Test and Energy measurement with the LEP Spectrometer - PowerPoint PPT Presentation

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Test and Energy measurement with the LEP Spectrometer

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2. Tunnel Test of BPM Electronic (Temperature, Stability... CONSISTENCE IN THE RESULTS. 7th December. E.Barbero - BI day 2000. 16. Environmental magnetic field ... – PowerPoint PPT presentation

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Title: Test and Energy measurement with the LEP Spectrometer


1
Test and Energy measurement with the LEP
Spectrometer
  • E.Barbero - SL/BI/SD
  • 1. Laboratory test of BPM Electronic
  • (Frequency , Current)
  • 2. Tunnel Test of BPM Electronic
  • (Temperature, Stability)
  • 3. Environmental magnetic field in the drift
    space.
  • (Corrections)
  • 4.Conclusions

2
Spectrometer Principle
Concept Measurement bending angle of particle
passing a magnetic dipole field.
  • Measure ? Bdl and to give the Ebeam the
    accuracy required
  • ? Bdl from local NMRs and field map
  • Max.error from the BPMs 1?m?
  • Max.error on integral magnetic field
    (almost zero)

3
Spectrometer Setup
  • Spectrometer is located between arc and straight
    section. (425 m from IP3)
  • Laminated steel dipole magnet ( 4NMR Probes).
  • 6 BPMs monitoring the incoming and outgoing beam.
  • BPMs mounted on individual limestone block to
    provide independence and shielded against
    synchrotron radiation.
  • Triple wire position system (WPS) to provide a
    reference against the ground and thermal-driven
    motion of BPM bodies.

4
Laboratory Test of BPM Electronics
1. Setup of the electronic
  • A Simulator card provide an input signal similar
    to the beam signal .
  • Four coaxial cables connected in parallel to the
    card (ensure the button inputs on the BPM
    electronic card receive the same signal).
  • Laboratory test of the electronic
  • BPM card temperatures variations 8 C
  • Signal frequency changes on BPM cards
  • Beam current changes
  • Stability of the beam position measurement

5
Laboratory Test of BPM Electronics
2. Effect of signal frequency Changes
  • Frequency changes until 5kHz have been set.
  • Results
  • The AGC signal and BPM readings show some
    dependence
  • ?f ? 5kHz ? ?BPM ? 8?m
  • The frequency changes in LEP order of
  • ?f ? 100 Hz ? ?BPM ? 0.16?m

No significant effects due to frequency changes.
6
Laboratory Test of BPM Electronics
3. The effects of the beam current
  • Switchable attenuator unit.
  • Same attenuation to each input signal
  • Results

Expected change in the AGC output
Change BPM position readings
Dependence of the position on beam current
larger than expected.
7
Laboratory Test of BPM Electronics
3.1. The effects of the beam current LEP running
  • We have been placed in the region
  • with a offset ? 400 ?m
  • and a of 0.8.
  • With LEP running conditions
  • a of 0.025

10 ?m
0.31 ?m
No significant effects due to beam current
changes.
8
Tunnel Test of BPM Electronics
1. The effects of the temperature changes
  • Variation on the BPM temperatures by blowing
    air.
  • Results
  • Different changes for different BPM cards.
  • ?T? 8?C ? ?BPMi ? 4?m
  • ?BPMii ? 7?m
  • ?BPMiii ? 200?m

9
Tunnel Test of BPM Electronics
  • Equal sum changes for all BPM s cards. (6 mV)
  • Results

?Temperature
Change reference of sum signal
Change sum signal
Change BPM position readings
BPM Electronic housed in temp-controlled rack
10
Tunnel Test of BPM Electronics
1.1. Effects of the temperature changes LEP
running
  • The rack ?Temperature
  • Mean 0.005 ºC
  • Sigma 0.03 ºC
  • With laboratory experience make a prediction in
  • ? BPMreadings? 0.7 ?m

11
Tunnel Test of BPM Electronics
2. Stability of the beam position measurement
  • Signal of one BPM card over 7h.
  • Results
  • In the absence temp. changes (?Tlt0.02 C) ? ?
    100 nm

12
Beam test of BPM Electronic
1. Cross-Calibration/Gains analysis
  • Relative gains calibrations with beam movements
    and rotation around 4 and 2.
  • Test of the reproducibility of the method used
    for calibration.
  • 2 relative gains ( horizontal and vertical
    plane) for each BPM.
  • Gain Calibration in different conditions
  • e High current
  • e- High current
  • e Low current
  • e- Low current

13
Beam test of BPM Electronics
1.1. Different mean per different particles types
  • Different mean value one side of 4.
  • Variation smaller 2.

14
Beam test of BPM Electronics
1.2. No energy dependence
15
Beam test of BPM Electronics
1.3 Conclusions
  • Identical conditions ? Identical gains
  • Mean gains difference e-, e.
  • No Energy Dependence.
  • Time dependence predictable.

CONSISTENCE IN THE RESULTS
16
Environmental magnetic field
1. Environmental Field (Earth fieldcablesvacuum
pumps)
  • Environmental field along spectro., 10E-4
    changes expected.
  • Field was assume constant along the
    spectrometer.
  • Changes of 2-3.10E-4 were observed.
  • Results
  • Installation of additional flux gates.
  • Maping the field in the drift space at
  • diff. Energies.
  • Calculation of the corrections for the
  • BPM readings.

17
Environmental fields
2. Stability of the fluxgates measurements
  • Three days of measurements without field.
  • Results
  • Measurements stable order of 10 mG.
  • Effect of the TGV observed.
  • Good correlation between fluxgates.

18
Environmental fields
3. Environmental Field Map/ Correction
19
Conclusions
  • Current and temperature dependence on the BPM
    readings .
  • First solved by choosing appropiates LEP
    running parameters.
  • Second housing the BPM card in a temp-controlled
    rack.
  • Bunch frequency variation not large enough during
    LEP running to cause perturbations.
  • Relative calibration of BPMs have been
    sufficiently well determinate to prevent
    systematic errors.

Both beam-based and electronic measurements
indicate BPM cards are stable with time for the
Spectrometer application.
  • Correction needed for the environmental ambient
    fields in the drift space.

20
Acknowledgements
All the work done in the Laboratory/Tunnel BPM
Electronic Test has been mainly developed by John
Matherson. I would like to express my sincere
thanks to my supervisor Bernd Dehning. I have to
express my gratitude to Massimo Placini and to
the members of the LEP Energy Calibration Group
for their support and collaboration.
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