A CCD-based vertex detector Chris Damerell on behalf of the LCFI Collaboration • Project overview and design principles • R&D programme • Development of.
Download ReportTranscript A CCD-based vertex detector Chris Damerell on behalf of the LCFI Collaboration • Project overview and design principles • R&D programme • Development of.
A CCD-based vertex detector Chris Damerell on behalf of the LCFI Collaboration • Project overview and design principles • R&D programme • Development of novel CCDs and readout electronics • Development of thinnest possible detector layers • Physics studies • Summary and future plans July 14 2003 US LC Workshop Cornell U – Chris Damerell 1 Project overview • Linear Collider Flavour ID Collaboration: Bristol U, Lancaster U, Liverpool U, Oxford U, QMUL and RAL • R&D assumes up to 5 CCD development cycles at intervals of ~20 months • Initially funded by PPARC for £2.3M for 3 yrs from April 2002 (£700K equipment, £1600K PPARC manpower) • Synergy with recent PPARC plans to play a major part in the LC BDS (beam delivery system) • Working to develop closer ties between other regional VTX activities. Our international phone conference at time of US workshop at UT Arlington was a major success • Looking forward to one international collaboration to build the LC vertex detector, once prototype ladders have enabled the technology choice to be made • One major unknown in the decision process is the accelerator technology July 14 2003 US LC Workshop Cornell U – Chris Damerell 2 Design principles • 5 layers, inner layer at radius 12-15 mm • 3-hit coverage to cosq = 0.96 • thin layers (<0.1% X0 ) for minimal mult scatt and g conversions July 14 2003 US LC Workshop Cornell U – Chris Damerell 3 • silicon pixels of size ~ 20 mm square for low cluster-merging in jets • support structure with micron precision/stability (specially important for oblique tracks near ladder ends) • on-detector signal processing, so almost no external connections • power dissipation measured in few tens of watts, so gas cooling sufficient ( vital for low material budget) • ‘adequate’ radiation hardness • readout time ~ 5 ms for JLC/NLC (between bunch trains) ~ 50 ms for TESLA (20 frames/bunch train) • 4 4 p sin3 / 2 q • crucial for efficient charm ID (1-prong decays), vertex charge (Bs), but quantitative physics examples still being worked on … July 14 2003 US LC Workshop Cornell U – Chris Damerell 4 Novel CCDs and readout electronics • CCD sizes similar to SLD, but readout needs to be 20-2000 times faster • eliminate bulky electronics which would degrade fwd tracking and calorimetry • total of 800 Mpixels, cf 307 Mpixels for SLD • TESLA readout requirement stimulated concept of ‘column parallel’ operation • innovative CCD/CMOS hybrid. If successful, this architecture may also be preferred for NLC/JLC. However, for this case, the conventional architecture with a multiple-output linear register should also be evaluated July 14 2003 US LC Workshop Cornell U – Chris Damerell 5 M N N “Classic CCD” Readout time NM/Fout Column Parallel CCD Readout time = N/Fout • Max possible readout speed, for given noise performance • Readout IC (amp+ADC on 20 mm pitch) only became available with deep submicron CMOS technology • TESLA requires parallel register clocking at 50 MHz: 1 MHz is fine for NLC July 14 2003 US LC Workshop Cornell U – Chris Damerell 6 electronics only at the ends of the ladders bump-bonded assembly between thinned CPCCD and readout chip readout chip does all the signal processing, yielding sparsified digital data CPCCD is driven with high frequency, low voltage clocks low inductance layout required for clock delivery July 14 2003 US LC Workshop Cornell U – Chris Damerell 7 Standard 2-phase Field-enhanced 2-phase implant implant (high speed) Features of our first CPCCD: Metallised gates (high speed) • 2 different charge transfer regions • 3 types of output circuitry Source followers Direct 2-stage source followers Readout ASIC Source followers Metallised gates (high speed) Direct Readout ASIC To pre-amps • Independent CPCCD and readout chip testing possible: •without readout chip - use external wire bonded electronics • without bump bonding - use wire bonds to readout chip • finally, bump-bonded • Different readout concepts can be tested (direct charge sensing, and voltage sensing via source follower) July 14 2003 US LC Workshop Cornell U – Chris Damerell 8 CPC-1 delivered & under test Direct connections and 2-stage source followers 1-stage source followers and direct connections on 20 μm pitch July 14 2003 US LC Workshop Cornell U – Chris Damerell 9 July 14 2003 US LC Workshop Cornell U – Chris Damerell 10 Single pixel events seen in one column of CPC-1 with 2 V peak-peak clocks July 14 2003 US LC Workshop Cornell U – Chris Damerell 11 Wire/bump bond pads Charge Amplifiers Voltage Amplifiers 250 5-bit flash ADCs FIFO Wire/bump bond pads July 14 2003 US LC Workshop Cornell U – Chris Damerell 12 July 14 2003 US LC Workshop Cornell U – Chris Damerell 13 Thinnest possible detector layers 3 approaches • Unsupported silicon • Semi-supported silicon • Supported silicon Unsupported approach attractive – ‘like wires in a drift chamber’ Works beautifully along ladder length (sagitta stability around 2 microns) However, processed thin CCD is not like a wire: it’s an inhomogeneous membrane in which transverse stresses may lead to somewhat uncontrollable shape Also, we have concerns about handling issues, for attaching readout chips etc Not abandoned, but semi-supported approach may be more practicable July 14 2003 US LC Workshop Cornell U – Chris Damerell 14 July 14 2003 US LC Workshop Cornell U – Chris Damerell 15 Beryllium substrate with adhesive balls Thinned CCD ( 20 μm) CCD brought down Shims Assembly after shim removal and curing Adhesive 0.2mm Beryllium substrate (250 μm) 1 mm July 14 2003 US LC Workshop Cornell U – Chris Damerell 16 July 14 2003 US LC Workshop Cornell U – Chris Damerell 17 Physics studies The design of the VXD should be driven by the physics requirements: • 4 configurations, 5 layer single thickness and 4 layer double thickness, and other combinations • make single muon and pion tracks in Brahms for all momenta and angles. Fit the distributions • include the parametrizations in Simdet • biggest effect comes from removal of the inner layer • provide to physics groups July 14 2003 US LC Workshop Cornell U – Chris Damerell 18 5layers • • 4 layers, double Clear performance difference between configurations Charm suffers most, B tagging is “easy” July 14 2003 US LC Workshop Cornell U – Chris Damerell 19 • New procedure to attach track to vertices • Charged B, up to 89% correct tag, 6-8% worse for 4 layer double thickness configuration • Charged D, excellent purity, less difference between configurations July 14 2003 US LC Workshop Cornell U – Chris Damerell 20 • Neutral B: dipole • Maintain, develop and improve tools • Provide them to the physics community so we can get feedback on detector parameters from various physics channels • Make a transition to Java/JAS environment July 14 2003 US LC Workshop Cornell U – Chris Damerell 21 Summary and future plans • Fast CCDs: • much to study with CPC-1 • tentative plan for design/production of CPC-2 (including detectorscale prototypes, 10x2 cm2) Oct 2003-June 2004 • readout chips CPR-1 and CPR-2 all we need in medium term future • Thin ladders: • semi-supported assemblies with a well-behaved adhesive may be fine, including satisfying the bump-bonding assembly requirements • numerous alternative ideas, some (fortunately) being pursued by other groups – notably the DEPFET collaboration • Physics studies: • totally dependent on available effort, a small but dedicated team • Major opportunities for wider collaboration in all areas, and informally it is happening July 14 2003 US LC Workshop Cornell U – Chris Damerell 22