W combination for ‘98 winter conferences
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Transcript W combination for ‘98 winter conferences
The LHCb vertex detector
Frederic Teubert
CERN
EP division
VERTEX 99 (20-25) June
Frederic Teubert
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What do we want to measure?
The main goal is the determination of
the origin of CP violation, by precision
measurements in many B decay modes.
The possibility of measuring several of
the CP parameters in a single
experiment, could give a glimpse on new
physics beyond the SM.
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What do we want to measure?
Vtd Vtb*+ Vcd Vcb*+ Vud Vub*= 0
Vtd Vud*+ Vts Vus*+ Vtb Vub*= 0
Bd p+pp
D-p+
Vub
Vcb
Bs DSK
Bd DK
VERTEX 99 (20-25) June
Vtd
Vub
h
Vtd
Vts
=l2h
Bs J/yKS
J/yKL
Bs J/yf
(Theoretically clean channels)
Frederic Teubert
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LHC environment
-
Large bb cross section (~500 b), with
L = 2·1032 cm-2 s-1 1012 bb pairs per year.
Energy of the B’s ~80 GeV ~7 mm.
A single-arm spectrometer covering
min ~ 15 mrad (beam pipe and radiation)
max ~ 300 mrad (cost)
i.e. h ~ 1.9 to 4.9
-
Has similar bb
acceptance to large
central detector
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LHCb detector
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Critical LHCb detectors
RICH detectors
Two detectors covering the range
between 1 and 150 GeV. Needed for
particle ID (for instance Bpp/Kp).
Vertex detector
Need to reconstruct S.V. with good
resolution (IP 40m), for instance Bs
oscillations, and for trigger purposes.
Trigger system
bb / tot = 0.005
Reduce the input rate from 40 MHz to
200 Hz.
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LHCb Trigger system
Level
Level 0
Characteristics
Sub-detector rates/latency
High Pt:
e
h
ECAL
HCAL
Muon detector
40 MHz
4 s
Interaction point
VELO
on-detector off-detector electronics (1 TB/s)
Level 1
Large Impact Parameter
Secondary Vertices
VELO
High Pt
Tracker
1 MHz
256 s
off-detector event buffer (2-4 GB/s)
Level 2
Refine secondary vertices VELO+Tracker
40 KHz
10 ms
Level 3
Partial reconstruction
5 kHz
200 ms
All
To tape = 200 Hz
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VELO: The LHCb vertex detector
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VELO: The LHCb vertex detector
Small overlap
6 cm during
injection
12 cm
• Detector length 1m
• Closest distance to the beam axis
1 cm.
• Station spacing varying
from 4-12cm
• Each station has an r and
a f measuring detector
• Stereo angle between
successive f detector layers
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Vacuum vessel
The design of the vacuum tank and support structures of VELO
needs to satisfy several requirements:
Low mass in the acceptance region
Provide alignment and retractability of VELO
Mechanical stresses induced by heat loading
Maintain high-vacuum compatibility while providing signal
feed-through (22000 signal wires 50 twisted-pairs per
hybrid)
manipulators
vessel
Top
Half
window
primary vacuum
100cm
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Frederic Teubert
detectors
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Mechanical Support
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RF shield primary
secondary Vacuum
2*100 micron / detector station
Need wake field suppressor
Best case: 100 micron once
Worst case:
2.4*100 micron/detector station
for low angle tracks (but high p)
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VELO baseline design
The design of the vertex
detector is driven by:
Fast track
reconstruction (L1
trigger) rf geom.
Radiation hard rf
geom. + n on n
technology + operating
temperature 5C +thin
detector (depletion
voltage)
Reduce multiple
scattering 150m thin
detectors
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Routing of channels
Both detectors utilize a double metal layer to
readout inner strips.
Detectors fabricated
on 100mm wafer
inner radius 10mm
readout tracks
spaced 50m
r-measuring
detectors
VERTEX 99 (20-25) June
Frederic Teubert
f-measuring
detectors
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Irradiation
The particle
fluence
is dominated by
primary particles.
The maximum
equivalent dose of
1MeV neutrons per
station in one year is
1014/cm2
The idea is to
replace the innermost
detectors each year.
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Overview of the Readout scheme
Analogue readout
FE Radiation Hard
FADC + L1
buffers 10m away
Processing in
DSPs after L1 accept
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Test Beam Setup
6 r-sectors and 6 f-sectors (61) following closely the
baseline design, (300 m, n on n detectors, rf geometry, slow
readout VA2 chips).
LHCb like events mimicked by arranging Cu-targets in front
of the silicon detectors.
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Alignment and cluster resolution
The alignment of the detectors is an important
issue for the trigger performance.
No possibility to use the alignment constants for
tracks in the rz plane. The position of the detector
needs to be known with a precision of few 10 m.
The alignment constants measured with the POLI
machine (3D survey machine) and minimizing the 2 of
the fitted tracks agree better than 50 m.
We expect to be able to install the detectors
with a precision better than 10 m.
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Alignment and cluster resolution
By measuring the
residuals we
determine a
cluster resolution
of
= 6 m
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Primary vertex reconstruction
Target thickness
300m
Distance to the
first silicon detector
7.5 cm
Extrapolating this
results to the
statistics of an LHC
event and full angular
coverage in f implies,
PV 56 m
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First Test with a Fast Readout Chip (SCTA 128)
One r-detector
equipped with
4 SCTA/hybrid
Main goal:
Noise Study
Over Spill
Clock 40 MHz
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Results obtained in the lab with the SCTA chip
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Results obtained in the Test Beam with the SCTA chip
S/N 20
Rising time
25 ns
After 25 ns
the signal is
reduced to 1/3 of
the maximum.
VERTEX 99 (20-25) June
25 ns
Frederic Teubert
25 ns
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Outlook
First prototype of the VELO detector
in a test-beam shows reasonable
performance
Cluster resolution 6 m
Alignment studies, Level 1 studies
LHCb like events mimicked by
arranging Cu-targets in front of the Si
Equivalent LHCb resolution pv 56 m
Test of fast electronics (SCTA 128)
S/N30 (in the LAB), S/N20 (in the TB)
25 ns rising time, 1/3 of the signal after
25 ns.
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Future plans
Test of irradiated n on n detectors with
fast electronics in the TB (August ‘99)
Test of p on n technology (smaller pitches)
in the TB. Come to a conclusion about the
best technology at the end of ‘99
Detector optimization (2 modules of 182
with 45.5 sectors, reduce inner radius to 8
mm and reduce outer radius to fit in one
wafer).
Test (SCTA or BEETLE) + ODE in the TB by
summer ‘00. Come to a conclusion by the end
of ‘00
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