mice beam loss vs particle rate

14
MICE Beam Loss vs Particle Rate Adam Dobbs, ISIS Meeting, 18 th December 2009

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MICE Beam Loss vs Particle Rate. Adam Dobbs, ISIS Meeting, 18 th December 2009. Outline. Current Beamline Analysis Procedure Latest High Beam Loss (~5V) results Future Plans. Current MICE beamline. D = Dipole bending magnet Q = Quadrupole magnet - PowerPoint PPT Presentation

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Page 1: MICE Beam Loss  vs  Particle Rate

MICE Beam Loss vs Particle Rate

Adam Dobbs, ISIS Meeting, 18th December 2009

Page 2: MICE Beam Loss  vs  Particle Rate

2

Outline Current Beamline Analysis Procedure Latest High Beam Loss (~5V) results Future Plans

18/12/2009A Dobbs

Page 3: MICE Beam Loss  vs  Particle Rate

3

Current MICE beamline

18/12/2009A Dobbs

Target

Q1-3

D1 D2 Q4-6 Q7-9

DS

CKOV A, BGVA1

BM1 TOF0

BM2

TOF1

D = Dipole bending magnet Q = Quadrupole magnetDS = Decay solenoid DSA = Decay Solenoid Are a GVA1 = Scintillator counter CKOV = Cherenkov detector BM = Beam Profile Monitor TOF = Time of Flight

ISIS

DSA MICE Hall

Page 4: MICE Beam Loss  vs  Particle Rate

4

Beam Loss vs Particle Rate Flow Diagram

18/12/2009A Dobbs

Target DAQ data DATE DAQ data

Data Reduction 1 – fitted peak beam loss analysis, etc

Particle rate data extraction with ScalersAnalysis

Reduced Beam Loss data

Particle Rate data

Combine data by matching time stamps

Combined data (ROOT files)

Data reduction 2: extract means and sigmas for variables on a run-by-run basis

Final plots of beam loss vs particle rate

Page 5: MICE Beam Loss  vs  Particle Rate

5

Results

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 50

500,000

1,000,000

1,500,000

2,000,000

2,500,000

3,000,000

3,500,000

GVA1 vs Sector 7 Fit Beam Loss

Magnitude of Sector 7 Fit Beam Loss (V)

Aver

age

GVA

1 du

ring

spi

ll ga

te (

coun

ts /

sec)

18/12/2009A Dobbs

One point = the mean values of the beam loss and particle rate for a run

Page 6: MICE Beam Loss  vs  Particle Rate

6 18/12/2009A Dobbs

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 50

200,000

400,000

600,000

800,000

1,000,000

1,200,000

1,400,000

1,600,000

1,800,000

BPM1 vs Sector 7 Fit Beam Loss

Magnitude of Sector 7 Fit Beam Loss (V)

Aver

age

BPM

1 du

ring

spill

gat

e (c

ount

s / se

c)

Page 7: MICE Beam Loss  vs  Particle Rate

7 18/12/2009A Dobbs

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 50

200,000

400,000

600,000

800,000

1,000,000

1,200,000

BPM2 vs Sector 7 Fit Beam Loss

Magnitude of Sector 7 Fit Beam Loss (V)

Aver

age

BPM

2 du

ring

spill

gat

e (c

ount

s / se

c)

Page 8: MICE Beam Loss  vs  Particle Rate

8

Future Plans

18/12/2009A Dobbs

Another high beam loss study planned for December machine physics period Reproducibility Better statistics (400 – 500 pulses per setting)

Use ToF data Another rate counter PID

Compare with G4BeamLine simulations

Page 9: MICE Beam Loss  vs  Particle Rate

9

Preliminary ToF Data for Run 1231

18/12/2009A Dobbs

Produced using G4MICE/TofMonitor

e µ π

Page 10: MICE Beam Loss  vs  Particle Rate

10

Analysis Procedure Step I.I – Beam Loss

18/12/2009A Dobbs

Initially for each target dip a whole spectrum of data is present for each variable (black sample spectra shown above). Canonical single values for each variable are calculated from the spectra using BLA Part 2 to given one value for each variable per target dip (fits doing this shown in red). These are written to an ascii file.

Target DAQ data

Reduced Beam Loss data

Page 11: MICE Beam Loss  vs  Particle Rate

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Analysis Procedure Step I.II- Particle Rate Held in DATE data stream i.e. in

binary Contains GVA1, BM1, BM2, various

TOF0 and TOF1 data Extracted using a modified version of

G4MICE ScalersAnalysis application Output is an ascii file containing the

number of hits for each detector per spill (i.e. per target dip)

TOF data harder to interpret

18/12/2009A Dobbs

DATE DAQ data

Particle Rate data

Page 12: MICE Beam Loss  vs  Particle Rate

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Analysis Procedure Step II- Combine the data Once the beam loss and particle rate data has been

converted to ascii files containing values for each target dip, the data from the two streams must be combined

Data are synchronised using timestamps associated with each target dip data set (the clocks of the two DAQs are synched)

-> Leads to combined data set holding both beam loss and particle rate data per target dip

18/12/2009A Dobbs

Reduced Beam Loss data Particle Rate data

Combined data (ROOT files)

Page 13: MICE Beam Loss  vs  Particle Rate

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Analysis Procedure Step III- extract mean values per run and plot A combined data file is produced for

each run This file is processed using ROOT to

calculate the mean and sigma of each value for a run (a second data reduction) e.g. the mean of GVA1, the mean summed beam loss in sector 7

The values are finally plotted for a series of runs, each having a different nominal beam loss value, but with all other parameters (e.g. Optics) held constant

18/12/2009A Dobbs

Combined data (ROOT

files)

Final plots of beam loss vs particle rate

Page 14: MICE Beam Loss  vs  Particle Rate

14

Histogramme of GVA1 rate per target dip, for run 1231

18/12/2009A Dobbs

One of the better fits!