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Presented by A.Kashchuk 22-23.04.2002 Muon meeting, CERN A.Kashchuk LHCb muon front-end chip by user’s eyes Why 2 chips? CARIOCA negative CARIOCA positive 1.What I like and accept 2.What I don’t like and can not accept 22-23.04.2002 Muon meeting, CERN A.Kashchuk It is possible: “Bipolar” 22-23.04.2002 Muon meeting, CERN A.Kashchuk It was clear already in Dec.1999, that we’ll not find perfect chip... In order to satisfy specific requirements of the LHCb experiment, it has been suggested in January 2000 (to Burkhard and Pierre) to start designing own LHCb Muon ASIC for MWPC using submicron CMOS 22-23.04.2002 Muon meeting, CERN A.Kashchuk Innovation in the CMOS amplifier is the active feedback (see P.Jarron et al.,1995) It provides in CMOS fast shaping and low noise at high Cdet Input Output SPICE model of the Current Amplifier based on the active feedback 22-23.04.2002 Muon meeting, CERN A.Kashchuk I like that LHCb Muon front-end chip is designed in 0.25 micron CMOS technology of IBM; It based on the new active feedback schematics which provides in CMOS fast shaping and low noise at high Cdet; It is radiation hard; It has single power supply +2.5V and low power consumption; It can also be applied for RPC; It can be optimized for negative and positive input polarities I like also that Its further integration with DIALOG chip can provide compact and cost-effective solution for any number of channels/board needed in various regions of the LHCb Muon System 22-23.04.2002 Muon meeting, CERN A.Kashchuk Input polarity definition in CARIOCA chip versions: Input current must be added to bias current to maximize dynamic range Positive version nMOS If=Iin+Ibias 22-23.04.2002 Muon meeting, CERN Negative version pMOS -If=Iin+Ibias A.Kashchuk What do not like I’ll show problems (and my statements) I suggest changes in schematics of the CARIOCA preamplifiers Stability margin is not enough; Optimization of CMOS transistor parameters within feedback loop has to be done; Cfeed should be avoided 22-23.04.2002 Muon meeting, CERN A.Kashchuk Equivalent circuit and its impulse response: CARIOCA negative Qin =1fC Parameters taken from chip: G5=42.35mA/V, G6=1.1mA/V, G7=52.6uA/V, Cfeed=400fF, capacitors Model is ringing even at small Cdet 22-23.04.2002 Muon meeting, CERN A.Kashchuk CARIOCA negative (cont.) Cdet is increased G5=42.35mA/V, G6=1.1mA/V, G7=52.6uA/V, Cfeed=400fF, capacitors Model is unstable at Cdet=10-100pF Note: similar response has been reproduced on real schematics with increasing G7 Being connected to SPB, all 16 channels of CARIOCA negative generate 80 MHz at any threshold 22-23.04.2002 Muon meeting, CERN A.Kashchuk Equivalent circuit and its impulse response: CARIOCA positive Parameters taken from chip: G5=42.35mA/V, G6=1.4mA/V, G7=19uA/V, Cfeed=400fF, capacitors Model is close to instability 22-23.04.2002 Muon meeting, CERN A.Kashchuk Both versions will be stable at reduced G7 (factor10) 22-23.04.2002 Muon meeting, CERN A.Kashchuk As shown, without Cfeed it is unstable again Cfeed=0.4pF introduces dynamic capacitor of about 120 pF 22-23.04.2002 Muon meeting, CERN A.Kashchuk It’ll be stable without Cfeed at reduced G6 (factor 10) Only G5 is taken from chip Excellent response Excellentimpulse response Excelent response Cdet=0-1000pF, 50% amplitude reduction at Cdet=1000pF 22-23.04.2002 Muon meeting, CERN A.Kashchuk Note: feedback loop in CARIOCA has been designed incorrectly in both preamplifiers As a result: CARIOCA negative can not be used; CARIOCA positive has small stability margin 22-23.04.2002 Muon meeting, CERN A.Kashchuk I suggest changes in schematics Preamplifiers (cont.) Current-mirrors from preamplifiers to the shaper stage (providing about 3mV/fC gain) must be avoided; Existing gain (25mV/fC) has to be used; Proposed schematics will also reduce voltage spread propagated to the next stages 22-23.04.2002 Muon meeting, CERN A.Kashchuk Existing voltage gain has to be used, it will also reduce voltage spread propagated to the next stages Negative version Vout to shaper 22-23.04.2002 Muon meeting, CERN Positive version Vout to shaper A.Kashchuk One ASIC versus two 22-23.04.2002 Muon meeting, CERN A.Kashchuk Solution 1: by increasing Ibias How I have modified positive version to work with negative signals: To the existing connections within CARIOCA chip Iin (dummy input) Increased Ibias=60uA instead of 6uA 22-23.04.2002 Muon meeting, CERN A.Kashchuk MWPC on cosmics equipped by the positive board with the negative input signal Gas 40Ar/50CO2/10CF4, Th=+/-200mV Sigma 2.9ns within requirements TDC spectrum at 3.15kV (OR of 3 wire strips 6mm width x 25cm length each one) 22-23.04.2002 Muon meeting, CERN A.Kashchuk Solution 2: by switching Ibias polarity Both main and dummy inputs will be used in this version to save threshold polarity 22-23.04.2002 Muon meeting, CERN Only one bias current is ON A.Kashchuk I suggest changes in schematics Shaper Time constants cancelled in CARIOCA: 9 and 80ns I did not see how looks difference of the real signal and its approximation by sum of the exponents implemented in CARIOCA; I’ll show (see below), that another time constants have to be cancelled, using another optimization criterion 22-23.04.2002 Muon meeting, CERN A.Kashchuk Pulse width vs HV measured with 241Am-source shows HV=3.15kV Average pulse width shows tail Bursts of pulses occur when tail crosses threshold 22-23.04.2002 Muon meeting, CERN A.Kashchuk ASDQ++ has no such ‘defect’ up to 3.3kV Wire and Cathode readout (average pulse FWHM and 10% width vs HV, 241Am, gas 40Ar/50CO2/10CF4) Pulse width (ns) Rise starts at 2.9-2.95kV! Carioca_v0 ASDQ++ pn#2c#10 10%width 200 p#3c#10 150 10%width Carioca+ ASDQ++ max 100 50 0 2.6 2.7 2.8 2.9 3 3.1 3.2 HV (kV) 22-23.04.2002 Carioca+/- Muon meeting, CERN A.Kashchuk 3.3 3.4 Base Line Restorer (BLR must reduce base line fluctuations introduced by another sources) Spread of DC levels produced by BLR on discriminator inputs must be avoided; (See Werner’s report) 22-23.04.2002 Muon meeting, CERN A.Kashchuk Discriminator Differential thresholds should be changed to single polarity; Threshold has to be common for even and odd channels; Hysteresis has to be studied better (can be reduced on board) 22-23.04.2002 Muon meeting, CERN A.Kashchuk Conclusion Very good general architecture of CARIOCA chip (dummy channel followed differential stages) has been implemented rather bad ‘Bipolar’ solution ‘One ASIC instead of two’ is real one. We have to work effectively to implement many improvements for submission in July 2002 22-23.04.2002 Muon meeting, CERN A.Kashchuk