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Halo scraping and loss rates at collimators F. Burkart F. Burkart R. Assmann, R. Bruce, R. Assmann, R. Bruce, M. Cauchi, D. M. Cauchi, D. Deboy, S. Redaelli, A. Rossi, Deboy, S. Redaelli, A. Rossi, G. Valentino, D. G. Valentino, D. Wollmann Wollmann

Halo scraping and loss rates at collimators

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Halo scraping and loss rates at collimators. F. Burkart R. Assmann, R. Bruce, M. Cauchi, D. Deboy, S. Redaelli, A. Rossi, G. Valentino, D. Wollmann. 1. Introduction 2. Halo scraping measurements 3. Results of data analysis from measurements - PowerPoint PPT Presentation

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Page 1: Halo scraping and loss rates at collimators

Halo scraping and loss rates at collimators

F. BurkartF. Burkart R. Assmann, R. Bruce, M. R. Assmann, R. Bruce, M. Cauchi, D. Deboy, S. Cauchi, D. Deboy, S.

Redaelli, A. Rossi, G. Redaelli, A. Rossi, G. Valentino, D. WollmannValentino, D. Wollmann

Page 2: Halo scraping and loss rates at collimators

Outline

Florian Burkart2

1. Introduction

2. Halo scraping measurements

3. Results of data analysis from measurements

4. Collimation losses during high-luminosity fills

5. Results of data analysis from physics fills

6. Conclusion

7. Future work

Page 3: Halo scraping and loss rates at collimators

Why halo scraping?

• Understand population and repopulation speed of the beam halo at 3.5 TeV

→ extrapolate the results to 7 TeV

→ loss rates at collimators

→ minimum instantenious lifetime of the beams

• Calibrate BLM-signal at primary collimator [Gy/s] to a particle lossrate [p/s]

→ compare to losses seen in collimation region during high-luminosity runs

→ distinguish between hor.,ver. and skew losses

Florian Burkart 3

Page 4: Halo scraping and loss rates at collimators

Halo scraping procedure

• Move single jaw of a primary collimator into the beam halo

• with different step sizes (5 micron, 20 micron, 40 micron)

• at different intensities

• in different machine states (injection, collision)

- measure beam intensity (FBCT) → loss rate

- measure BLM-signals

• Most EoF-studies after physics → beam dumped by BLMs

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Page 5: Halo scraping and loss rates at collimators

Usage of different step sizes

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10 μm step size

5 μm step size

Page 6: Halo scraping and loss rates at collimators

BLM-responseScraping with TCP.D B1, running

sum: 1.3 s

6

C-BLM: 8.5E+11 p/Gy

D-BLM: 1.7E+12 p/Gy

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Signal in TCP.C-BLM dominatedby vertical losses

Page 7: Halo scraping and loss rates at collimators

BLM-response for different running sums

Scraping with TCP.D B1

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1.3s: 8.5E+11 p/Gy

10.24ms: 3.4E+12 p/Gy Loss rate diluted in large running sums

Page 8: Halo scraping and loss rates at collimators

Calibration factor Halo scraping

RS09 / RS06

Florian Burkart8

5/1/10 6/20/10 8/9/10 9/28/10 11/17/10 1/6/11 2/25/11 4/16/111.00E+11

6.00E+11

1.10E+12

1.60E+12

2.10E+12

2.60E+12

3.10E+12

3.60E+12

1,3s10,24ms

Date

calib

rati

on

fac

tor

[p/G

y]

Variation up to a factor 6.6 → to be understood → impact parameter → error in lossrate due to 1 Hz FBCT-signal

Page 9: Halo scraping and loss rates at collimators

Overview of different scrapings

9Florian Burkart

ScrapingCollimator

BLM on TCP.C

calibration factor [p/Gy]

1,3serror points

28.05.10 TCP.D6L7.B1 1.9E+11 5.4E+09 4

25.08.10 TCP.D6R7.B2 8.6E+11 4.4E+10 27

04.04.11 TCP.D6L7.B1 1.7E+11 2.8E+10 5

04.04.11 TCP.D6R7.B2 1.3E+11 2.5E+10 6

variation up to a factor 6.6 → not understood

Page 10: Halo scraping and loss rates at collimators

Collimation losses during high-luminosity fills – steady

state

Florian Burkart10

• Measure BLM signals [Gy/s] on Collimators (TCP.C)

• Measure Beam Intensity (FBCT) [p]

→ steady state lossrate [p/s] (dominated by losses at collimators)

→ calibration factor [p/Gy]

Page 11: Halo scraping and loss rates at collimators

Losses with colliding beams Fill 1722, 336 bunches

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Courtesy D.Wollmann

IR7: ~87%

IR8: ~6%

IR3: ~2.5%IR1:

~1%

Linear scale!

