Energy Spectrum Measurement of the Multipacting Electons the SPS. Analysis the Possible Uti.pdf
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Energy Spectrum Measurement of the Multipacting Electons the SPS. Analysis the Possible Uti
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH
CERN SL DIVISION
Geneva, Switzerland
May 2000
SL-Note-2000-040 BI
Energy Spectrum Measurement of the Multipacting
Electons in the SPS.
Analysis of the Possible Utilisation of the BGIP Monitor
Pivi, M. – LHC Division – VAC Group
Variola, A. – SL Division – BI Group
Abstract
See the introduction in next page.
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH
CERN SL DIVISION
2
Energy Spectrum Measurement of the Multipacting Electrons in the SPS.
Analysis of the Possible Utilisation of the BGIP Monitor
Mauro Pivi
CERN – LHC Division – VAC Group
Alessandro Variola
CERN – SL Division – BI Group
Introduction
An electron cloud cascade driven by the proton beam space charge field is expected to occur in the
LHC. This charge cloud composed of secondary, ionisation and photo - electrons is accelerated
under the influence of the proton beam electric field as a function of both bunch intensity and
period. This process results in the production of a large heat load on the surface (especially on the
dipole section beam screen at cryogenic temperature), multiplication of space charge in the
chamber, coupling between electrons and the beam and increased vacuum pressure that could
ultimately cause the loss of the proton beam itself.
In-depth theoretical and experimental work has recently been carried out at CERN [1-1b]. In this
framework, a numerical simulation code has been developed [2-2b] following the analytical
approach to the problem [3] and a deep research program has been executed. To test the validity of
the simulation code, experimental results were obtained in a TW test chamber simulating the proton
beam by means of RF pulse trains. Good agreement was observed between experiments and
simulations when measuring the energy spectrum of the emitted electrons and the current as a
function of the RF pulse parameters. Furthermore, in the SPS-MD with an LHC-type beam, above a
beam intensity threshold a pressure rise by more than a fact
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