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Comparison between simulations and measurements in the LHC with heavy ions

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Comparison between simulations and measurements in the LHC with heavy ions. T. Mertens , R. Bruce, J.M. Jowett, H. Damerau,F . Roncarolo. Outline. Introduction Comparison of different IBS Models Measured data and simulation input Comparing the simulation with single bunch data - PowerPoint PPT Presentation
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Comparison between simulations and measurements in the LHC with heavy ions T. Mertens, R. Bruce, J.M. Jowett, H. Damerau,F. Roncarolo
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Page 1: Comparison between simulations and measurements in the LHC with heavy ions

Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens,R. Bruce, J.M. Jowett, H. Damerau,F. Roncarolo

Page 2: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 2

Outline

• Introduction• Comparison of different IBS Models• Measured data and simulation input• Comparing the simulation with single bunch data• Comparing the simulation with averaged bunch

data• Side note on Protons• Conclusion and outlook

5/2/2011

Page 3: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 3

Introduction

• Goal is to simulate Ion runs in 2010 during physics

• Different IBS models available• Which fills should we try to simulate? Is all the

necessary data to compare with simulation available?

5/2/2011

Page 4: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 4

Comparison of different IBS Models[1]Model Summary

Model Description

Piwinski Smooth (Piwi) •Uses Piwinski’s formulas as described on page 126 of “The Accelerator Handbook” assuming vertical Dispersion to be zero.•Uses a smooth Lattice approximation

Piwinski Lattice (PiwLat) •Uses Piwinski’s formulas as described on page 126 of “The Accelerator Handbook” assuming vertical Dispersion to be zero.•Uses optical functions in the Lattice elements and sums growth rates over all the elements in the accelerator.

Piwinski Modified Lattice (modPiwLat)

•Uses Piwinski’s formulas as described on page 126 of “The Accelerator Handbook” assuming vertical Dispersion to be zero.•Uses optical functions in the Lattice elements and sums growth rates over all the elements in the accelerator.• Also takes derivatives of the horizontal Beta and horizontal Dispersion into account

Interpolation (Interpolat) Uses tri-linear interpolation on a lattice in an external file. This file can be generated using any IBS model of choice! Here we used a stand-alone software version of the modPiwLat Model to calculate the IBS growth rates on such a lattice.

Bane (Bane) High Energy approximation using Bane’s Approximation Function(Reference : SLAC-PUB-9226 . A simplified Model of Intrabeam Scattering, 2002. Stanford Linear Accelerator Center.)

Nagaitsev (Nagaitsev) Based on Bjorken-Mtingwa but expressed in Carlson’s Elliptic Integrals to calculate the IBS growth rates. Does not take Vertical Dispersion into account.(Reference : S. Nagaitsev. Intrabeam scattering formulas for fast numerical evaluation. Physical Review Special Topics – Accelerators and Beams, 2005. PhysRevSTAB.8.064403.)

5/2/2011

2

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Page 5: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 55/2/2011

Comparison of different IBS Models[2]Simulations Input

1 = Process is on 0 = Process is off

Normalized Emittances

Page 6: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 6

Comparison of different IBS Models[3]

5/2/2011

Coupled = Full coupling between horizontal and vertical plane, growth rate for both planes set equal

yx TTT

11

2

11

Page 7: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 7

Comparison of different IBS Models[4]

5/2/2011

Hor

izont

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rtica

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Page 8: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 8

Comparison of different IBS Models[5]

• Decided to use Nagaitsev• Based on Carlson’s Elliptic Integral (Reference: Numerical recipes in Fortran,

page 1130)

• Does not include Vertical Dispersion• Depends on Coulomb Logarithm, set to 20 for the

simulations here (Reference: S.K. Mtingwa J.D. Bjorken. Intrabeam scattering.

Part. Acc., 13:115–143, 1983)5/2/2011

032

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We hope to get rid of this in the future.

Page 9: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 9

Measured data and simulation input [1]Selecting Ion Fills to Study

• Duration of STABLE beam mode

5/2/2011

Page 10: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 10

Measured data and simulation input [2]Selecting Ion Fills to Study

• All required data available?

5/2/2011

Page 11: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 11

Measured data and simulation input [3]Selecting Ion Fills to Study

Final selection of Fills we simulated

5/2/2011

Fill N bunches Beam 1

N bunches Beam 2

N bunches colliding in ATLAS/CMS

Fill Length in Physics

1494 121 121 113 6.5 h

1504 121 120 112 7.25 h

1511 121 121 113 10 h

1514 121 121 113 6.5 h

Page 12: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 12

Measured data and simulation input [4]

• Single bunch for each beam– Select a bunch in beam 1 and the bunch in beam 2 that collides

with this first bunch in ATLAS/CMS– Extract the data for these 2 bunches– Use data at the beginning of STABLE mode to set initial conditions

for the simulation• Averaged data

– Select the bunches colliding in ATLAS/CMS from beam 1 and beam 2– Extract the data and average it over the selected bunches– Use these averages at the beginning of STABLE mode to set initial

conditions for the simulation5/2/2011

Page 13: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 13

Comparing simulation with single bunch data[1]

Bunch length for bunch 2 Fill 1494

Bunch length for bunch 3Fill 1494

5/2/2011

Page 14: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 14

Comparing simulation with single bunch data[2]

Intensity for bunch 2Fill 1514

Intensity for bunch 4Fill 1514

5/2/2011

Page 15: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 15

Compare simulation with averaged bunch data[1]

Uncorrected data• Luminosity from ATLAS• Luminosity from (just 2 bunches

colliding)

• Bunch length data BQM• Intensity data FBCT• Transverse data from BSRTS

corrected as (F. Roncarolo)

Note : correction factors different in horizontal and vertical plane but the same for all fills

Corrected data

2121

*21

2 yyxx

IIfL

22

cfmeascorr

• Luminosity from ATLAS• Bunch length data BQM• Intensity data FBCT• Transverse data from BSRTS

corrected so that luminosity from ATLAS and simulated luminosity match.

