SCIPP R&D on Linear Collider Tracking – Hardware and Simulation

1. SCIPP R&D on Linear Collider Tracking – Hardware and Simulation DOE Site Visit June 10 2008 Bruce Schumm Santa Cruz Institute for Particle Physics

2. Support Recently, ILC R&D has been supported at fluctuating levels by the DOE’s Linear Collider R&D (LCRD) program 2006-2007: We received $53,000 in regular funding, and received another $37,500 in supplemental funding 2007-2008: We received $67,000 in regular funding. And another $50,000 in supplemental funding. 2008-2009 No call yet for proposals.

3. The SCIPP/UCSC SiLC/SiD GROUP (Harwdare R&D Participants) Faculty/Senior Vitaliy Fadeyev Alex Grillo Bruce Schumm Post-Docs Lei Wang Undergrads Greg Horn Luke Kelley Ian Horn Sean Crosby Jerome Carmen Lead Engineer: Ned Spencer Technical Staff: Max Wilder, Forest Martinez-McKinney All participants are mostly working on other things (BaBar, ATLAS, biophysics, Undergraduate major…) Students are undergraduate physics majors at UCSC

4. FOCUS AND MILESTONES Goal: To develop readout generically suited to any ILC application (long or short strips, central or forward layers) • Current work focused on long ladders (more challenging!): • Front-end electronics for long (~1 meter) ladders • Exploration of sensor requirements for long ladders • Demonstration (test-beam) of < 10 m resolution mid-2008 After long-ladder proof-of-principle, can re-optimize (modest changes) for short-ladder, fast-rate application We also hope to play an increasing role in complementary hardware effort (KPiX, SiD sensor development)

5. Silicon Microstrip Readout R&D • Initial Motivation • Exploit long shaping time (low noise) and power cycling to: • Remove electronics and cabling from active area (long ladders) • Eliminate need for active cooling SiD Tracker

6. BRIEF SUMMARY OF STATUS • Testing of 8-channel (LSTFE-1) prototype completed: • Reproducible operation (4 operating boards) • Most features working, with needed refinements understood • A number of “subtleties” (e.g. channel matching, environmental sensitivity) under control • Starting to make progress on fundamental issues confronting long-ladder/high-resolution limit. • 128-channel test-beam prototype (LSTFE-2) has been fabricated; bench tests getting underway • Now for the details…

7. The LSTFE ASIC Process: TSMC 0.25 m CMOS 1-3 s shaping time (LSTFE-I is ~1.2 s); analog measurement is Time-Over-Threshold

8. 128 mip 1 mip Operating point threshold Readout threshold 1/4 mip High gain advantageous for overall performance (channel matching)

9. Simulated Resolution for 167 cm Ladder Detector Noise: Capacitive contribution; from SPICE simulation normalized to bench tests with GLAST electronics Detector Resolution (units of 10m) Analog Measurement: Provided by time-over-threshold; lookup table provides conversions back into analog pulse height (as for actual data) RMS Gaussian Fit Lower (read) threshold in fraction of min-i (High threshold is at 0.29 times min-i)

10. DIGITAL ARCHITECTURE: FPGA DEVELOPMENT Digital logic under development on FPGA (Wang, Kroseberg), will be included on front-end ASIC after performance verified on test bench and in test beam.

11. Li Hi Li+1 Hi+1 Li+2 Hi+2 Li+3 Hi+3 Li+4 Hi+4 Li+5 Hi+5 Li+6 Hi+6 Proposed LSTFE Back-End Architecture Low Comparator Leading-Edge-Enable Domain 8:1 Multi-plexing (clock = 50 ns) FIFO (Leading and trailing transitions) Event Time Clock Period  = 400 nsec

12. Note on LSTFE Digital Architecture Use of time-over-threshold (vs. analog-to-digital conversion) permits real-time storage of pulse-height information.  No concern about buffering  LSTFE system can operate in arbitrarily high-rate environment; is ideal for (short ladder) forward tracking systems as well as long-ladder central tracking applications.

13. INITIAL RESULTS LSTFE chip mounted on readout board FPGA-based control and data-acquisition system

14. EQUIVALENT CAPACITANCE STUDY Noise vs. Capacitance (at shape = 1.2 s) Measured dependence is roughly (noise in equivalent electrons) noise = 375 + 8.9*C with C in pF. Experience at 0.5 m had suggested that model noise parameters needed to be boosted by 20% or so; these results suggest 0.25 m model parameters are accurate  Noise performance somewhat better than anticipated. Expected Observed 1 meter

15. Power Cycling (with Small Injected Current for now) It is essential to turn off chip for the 99% of the time that the beam is not there  Must be able to turn chip back on in 1 millisecond! Power Control Preamp Response Shaper Response Solution in hand to maintain bias levels in “off” state with low-power feedback; will eliminate need for external trickle current

16. LONG LADDER CONSTRUCTION

17. Measured noise Noise calculation assuming 20m strip width (actual is 60 m) 72 cm Ladder Sum of estimates Projected Johnson noise for 20 m strip (not part of estimate) 143 cm Ladder Estimated Johnson noise for actual 65 m strip (part of estimate) Measured Noise vs. Sum of Estimated Contributions

