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Direct Electron Cloud Measurements in the Main Injector

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Required lots of noise reduction. Could not get a good zero for subtraction. Dip at 1.1 s ... With reduction of noise and more careful electronics, a wide range of ... – PowerPoint PPT presentation

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Title: Direct Electron Cloud Measurements in the Main Injector


1
Direct Electron Cloud Measurements in the Main
Injector
  • Reminder of Situation
  • Direct Measurements
  • Bob Zwaska
  • August 23, 2006
  • AP Department Meeting

2
Considering the Cloud
  • Simulations suggest that MI might be near a
    threshold
  • 4-5 orders or magnitude increase of cloud density
    with a doubling of bunch intensity
  • Not yet established
  • How well code pertains to Main Injector (question
    of SEY)
  • What the effects of electron neutralization will
    be on the beam

Bill Ng (FNAL)
M. Furman (LBL) FERMILAB-PUB-05-258-AD
3
Electron Cloud Effect (my view)
Proton Beam
Many Processes
Heating
Primary Electrons
Scattering, tune shift, plasma instabilities
Secondary Electrons (cloud)
Secondary Emission
Ions (plasma)
Secondary Emission
Beam Pipe
Desorption
Gas
4
First Measurements of Dynamic Pressure Rise
Ion Pump Current
  • See fast rise over the course of a cycle (1s)
  • The control system barely keeps up

Ceramic beam pipes
5
Nonlinear Response
Different beam structure
first pulses
Turn on
6
50 Hz Pump
Type of pump installed at two locations
  • Higher resolution reveals cycle details
  • Injections
  • RF capture
  • Ramp
  • Transition
  • Flattop
  • Extraction

1.0 1011 / bunch
0.5 1011 / bunch
7
Electron Probe
  • Retarding Field Analyzer
  • Borrowed from Argonne
  • Two electrodes connected externally
  • Retarder can be biased to allow energy
    measurements
  • Currently being used as a simple electron counter

Collector
Retarder
8
Electron Detector
  • See some activity on all production cycles
  • Have some noise issues
  • Device - ICLOUD
  • V correspond to uA current (amplifier MADC)
  • Very noisy
  • Sampled to Datalogger at time of maximum

9
Time Measurements
  • Unbiased signal
  • Required lots of noise reduction
  • Could not get a good zero for subtraction
  • Dip at 1.1 s
  • Rapid increase of signal occurs into acceleration
  • Dip at transition (next slide)

10
Transition Effect
  • Definite decrease in cloud signal at transition
  • Not expected
  • Simulations have suggested that cloud current
    only increases with smaller bunch length
  • Will follow this in the future

11
Collected results
  • Clear turn-on at higher intensities
  • Noise is worse due to amplifier/MADC system
  • 0.1 uA 1 neutralization at 20e12

12
SSNuMI Histogrammed
13
Conclusions
  • Electron Cloud Detector is installed and
    operating in the Main Injector
  • New measurements are consistent with pressure
    measurements, but differ in details
  • Expected due to different conditions at devices
  • Directly measured turn-on of electron cloud
    current with intensity
  • Unexpected dip of current at transition
  • With reduction of noise and more careful
    electronics, a wide range of measurements should
    be possible
  • Will also consider new detectors for further
    investigation of the MI electron cloud
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