Note: same correction factor used for both planes here (can be improved!) but not the same for all fills -> Fill dependent!

2

2

22

cfcfmeascorr

5/2/2011

Page 16: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 16

Compare simulation with averaged bunch data[2]

ba iiBSRTSLiiATLASL ,_,_

5/2/2011

2

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iBSRTSiBSRTS

iBSRTSL

Careful : sigma's are at ATLAS IP, take Beta’s into account!

Page 17: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 17

Compare simulation with averaged bunch data[3]Determining Averages

• Bunch lengths : all bunches have same timestamp -> just average for each point in time

• FBCT : same procedure as for Bunch Lengths• BSRTS :

– Scans through the bunches : data for different bunches is at different moments in time!

– Create an interpolation function for each bunch – Create a lattice of points in time– Calculate values of interpolation functions on time lattice– Use these values to calculate averages

5/2/2011

Page 18: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 18

Compare simulation with averaged bunch data[4]Determining Averages

5/2/2011

Plots of the BSRTS interpolating functions for some of the bunches

Page 19: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 19

Compare simulation with averaged bunch data[5]Determining Averages

5/2/2011

Plots of the BSRTS interpolating functions for some of the bunches

Page 20: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 20

Compare simulation with averaged bunch data[6]

5/2/2011

Fill 1511

Page 21: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 21

Compare simulation with averaged bunch data[7]Example 1

Uncorrected Corrected

5/2/2011

Page 22: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 22

Compare simulation with averaged bunch data[8]Example 1

Uncorrected Corrected

5/2/2011

Page 23: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 23

Compare simulation with averaged bunch data[9]Example 1

Uncorrected Corrected

5/2/2011

Page 24: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 24

Compare simulation with averaged bunch data[10]

5/2/2011

Fill 1494

Page 25: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 25

Compare simulation with averaged bunch data[11]Example 2

Uncorrected Corrected

ai

5/2/2011

Page 26: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 26

Compare simulation with averaged bunch data[12]Example 2

Uncorrected Corrected

5/2/2011

Page 27: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 27

Compare simulation with averaged bunch data[13]Example 2

Uncorrected Corrected

5/2/2011

Page 28: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 28

Side note on Protons[1]

5/2/2011

• We are planning to use particle tracking to simulate proton runs.

• 2010 : used different approach– Assuming round beams calculate IBS growth rates on a

Lattice (RF Voltage, Longitudinal Emittance, Transverse Emittance) using MAD-X

– Choose initial point (Longitudinal and Transverse emittance)– Use iterative function (NestList command in Mathematica)

Page 29: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 29

Side note on Protons[2]

5/2/2011

Blue curves are the simulations based on the iterative function.

Red curves are ATLAS Luminous Region Data

Page 30: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 30

Side note on Protons[3]

5/2/2011

Blue curves are the simulations based on the iterative function.

Red curves are ATLAS Luminous Region Data

Page 31: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 31

Conclusion and outlook

• Observations of comparison with particle tracking:– Transverse growth underestimated– Bunch length growth overestimated– Both are different expressions of same effect, when simulation would follow the

transverse growth, bunch length would also agree better with data.• Particle Tracking Simulation seems to be missing some effect(s) that

makes transverse emittances grow faster than predicted by our IBS models. (hump?, particularly in vertical plane)

• Same observations can be made for protons.• Would be interesting to do same comparison at injection energy without

beams in collision. But more problems with data at injection : no BSRTS, BGI can not be trusted yet. Usually short periods of time at injection -> not much data available.

• Next step add hump model to simulation (Vertical? Beam 2? )• Try to compare particle tracking simulations for protons.

5/2/2011

Page 32: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 32

Back up

5/2/2011

Page 33: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 33

Correction Factors F. Roncarolo

5/2/2011

Page 34: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 34

Compare simulation with averaged bunch dataExample 3

Uncorrected Corrected

ai

5/2/2011

Page 35: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 35

Compare simulation with averaged bunch dataExample 3

Uncorrected Corrected

5/2/2011

Page 36: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 36

Compare simulation with averaged bunch dataExample 3

Uncorrected Corrected

5/2/2011

Page 37: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 37

Compare simulation with averaged bunch dataExample 4

Uncorrected Corrected

ai

5/2/2011

Page 38: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 38

Compare simulation with averaged bunch dataExample 4

Uncorrected Corrected

5/2/2011

Page 39: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 39

Compare simulation with averaged bunch dataExample 4

Uncorrected Corrected

5/2/2011

Page 40: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 40

Formulas Piwinski

5/2/2011

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Page 41: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 41

Formulas Bane

5/2/2011

Page 42: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 42

Formulas Nagaitsev[1]

5/2/2011

Page 43: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 43

Formulas Nagaitsev[2]

5/2/2011

Page 44: Comparison between simulations and measurements in the LHC with heavy ions

T. Mertens 44

Formulas Nagaitsev[3]

5/2/2011


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