motivation general rule for muon triggers:
DESCRIPTION
HO Scintillators in RPC Muon Trigger Conceptual design. J. F. de Trocóniz, UA-Madrid. 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: - PowerPoint PPT PresentationTRANSCRIPT
MotivationGeneral 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 pt 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
Towers 8+9 represent 92% of the rate
(pt> 10 GeV, || <1.24), but only 16% of the acceptance
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 ()
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
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
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 pefor “quiet” QIEs.
Is this performance good enough? Can be achieved systematically at
CMS?
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 EHO > 150 MeV (3% tile occupancy).
Backgrounds
p-p interactions (1034 cm-2 s-1): < 2 Hz/cm2
Neutron-induced conversions: < 10 Hz/cm2 (MB1 level)
n-p elastic collisions: < 25 Hz/cm2 (for EHO > 150 MeV)
Electronic Noise
HO-RPC Mapping Equilibrium between large acceptance and simplicity (hardware implementation) Minimal Map
Acceptance always larger than 90% (often much larger).
HO provides extra “RPC plane”
Trigger Algorithm
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)
Rate reduction
RPC noise trigger rates simulated using ORCA (50 Hz/cm2, 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, EHO > 150 MeV Reduction factor = 100
For 1.5 pe/bucket, EHO > 150 MeV Reduction factor = 30
Low-pt rates w/ HO comparable to high-pt w/o
HO
ORCA Results
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.
HCAL (HO) in RPC Trigger
TRIGGER BOARD
READOUT BOARD
SPLITTER
S-linkto DAQ
to Level-1 trigger
90 m @ 1.6Gbit/s
up to 5 m LVDS @ 80MHz
QIE
GOLQIE
QIE
HTR(Readout)Board
Optical Tx
Optical Tx
HCAL Front-end
New 'Optical SLB'
HTR Configuration for HO
P2
P1
8
88-way fiber in
8-way fiber in
FPGA
Rx Deser.Rx Deser.Rx Deser.Rx Deser.
Rx Deser.Rx Deser.Rx Deser.Rx Deser.Rx Deser.Rx Deser.Rx Deser.Rx Deser.
Rx Deser.Rx Deser.Rx Deser.Rx Deser.
Rx Deser.Rx Deser.Rx Deser.Rx Deser.
Rx Deser.Rx Deser.Rx Deser.Rx Deser.Rx Deser.Rx Deser.Rx Deser.Rx Deser.
Rx Deser.Rx Deser.Rx Deser.Rx Deser.
SLBSLB
SLB
SLB
SLB
SLB
FPGA
Outputs toRPC Crate
Total of 48 calorimeter channels per HTR
DAQout
Front-end datainputs
Example of cabling scheme satisfying
all constraints at HO and RPC ends
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/cm2 consider HO to improve efficiency (less restrictive algorithms, tower 6, “classic” 3/4).
HO is now part of the L1 Trigger Baseline