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Comparison of Timing Properties of Glass Multigap RPCs with 0.3 and 0.6 mm Subgap Width
High Energy Physics - Experiment · Submitted 17 May 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The rate capability of the (2x0.6mm) counter was found to be considerably lower than for the (2x(2x0.3mm)) one.
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The abstract, sentence by sentence
Timing characteristics of two multigap RPCs were compared. One had four subgaps 0.3 mm wide and the other - two subgaps 0.6 mm wide. Specially developed electronics was used. Electronics resolution convoluted with measured charge spectra at operating point was estimated as about 65 ps. The best time resolutions obtained at low counting rate were 75 ps for the 0.3 mm subgap and about 125 ps for the 0.6 mm one, after slewing corrections. The rate capability of the (2x0.6mm) counter was found to be considerably lower than for the (2x(2x0.3mm)) one.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Timing characteristics of two multigap RPCs were compared. | contribution 0.96 | 0.84 | 0.04 | asserted 0.98 |
| s1 | One had four subgaps 0.3 mm wide and the other - two subgaps 0.6 mm wide. | method 0.82 | 0.60 | 0.04 | asserted 0.99 |
| s2 | Specially developed electronics was used. | method 1.00 | 0.62 | 0.02 | asserted 0.97 |
| s3 | Electronics resolution convoluted with measured charge spectra at operating point was estimated as about 65 ps. | result 0.71 | 0.88 | 0.05 | asserted 0.91 |
| s4 | The best time resolutions obtained at low counting rate were 75 ps for the 0.3 mm subgap and about 125 ps for the 0.6 mm one, after slewing corrections. | result 1.00 | 0.94 | 0.43 | asserted 1.00 |
| s5 | The rate capability of the (2x0.6mm) counter was found to be considerably lower than for the (2x(2x0.3mm)) one. | result 1.00 | 0.95 | 0.51 | asserted 1.00 |
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Original abstract
Timing characteristics of two multigap RPCs were compared. One had four subgaps 0.3 mm wide and the other - two subgaps 0.6 mm wide. Specially developed electronics was used. Electronics resolution convoluted with measured charge spectra at operating point was estimated as about 65 ps. The best time resolutions obtained at low counting rate were 75 ps for the 0.3 mm subgap and about 125 ps for the 0.6 mm one, after slewing corrections. The rate capability of the (2x0.6mm) counter was found to be considerably lower than for the (2x(2x0.3mm)) one.
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