Title: Test and Energy measurement with the LEP Spectrometer
1Test 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
2Spectrometer 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)
3Spectrometer 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.
4Laboratory 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
5Laboratory Test of BPM Electronics
2. Effect of signal frequency Changes
- Frequency changes until 5kHz have been set.
- 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.
6Laboratory Test of BPM Electronics
3. The effects of the beam current
- Switchable attenuator unit.
- Same attenuation to each input signal
Expected change in the AGC output
Change BPM position readings
Dependence of the position on beam current
larger than expected.
7Laboratory 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.
8Tunnel 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
9Tunnel 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
10Tunnel 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
11Tunnel 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
12Beam 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
13Beam test of BPM Electronics
1.1. Different mean per different particles types
- Different mean value one side of 4.
- Variation smaller 2.
14Beam test of BPM Electronics
1.2. No energy dependence
15Beam 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
16Environmental 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.
- Installation of additional flux gates.
- Maping the field in the drift space at
- diff. Energies.
- Calculation of the corrections for the
- BPM readings.
17Environmental fields
2. Stability of the fluxgates measurements
- Three days of measurements without field.
- Measurements stable order of 10 mG.
- Effect of the TGV observed.
- Good correlation between fluxgates.
18Environmental fields
3. Environmental Field Map/ Correction
19Conclusions
- 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.
20Acknowledgements
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.