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Recent Achievements of the ATLAS Upgrade Planar Pixel Sensors R&D Project

Recent Achievements of the ATLAS Upgrade Planar Pixel Sensors R&D Project . Gianluigi Casse. on behalf of the ATLAS PPS R&D Collaboration. Acknowledgements : PPS Collaboration Members . MPP & HLL Munich (Germany) Università degli Studi di Udine – INFN (Italy) KEK (Japan)

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Recent Achievements of the ATLAS Upgrade Planar Pixel Sensors R&D Project

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  1. Recent Achievements of the ATLAS Upgrade Planar Pixel Sensors R&D Project GianluigiCasse on behalf of the ATLAS PPS R&D Collaboration IPRD13 - 7-10 Oct. 2013, Siena

  2. Acknowledgements: PPS Collaboration Members • MPP & HLL Munich (Germany) • UniversitàdegliStudi di Udine – • INFN (Italy) • KEK (Japan) • Tokyo Inst. Tech. (Japan) • IFAE-CNM, Barcelona (Spain) • University of Liverpool (UK) • University of Glasgow (UK) • UC Berkeley/LBNL (USA) • UNM, Albuquerque (USA) • UCSC, Santa Cruz (USA) • PPS’s participating members: • CERN • AS CR, Prague (Czech Rep.) • LAL Orsay (France) • LPNHE (France) • University of Bonn (Germany) • HU Berlin (Germany) • DESY (Germany) • TU Dortmund (Germany) • University of Göttingen (Germany) • University of Geneva (CH) IPRD13 - 7-10 Oct. 2013, Siena

  3. ATLAS Planar Pixel Sensor Project GOALS • Prove Planar Technology for all radii of HL-LHC with rad-hard geometries (n-in-n, n-in-p) • Geometry optimization: Slim/Active edges for improved tiling, other optiimisations. • Productions • CiS, MPI-HLL, MICRON, HPK, VTT • Irradiations • Reactor neutrons (Ljubljana) • 26 MeV protons (Karlsruhe) • 800 MeV protons (Los Alamos) • 24 GeV protons (CERN) • 70 MeV protons (CYRIC) • 26 MeV protons Cyclotron (Birmingham) • Advanced simulations • TCAD packages with radiation parameters • Cost reduction TOOLS • Lab and test beam measurements Radioactive sources • 120 GeV π (CERN) • 4 GeV e- (Desy) • Eudet telescope IPRD13 - 7-10 Oct. 2013, Siena

  4. ATLAS Planar Pixel Sensor Project Silicon Planar technology for ATLAS upgrade pixels?? Have you seen the requirements? Simone Martini ( c. 1284 – 1344) IPRD13 - 7-10 Oct. 2013, Siena

  5. Phase-II Upgrade Pixel Detector Outer radii: 2 layers Layer 3 & 4: 2940 4-chip modules Issues: large scale production of cheap thinned modules 1.7x1015n/cm2; 0.9MGy Barrel pixels: 5.1 m2 silicon area Forward pixels 6 disks per side 552 6-chip modules 280 4-chip modules 3.1 m2 silicon area Issues: large scale production of cheap thinned modules 1.8x1015n/cm2; 0.9MGy Inner radii: 2 layers Layer 1: 352 2-chip modules Layer 2: 576 4-chip modules Issues: radiation damage & small pixels 1.4x1016n/cm2; 7.7MGy NOTE: ATLAS applies a safety factor of 2 to the estimated doses for detector qualification! IPRD13 - 7-10 Oct. 2013, Siena

  6. Requirements • 2 outer Barrel layers / Disks • Sensor planar n-in-p • Pixel size 50 μm x 250 μm • 150 μmthicknesss • ROIC FE-I4X; 2x2cm2 thickness 150 μm • ToT = 4 bits • 2x2 FE-I4 (Quad) ~4x4cm2 • Data rates of 640 Mbit/s per module • 2 Inner Barrel layers • Sensors All sensor materials possible 150 μm silicon or thinner • Pixel size 25 μm x 150 μm • ROIC thickness 150 μm • ToT = 0-8 bits • 2x1 and 2x2 chip modules • Data rate as high as 2 Gbit/s per module Phase-II upgrade ATLAS Current ATLAS IPRD13 - 7-10 Oct. 2013, Siena

