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Monitoring of the accelerator beam distributions for internal target facilities
Nuclear Experiment · Submitted 16 Oct 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The method allows for the observation of the proton beam size as well as the position of the beam relative to the target.
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The abstract, sentence by sentence
We describe a direct method for monitoring the geometrical dimensions of a synchrotron beam at the target position for internal target installations. The method allows for the observation of the proton beam size as well as the position of the beam relative to the target. As a first demonstration of the technique, we present results obtained by means of the COSY-11 detection system installed at the cooler synchrotron COSY. The influence of the stochastic cooling on the COSY proton beam dimensions is also investigated.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We describe a direct method for monitoring the geometrical dimensions of a synchrotron beam at the target position for internal target installations. | contribution 0.95 | 0.81 | 0.16 | asserted 0.99 |
| s1 | The method allows for the observation of the proton beam size as well as the position of the beam relative to the target. | contribution 0.56 | 0.59 | 0.11 | asserted 0.96 |
| s2 | As a first demonstration of the technique, we present results obtained by means of the COSY-11 detection system installed at the cooler synchrotron COSY. | method 0.65 | 0.94 | 0.06 | asserted 1.00 |
| s3 | The influence of the stochastic cooling on the COSY proton beam dimensions is also investigated. | contribution 0.80 | 0.88 | 0.07 | asserted 0.88 |
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The paper
Original abstract
We describe a direct method for monitoring the geometrical dimensions of a synchrotron beam at the target position for internal target installations. The method allows for the observation of the proton beam size as well as the position of the beam relative to the target. As a first demonstration of the technique, we present results obtained by means of the COSY-11 detection system installed at the cooler synchrotron COSY. The influence of the stochastic cooling on the COSY proton beam dimensions is also investigated.
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How the literature uses it
2 arXiv papers cite this in 2 sentences
Papers citing it
Uses its data or values 2 papers
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For the calculations of the missing mass resolution a typical beam and target parameters available at the Cooler Synchrotron COSY [ref] were assumed: beam momentum spread $Δp/p≈10^-3$ (FWHM), perpendicular beam profiles: horizontal $σ_X$=2 mm, vertical $σ_Y$=5 mm [ref] .
Reaction pp -> pp \pi \pi \pi as a background for hadronic decays of the eta-prime meson · Feasibility for a large acceptance detector · 0.86
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The beam momentum spread $Δp/p$ after applying both types of cooling method can be reduced to around $10^-3$ [ref] .
Test of charge conjugation invariance in eta->pi0 e+e- and eta->pi+pi-pi0 decays · Cooler Synchrotron COSY · 0.81
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