18. Strip Noise Idea: “Center Tapping” – half the capacitance, half the resistance? Result: no significant change in measured noise Expected noise, assuming 75% reduction in strip noise Measured noise

19. Strip Noise Study: Smaller Pitch Detector Sensors used so far have 237 m pitch (GLAST test sensors Currently developing faux long-ladder with old CDF L00 sensors, with 60 m pitch  strip noise should dominate Involves microscopic alteration to biasing circutry, implementation of low-noise readout (Sean Crosby) General study of effect of strip resistance on readout noise (generic ILC R&D)

20. Summary/Outlook [Hardware effort] LSTFE-2 back in lab; testing getting underway Generic R&D study of strip noise underway Development of FPGA-based readout and Data Acquisition system (test-beam) underway (Wang, Kelley) Independent project to explore charge division (longitudinal coordinate) for special SiD sensor run underway (Jerome Carmen) Hoping to visit testbeam by end of calendar year (recent ILC upheavals at Labs have introduced uncertainties)

21. Tracking Simulation Studies at UC Santa Cruz • Non-prompt tracks with SiD

22. People and Contributions Work done by UCSC thesis students supervised by Schumm Lori Stevens: “Virtual” Z segmentation studies Tyler Rice, Chris Meyer: Calorimeter-assisted tracking algorithm Chris Betancourt: Application to Gauge- Mediated SUSY models

23. Non-Prompt Tracks with the SiD About 5% of tracks originate outside the 2nd layer of the VXD. Is the SiD able to reconstruct these?

24. Prior Tools Stand-alone (no Vertex Detector) reconstruction: AxialBarrelTracker (Tim Nelson, SLAC; optimized by Rice, Meyer) Calorimeter stub-finding within Garfield package (Dima Onoprienko; Kansas State) Work within ILC “Java Analysis Studio” (JAS) framework

25. Z Segmentation (Lori Stevens) Can we use z-segmentation to further clean up seeds and eliminate fake tracks? Can we make 4-hit tracks usable? For now, apply only to three-hit seeds… Note: Not actual spacing between modules Hit 1 Hit 2 Possible modules for following hits

26. Non-Prompt Track Effieciency vs. Segmentation Lori Stevens

27. 3-Hit Tracks & Non-Prompt Signatures Probably need 5+1 layers for prompt track If we require 4 hits for non-prompt tracks, sensitive region for kinked tracks is very limited.

28. Seeds-to-Stubs Program UCSC students proposed matching precise three-hit tracker seeds to Garfield stubs • Helix – Stub Matching (optimized for Z  qq) • Base Difference < 2 mm • Phi Difference < 100 milliradians • Curvature Ratio ( (seed - stub)/ seed ) < 10 e.g.: Position-matching for isolated muons (mm)

29. Seed-to-Stubs Performance; Z  qq • Of a total of 20 3-hit particles: • 12 were reconstructed as 3-hit tracks, with only 4 fakes • Two additional 4-hit particles were found • BUT: Performance much worse for e+e-  qq at Ecm = 500 GeV. Could optimize for this type of event, but do we want to? •  Algorithm tuning dependent on signature under exploration

30. Seed-to-Stubs Performance; Z  qq • Of a total of 20 3-hit particles: • 12 were reconstructed as 3-hit tracks, with only 4 fakes • Two additional 4-hit particles were found • Chris Betancourt applying Seed-to-Stubs algorithm to physics process with kinked tracks • Currently generating Stau  tau gravitino events with ~10cm mean decay length (signal) and e+e- + - (background)

31. Simulation effort Summary • UCSC Undergraduates making important contribution to development of SiD detector. • Attracts best students and propels them on: • Lori Stevens: SLAC Pope Fellowship, Berkeley engineering grad • Tyler Rice: Dean’s award for thesis, UC Irvine physics grad with Chancellor’s fellowship • Chris Meyer: University of Chicago physics grad; will join ATLAS at CERN this summer with Merritt/Oreglia

32. Pulse Development Simulation Christian Flacco & Michael Young (Grads); John Mikelich and Luke Kelley (Undergrads) Long Shaping-Time Limit: strip sees signal if and only if hole is collected onto strip (no electrostatic coupling to neighboring strips) Include:Landau deposition (SSSimSide; Gerry Lynch LBNL), variable geometry, Lorentz angle, carrier diffusion, electronic noise and digitization effects

33. RANDOM BACK-UP SLIDES

34. Comparator S Curves Vary threshold for given input charge Read out system with FPG-based DAQ Get 1-erf(threshold) with 50% point giving response, and width giving noise Qin= 1.0 fC Qin= 0.5 fC Qin= 1.5 fC Qin= 2.0 fC Stable operation to Vthresh ~ 5% of min-I Qin= 2.5 fC Qin= 3.0 fC Hi/Lo comparators function independently