Page 12: Halo scraping and loss rates at collimators

Beam Intensity versus time Fill 1749, B1

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Intensity [p]

14 h

Time [s]

7.6*10^13

7.1*10^13

Page 13: Halo scraping and loss rates at collimators

Loss rate versus time Fill 1749, B1, running average

240sec

Florian Burkart13

14 h

Time [s]

Lossrate [p/s]

dN FBCT

dt

4*10^8

1*10^8

Page 14: Halo scraping and loss rates at collimators

BLM-signal versus time Fill 1749, B1

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14 h

Time [s]

BLM-signal [Gy/s]

0.0001

0.0006

Page 15: Halo scraping and loss rates at collimators

Calibration factors(stable beams)

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Average value B1: 2.2E+12 p/Gy B2: 1.54E+12 p/Gy Variation : 6,5 (B1), 3,4 (B2)

17421743174417451746174717481749175017511752175317541755175617571.00E+11

1.00E+12

1.00E+13

Beam1Beam2

fill number

ca

lib

rati

on

fa

cto

r [p

/Gy

]

Page 16: Halo scraping and loss rates at collimators

Minimum Lifetime RS09 (1.3 s)

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17421743

17441745

17461747

17481749

17501751

17521753

17541755

17561757

0

10

20

30

40

50

60

70

Beam1Beam2

fill number

min

. li

feti

me

[h

]

• 624 b, 768 b

min=3h

=N FBCT

RBLM

Page 17: Halo scraping and loss rates at collimators

Comparison Min.Lifetime B1 RS09, RS06

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17421743

17441745

17461747

17481749

17501751

17521753

17541755

17561757

0

5

10

15

20

25

fill number

min

. li

feti

me

[h

]

Min. Lifetime for multiturn losses → RS06

Page 18: Halo scraping and loss rates at collimators

Comparison Min.Lifetime B2 RS09, RS06

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17421743174417451746174717481749175017511752175317541755175617570

10

20

30

40

50

60

70

RS06 Beam2RS09 Beam2

fill number

min

. li

feti

me

[h

]

Page 19: Halo scraping and loss rates at collimators

Overview of physics fills RS09

Florian Burkart19

Fill numb

er

#bunch

e

calibration factor

B1 [p/Gy]

calibration factor

B2 [p/Gy]Peak loss B1 [p/s]

Peak loss B2 [p/s]

min lifetime B1 [h]

min lifetime B2 [h]

1743 624 3.2E+12 2.2E+12 3,28E+09

1,45E+09 6,50 14,40

1744 624 2.4E+12 1.3E+12 6,90E+09

1,02E+09 3,00 20,11

1748 624 1.8E+12 9.3E+11 2.26E09 1.73E+09 9,40 12,10

1749 624 3.0E+12 2.2E+12 7.1E+09 9.6E+08 3,00 21,20

1753 768 1.38E+12

1.52E+12 7.2E+09 9.5E+08 3,60 27,00

1755 768 1.9E+12 1.99E+12

1.49E+09 4.56E+9 18,40 58,90

1756 768 4.86E+11

6.29E+11 1.13E+9 1.6E+09 23,50 22,30

Page 20: Halo scraping and loss rates at collimators

Overview of physics fills RS06

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Fill number

#bunche

calibration factor B1

[p/Gy]

calibration factor B2

[p/Gy]Peak loss B1 [p/s]

Peak loss B2 [p/s]

min lifetime B1 [h]

min lifetime B2 [h]

1743 624 2,40E+12 1,68E+12 6,80E+09 2,74E+09 3,12 7,361744 624 1,82E+12 9,40E+11 1,57E+10 1,70E+09 1,33 11,901748 624 1,27E+12 6,23E+11 3,30E+09 2,17E+09 6,40 9,601749 624 2,09E+12 1,51E+12 1,02E+10 1,65E+10 2,09 1,151753 768 7,80E+11 1,17E+12 1,39E+10 4,00E+09 1,90 6,271755 768 1,37E+12 1,47E+12 2,76E+09 1,14E+09 9,96 23,401756 768 6,42E+11 4,20E+11 1,70E+09 4,20E+09 15,30 6,20

Courtesy D.Wollmann

Page 21: Halo scraping and loss rates at collimators

Conclusion

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Halo scrapings

• For vertical losses BLM at TCP.C shows highest signal

• More scraping experiments needed

• More usable data points per experiment → sufficient loss rate

• Variation of calibration factors (~ 6.6)

Physics fills

• Losses mainly appear at collimators (IR7: ~87%)

• Average calibration factor B1: 2.2E+12 p/Gy

• Average calibration factor B2: 1.54E+12 p/Gy

• Min. Lifetime B1 > 1.3 h (RS06)

• Min. Lifetime B2 > 1.15 h (RS06)

Page 22: Halo scraping and loss rates at collimators

Future work

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• Analysis of other integration times

• Analysis of other BLM-signals e.g. TCHSV (physics fills data, scraping data)

• More scrapings with different step sizes → understand variation of calibration factor

• Scrapings with different optics (squeezed, collision)

• Measure repopulation speed

Page 23: Halo scraping and loss rates at collimators

END

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Thank you for your attention!