunch count
– emittance from luminosity
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MO ¡polarity ¡change ¡ Q20 ¡& ¡split ¡coll ¡beam ¡process ¡
– more analysis required
Time in SB [h] Bunch Length [ns] Bunch length histogram evolution, Fill 3287 1 2 3 4 5 6 7 1.1 1.2 1.3 1.4 1.5
– build up during stable beams in beam 1 – no visible effect on beam 2 – for fills with selective transverse emittance blow-up
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Lumi Emittance [um] Bunch length [ns] Emittance vs. Length, 7h SB, Fill 3287 3 3.5 4 4.5 1.1 1.15 1.2 1.25 1.3 1.35 1.4 Time in SB [h] Emittance [um] Emittance histogram evolution, Fill 3287 1 2 3 4 5 6 7 2 2.5 3 3.5 4 4.5
– very reproducible, also there in 2011 – no correlation with number of long- range interactions – not visible on beam 2 (or smaller?)
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500 1000 1500 2000 2500 3000 3500 0.15 0.2 0.25 0.3 0.35 0.4 Beam 1 losses: Fill 3363, 10.0h SB Slot Number
500 1000 1500 2000 2500 3000 3500 0.15 0.2 0.25 0.3 0.35 0.4 Beam 2 losses: Fill 3363, 10.0h SB Slot Number
20 40 60 80 100 120 140 0.2 0.225 0.25 0.275 0.3 0.325 0.35 Bunch loss B1, Fill 3363 Offset in 144 bunch train Intensity loss in SB [1]
– after removing burn-off component from total losses (σproc = 101.8 mb) – particularly strong on b1
19 Dec 2012 25 giulia.papotti@cern.ch collisions ¡in ¡ IP ¡8 ¡15 ¡158 ¡
25 ¡ns ¡slot ¡
beam ¡1 ¡ beam ¡2 ¡
– capture (degradation towards the end possibly related to enhanced satellites?) – ramp: ~1% towards the end – squeeze: peak losses at precise moments for beam 2 – adjust: split collision beam process improved the reproducibility – stable beams
transverse emittance blow up
– stronger on beam 1
– more useful than end-of-the-year overview!
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2500 2600 2700 2800 2900 3000 3100 3200 3300 3400 0.1 0.15 0.2 0.25 0.3 0.35 Losses in 8h of SB [1]
2500 2600 2700 2800 2900 3000 3100 3200 3300 3400 1.2 1.4 1.6 1.8 2 x 10
14
Intensity at start of SB [p] 2500 2600 2700 2800 2900 3000 3100 3200 3300 3400 3 4 5 6 7 x 10
7
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