35. Tracking Performance Package Package is C++/ROOT written by Chris Meyer (UCSC physics major) Reads in platform-independent flat file with specific format (output by JAS, …) Flat file includes all relevant particles (MC) and tracks, with two-way MC Truth cross-referencing, and track/particle attributes Also reads in error-matrix information in cos/p grid (e.g. from LCDTRK)

36. Some examples… Efficiency vs.  500 GeV uds pT > 0.75 GeV pT > 5.0 GeV  = angle between jet axis and track

37. “Tri-Plots” (fitting validation)

38. TIME-OVER-THRESHOLD READOUT SUMMARY • The LSTFE readout system is: • Universally applicable (long strips, short strips, central, forward, SiD, LDC, GLD, 4th…) • Rigorously optimized for ILC tracking • Relative simple (reliability, yield) • In a relatively advanced stage of development • Is now being used as an instrument to understand fundamental principles of long ladder operation, particularly for narrow strips (CDF Layer00 sensors available, being qualified)

39. AxialBarrelTracker Effieciency Studies Out of 304 “findable” particles in Z0 bb events “Found”: associated with a track, with at most one hit coming from a different particle. “Fake”:Any non-associated track with pt>0.75 and DCA < 100mm. Particles Fakes Found 5 Hits 131 (43%) 1 Found 4 Hits 100 (33%) 270 Not Found 73 (24%) ----- • Find 43% of particles • Four-hit tracks seem difficult

40. c The Gossamer Tracker • Ideas: • Low noise readout  Long ladders  substantially limit electronics readout and support • Thin inner detector layers • Exploit duty cycle  eliminate need for active cooling Competitive with gaseous tracking over full range of momentum (also: forward region) Alternative: shorter ladders, but better point resolution

41. Alternative: shorter ladders, but better point resolution • The LSTFE approach would be well suited to use in short-strip applications, and would offer several potential advantages relative to other approaches • Optimized for LC tracking (less complex) • More efficient data flow • No need for buffering Would require development of 2000 channel chip w/ bump bonding (should be solved by KPiX development)

42. Sources of Inefficiency Restrict to particles that hit all five layers: 166 Findable MC Particles (304 before requirement) 113 Found with 5 hits (68% vs. 43%) 25 Found with 4 hits (15% vs. 33%) 28 Missed (17% vs. 24%) Also require all three “seed” hits to be from same particle: 144 Found with 5 hits (87% vs. 43%) 15 Found with 4 hits (9% vs. 33%) 7 Missed (4% vs. 24%)

43. Improving AxialBarrelTracker Efficiency For the vast majority of particles, all hits are within /2 of one another in azimuth (). Make this restriction… Some improvements in efficiency and reduction of fakes…

44. AxialBarrelTracker Effieciency Application of segment consistency to seeds provides improvement, but only for lengths less than 10cm

45. LSTFE-2 DESIGN LSTFE-1 gain rolls off at ~10 mip; are instituting log-amp design (50 mip dynamic range) Power cycling sol’n that cancels (on-chip) leakage currents Improved environmental isolation Additional amplification stage (noise, shaping time, matching Improved control of return-to-baseline for < 4 mip signals Multi-channel (64? 128? 256?) w/ 8:1 multiplexing of output Must still establish pad geometry (sensor choice!)

46. Note About LSTFE Shaping Time • Original target: shape = 3 sec, with some controlled variability (“ISHAPR”) • Appropriate for long (2m) ladders In actuality, shape ~ 1.5 sec; tests are done at 1.2 sec, closer to optimum for SLAC short-ladder approach Difference between target and actual shaping time understood in terms of simulation (full layout) LSTFE-2 will have ~3 sec shaping time

47. Power Cycling • Idea: Latch operating bias points and isolate chip from outside world. • Per-channel power consumption reduces from ~0.5 mW to ~5 W. • Restoration to operating point should take ~ 1 msec. • Current status: • Internal leakage (protection diodes + ?) degrades latched operating point • Restoration takes ~40 msec (x5 power savings) • Injection of small current (< 1 nA) to counter leakage allows for 1 msec restoration. • Future (LSTFE-2) • Low-current feedback will maintain bias points; solution already incorporated in LSTFE-2 design

48. LONG LADDER EXPERIENCE • A current focus of SCIPP activity • Using GLAST “cut-off” (8 channel) sensors; 237 m pitch with65 m strip width • Have now studied modules of varying length, between 9cm and 143cm. • Measure inputs to estimate noise sources other than detector capacitance: • Leakage current 1.0 nA/cm • Strip resistance 3.1 /cm • Bias resistance 35 M per sensor • All of these should be considered in module design! • Strip resistancefor fine pitch could be an issue  are doing dedicated studies and considering options  feedback to detector/module design.

49. Simulation Result: S/N for 167 cm Ladder (capacitive noise only) Simulation suggests that long-ladder operation is feasible

50. Timing Resolution Study (50 pF Load) Nominal expectation: where  = 1.2 s is the shaping time,  = 8.8 is the applied threshold in units of rms noise, and SNR = 28. This yields an expectation of t ~ 60 ns (expected) t was measured at a series of input charges, which were averaged together with weights from a Landau distributions, yielding t ~ 50 ns (measured)