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The frontend electronics for LHCb calorimeters

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Title: The frontend electronics for LHCb calorimeters


1
The front-end electronics for LHCb calorimeters
On behalf of the LHCb collaboration
  • Overview of the system
  • The different sub-detector electronics, focusing
    on the three specific ASICs
  • Ecal/Hcal (LAL Orsay)
  • PS (LPC Clermont-Ferrand)
  • SPD (Barcelona)
  • Other points of interest

2
The LHCb detector
Ionizing particles
PS/SPD 6000 ch pads fibers
ECAL 6000 ch shashlik (Pb-scint)
HCAL 1500 ch tilecal (Fe-scint)
3
Calorimeter trigger electronics scheme
(6000 ch)
(6000 ch)
(1500 ch)
(6000 ch)
4
40 MHz Front-End Electronics
  • 27 identical crates filled with two types of
    Front-End Boards
  • allows to provide Preshower or Ecal/Hcal crates
    at low cost
  • Motivation for electronics specificity
  • High level0 rate (1 MHz) gt time between
    level0 yes can be 25 ns
  • gt
    need full information every 25 ns
  • High occupancy and high rate gt need for fast
    shaping
  • Use of fast photomultiplier gt fast
    shaping is possible

5
ECAL/HCAL electronics
In HCAL/ECAL large number of photoelectrons
(50/GEV, 500-1000/GEV) gt pulse shape smooth and
reproducible gt shaping by delay line clipping
and deadtimeless integrator (no switch) gt
with this design pedestals and digital noise are
small and one can obtain a good dynamic range
in a 12-bit/40-MHz ADC followed by a pedestal
subtractor
Simulation plots with short input pulse
INTEGRATOR INPUT SIGNAL
ADC INPUT SIGNAL
T050ns
T0
T025ns
6
Ecal/Hcal ASIC schematics
Board implementation
7
Ecal/Hcal ASIC performances
8
Ecal/Hcal ASIC layout and FEB prototype
AMS BiCMOS 0.8um (1.9 x 2.1 mm2) (60mW/ch)
16-channel prototype of the Ecal/Hcal front-end
board (1999)
9
Preshower and SPD requirements
  • Preshower (PS) and Scintillator
  • Pad Detector (SPD) provide
  • PID for L0 electron trigger
  • photon/MIP separation by SPD
  • electron/pion separation by PS

Various 1-MIP signals Wiggles gt 70 ns parasitic
pickup
  • Because of the small number of photoelectrons
    (about 20-30 per MIP), PS SPD have a
    fluctuating pulseshape.
  • However, a 25 ns integration contains most of
    the charge (85) as seen on typical 5-MIP signals

10
PS ASIC block diagram
  • The Preshower requirements are twofold
  • for the level 0 trigger, perform the
    identification of electrons and photons while
    rejecting the charged pions. The corresponding
    threshold is about 5MIPs.
  • measure the part of energy lost in the PS to
    correct the global calorimeter information.
  • gt the useful measurements cover the 1MIP to
    100MIPs range
  • Choice of a multiplexed 40MHz real time
    integrator driving a 10-bit ADC.
  • LSB value fixed at 1/10 of a MIP, to obtain a
    sufficient precision on the MIP and properly
    cover the required dynamic range.
  • The 5MIP threshold will be applied digitally
    beyond the ADC. The precision obtained by a 25ns
    integration on a 5MIP signal is sufficient for
    the trigger system.

On the front-end board
  • The ASIC has to perform a clean integration
    every 25ns. Its critical parts are thus fully
    differential.
  • It actually consists in two parallel paths each
    running at 20MHz, then multiplexed at the output.

One among 8 channel of the ASIC.
11
PS ASIC main building blocks
  • Gain-2 stage of the
  • output multiplexor
  • with parallel compensation.
  • Advantages of this scheme
  • when compared to
  • usual serial compensation
  • no loss of dynamic range
  • ability two over-compensate
  • for taking two successive
  • stages into account

First stages of the chip common to differential
mode block and integrator
Output buffer A true push-pull using only NPN
transistors !
AOP with common mode feedback
With a quiescent current of 16ma, its able to
drive a 50ohm cable with a rise time of 3.5ns
with less than 0.5 of non linearity.
12
PS ASIC performances
The spreading of the signal over a few clock
periods can be observed here. The corresponding
integrated charge per clock period appears
clearly at the output of the multiplexor. The
linearity remains within a 1 window over the
whole dynamic range.
The plot of the pedestal distribution at the chip
output presents a double peak which is due to the
two independent paths per channel. These offsets
will be subtracted further in the chain. The
noise level appears well below one ADC count.
This plot displays a MIP measured in real
conditions at the extremity of a 15-meter cable.
The peak amplitude is about 10 ADC counts.
13
PS ASIC layout and VFE prototype
Prototype of the 8-channel ASIC AMS 0.8u BiCMOS
(2.60 x 4.40 mm2) (100mW/ch)
Prototype of the 64-channel Very Front-End Board
14
SPD ASIC block diagram
  • The main requirement for the SPD is to perform
    the selection between photons and charged
    particles.
  • As seen before, the corresponding threshold is
    necessarily very low (0.5MIP). Thus the potential
    reminder of the signal measured 25ns earlier
    (17) forces us to subtract the same fixed part
    of the preceding charge sample (17).

Like the Preshower ASIC and for the same reasons,
this chip is mostly differential. Its major
difference is that its output is merely digital
(one bit per channel).
One among 8 channel
15
SPD ASIC main building blocks
Subtractor
Integrator
Track Hold
Latched comparator
16
SPD ASIC current results
Linearity
  • General results of the analog part (4-channel
    prototype)
  • Offset (Output Zero Error) ltOZEgt 38.6 mV
    ?io 70 mV r.m.s.
  • Gain ltVo/Vigt 16.51 (typical pulse) ?io
    0.091 r.m.s. (0,55)
  • Treset 5.5 ns (for 1 V output)
  • Noise is about 1 mV r.m.s
  • Output range is gt?1V for an arbitrary input
    signal.
  • Linearity error is lt 0.5 full scale.

Threshold crossing
Threshold precision
17
SPD ASIC layout and test board
4-channel prototype test board
Prototype of the 4-channel ASIC AMS 0.8u BiCMOS
(2.64 x 3.12 mm2) (100mW/ch)
18
Standard calorimeter backplane
Top part for power supplies, TTC and ECS.
Bottom part for trigger and readout
interconnections.
19
Conclusion and other highlights
  • The requirements for the electronics of the four
    sub-detectors constituting the LHCb calorimeter
    have led us to design three different and
    specific front-end sub-systems.
  • Clermont-Ferrand (LPC) is in charge of the
    electronics for the Preshower, Barcelona of the
    SPD and LAL ORSAY of the Ecal/Hcal.
  • Those were however designed to share standard
    elements everywhere possible.
  • Three different ASICs have been designed. They
    are all based upon the AMS 0.8u BiCMOS
    technology. Two of them already passed the
    production readiness review.
  • The first level trigger requirements led us to
    implement dense interconnections within and
    between the 27 electronics crates.
  • There will be about 1000 cables carrying a total
    of 1200Gbit/s.
  • Each crate backplane will transfer about
    200Gbit/s.
  • The non negligible radiation level led us to
    realize a SEU and SEL hardened design.
  • The Preshower and ECAL/HCAL ASICs have
    successfully undergone radiation tests in a
    proton beam (50kRads) and in an ion beam looking
    for the SELs.
  • All the other sensitive components are currently
    undergoing the same kind of tests.
  • The design of all the boards had itself to take
    this problem into account.
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