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Published byBryan Merritt Modified over 9 years ago
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Motivation General rule for muon triggers: Never neglect a possible backup reduction factor. It will always come back to you. Even if RPC trigger works just fine from the beginning one still wants to: Reduce rate in regions with only 4 or 3 RPC planes available. Reduce p t thresholds as much as possible. HO should be better than any pre-scale. HO Scintillators in RPC Muon Trigger Conceptual design HO Scintillators in RPC Muon Trigger Conceptual design J. F. de Trocóniz, UA-Madrid
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Towers 8+9 represent 92% of the rate (p t > 10 GeV, | | <1.24), but only 16% of the acceptance
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HO Characteristics 10 mm Bicron scintillator tiles positioned between coil and MB1 RPC 1 plastic for Wheels ±1, ±2. 2 plastics separated by 15 cm iron slab in Wheel 0. Covers the full MB1 system (barrel + overlap) up to | | < 1.24 (Tower 9) Typical cell size: 40 cm ( ) × 50 cm ( ) Granularity: 0.087 ( ) × 0.087 ( )
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HO matches well muon system in r- view (MB1) : 0.087 5 deg 16 RPC strips OK Not that well in r- : 0.087 (HCAL standard tower size) detailed HO – RPC map needed
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HO Readout Standard HCAL readout: Fibers HPD (G=2500) QIE ( T=25 ns) 90% of energy in two samples (phase independent of HCAL) More light: Thicker plastics, 4 WLS loops/tile, shorter fiber path Designed to give 10 pe / mip Trigger: Energy-over-threshold bit
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Test beam results Actual performance of HO system (Wheel 1 scintillators) measured at 2002 test beam (Jim Rohlf). 6 pe/mip/plastic Gaussian noise at normal incidence. 1.5 pe-equivalent/bucket can be improved to 0.9 pe for “quiet” QIEs. Is this performance good enough? Can be achieved systematically at CMS?
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HO Performance Simulated with CMSIM123 280 MeV/mip/plastic at normal incidence 6 pe 0.9 pe/bucket 64 MeV Geometrical acceptance: 93% Signal width dominated by photo-statistics. HO threshold at 1% tile occupancy 150 MeV (1 MeV deposited). Similar efficiency for 1.5 pe/bucket of noise, but 8 pe at signal peak, for E HO > 150 MeV (3% tile occupancy).
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Backgrounds p-p interactions (10 34 cm -2 s -1 ): < 2 Hz/cm 2 Neutron-induced conversions: < 10 Hz/cm 2 (MB1 level) n-p elastic collisions: 150 MeV) Electronic Noise
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HO-RPC Mapping Equilibrium between large acceptance and simplicity (hardware implementation) Minimal Map Acceptance always larger than 90% (often much larger).
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HO provides extra “RPC plane” Trigger Algorithm
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Require HO confirmation for low-quality RPC coincidences Built-in high efficiency (low quality RPC muons are ~30%) Remarkable threshold stability (allows tuning at CMS)
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Rate reduction RPC noise trigger rates simulated using ORCA (50 Hz/cm 2, nominal neutrons) Large sample: 110 Mevents, corresponding to 4.4 s of LHC. High quality noise trigger fraction much smaller than 1%. For 0.9 pe/bucket, E HO > 150 MeV Reduction factor = 100 For 1.5 pe/bucket, E HO > 150 MeV Reduction factor = 30 Low-p t rates w/ HO comparable to high-p t w/o HO
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ORCA Results
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Connecting Hardware (preliminary) Processing of HO signals performed at HTR boards (4 boards/sector, 2 FPGA/board). Provide energy-over-threshold programmable bit (possibly -dependent). All OR-ing corresponding to the HO-RPC map also handled here Input fibers organized according to constraints at HO end. SLB cards organize HTR bits into bit streams, and transmit to RPC Trigger Boards using GOLs (32 bits/bx) Output streams organized according to constraints at RPC end.
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HCAL (HO) in RPC Trigger TRIGGER BOARD READOUT BOARD SPLITTER S-link to DAQ to Level-1 trigger 90 m @ 1.6Gbit/s up to 5 m LVDS @ 80MHz QIE GOL QIE HTR (Readout) Board Optical Tx HCAL Front-end New 'Optical SLB'
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HTR Configuration for HO P2 P1 8 8 8-way fiber in FPGA RxDeser.RxDeser. RxDeser. RxDeser.RxDeser.RxDeser.RxDeser.RxDeser. RxDeser.RxDeser.RxDeser. RxDeser. RxDeser. RxDeser. RxDeser. RxDeser.RxDeser.RxDeser.RxDeser.RxDeser.RxDeser.RxDeser.RxDeser.RxDeser. RxDeser. RxDeser.RxDeser.RxDeser. RxDeser. RxDeser.RxDeser.RxDeser. SLB FPGA Outputs to RPC Crate Total of 48 calorimeter channels per HTR DAQ out Front-end data inputs
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Example of cabling scheme satisfying all constraints at HO and RPC ends
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Conclusions Investigating how to incorporate HO into RPC trigger: Geometrical integration, RPC+HO extended algorithm, basic lines of hardware implementation established. If HO performance at 2002 test beam achieved systematically at CMS RPC trigger rate reduced by 100. Efficiency O(90%) stable as a function of HO energy threshold (allows tuning). Implications much more important in case RPC noise can be reduced to 5 Hz/cm 2 consider HO to improve efficiency (less restrictive algorithms, tower 6, “classic” 3/4). HO is now part of the L1 Trigger Baseline
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