  7. N-in-N vs N-in-P • Single sided process • No backside-alignment needed • More foundries available Easier handling/testing, due to lack of patterned back-side implant • Cost-effective • Danger of sparks between chip and sensor ? • Double sided process (more expensive, up to 40%) • Pixel can be shifted below guard-rings • Used already widely (ATLAS, CMS, ...) Issues to compare: Radiation hardness Prevention of edge sparks Edge Cost and handling IPRD13 - 7-10 Oct. 2013, Siena

  8. Radiation hardness and thickness It is well documented that radiation hardness is improved (after high fluences) by thinning the sensors. Good for reducing the material. Radiation hardness of n- and p-type substrates and optimal thickness for the pixel layers is investigated. IPRD13 - 7-10 Oct. 2013, Siena

  9. Radiation hardness of n-in-n and n-in-p sensors • Produced at CiS285 μm • Irradiated up to 2 · 1016neq/cm2 Charge as high as 4.2 ke at 1 kV • FE-I4 chip allows for low thresholds of (1-1.5) ke • Hit efficiency fully recoverable by increasing bias voltage • Irradiated with neutrons p to 1016neq/cm2 • Charge exceeds threshold by a factor 2 • Hit efficiency 98.1 % in central region (losses in punch through bias) T. Wittig, “Radiation hardness and slim edge studies of planar n+-in-n ATLAS pixel sensors for HL-LHC”, PIXEL2012 Combined results from MPP and TU Dortmund C. Gallrapp et al., “Performance of novel silicon n-in-p planar Pixel Sensors ”, Nucl. Instrum. Meth. A679 (2012) 29 IPRD13 - 7-10 Oct. 2013, Siena RESMDD, 9-12 October 2012- Florence

  10. Thin n-in-p Sensors with FE-I4 chip [KEK/HPK] R. Nagai, et al., "Evaluation of novel KEK/HPK n-in-p pixel sensors for ATLAS upgrade with testbeam", DOI: 10.1016/j.nima.2012.04.081 S. Terzo et al. (MPI Munich), Planar Pixel Sensors meeting, Paris, 30 Sep. 2013 A. Macchiolo, "Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at HL-LHC", PIXEL2012 IPRD13 - 7-10 Oct. 2013, Siena RESMDD, 9-12 October 2012- Florence

  11. Edge sparking issue • At Pixel 2010 T. Rohe reported discharges between sensor and read-out chip. • BCB: No Discharges observed up to 1000 V • Parylene: Tested up to 700 V, no sparks [1]. (Later, other samples, 1000 V) • Silicon adhesive: No discharges observed up to 1000 V Radiation tolerance might require the application of high bias voltage. This might have the risk of edge sparking due to the proximity of the high voltage edge and the grounded edge of the ROC. Several solutions are envisaged to address this problem both in n-in-n and n-in-p readout geometries. N-in-n : backplane guard rings N-in-p : Coating with parylene Edge implant on the sensor to reduce the voltage. Other coatings: glue, silicone adesive, BCB. Different solutions to be implemented at the detector producer or as a post processing step. Optimal solution to be chosen also based on cost and yield. Y. Unno et al., “Development of novel n+-in-p Silicon Planar Pixel Sensors for HL-LHC”, http://dx.doi.org/10.1016/j.nima.2012.04.061 IPRD13 - 7-10 Oct. 2013, Siena

  12. Geometry optimisation:adaptive pixel size • Compatible with the FE-I4 floor-plan • Better suited to particular z-regions of the barrel or forward disk/wedges regions • R&D towards strixel solutions 25x500 µm2 25x1000 µm2 50x1000 µm2 125x167 µm2 100x125 µm2 To study: inner pixel size, square pixels in forward direction (low R), strixel solutions ... Various pixel sizes, punch through or polysilicon biased, AC and DC coupled, Liverpool IPRD13 - 7-10 Oct. 2013, Siena

  13. Inclined tracks. (High eta). S. Terzo et al., PPS meeting, Paris, 30-09-2013. IPRD13 - 7-10 Oct. 2013, Siena

  14. Testbeam results comparing 50x250 mm2 and 25x500 mm2 Cluster Size X Cluster Size Y • As expected : • greater number of 2 hit clusters along Y in 500x25 (VTT10) • Increased charge sharing • Minimal change in cluster size in x-direction • (500x25 cluster size is slightly more skewed to 1 than 250x50(VTT5) ) H. Hayward, "Hiroshima" Symposium – HSTD-9, 2013 IPRD13 - 7-10 Oct. 2013, Siena

  15. Residual, efficiency and resolution – 250x50 vs500x25 RMS values are approximately (when the resolution from telescope of the DEY testbeam is accounted for) what is expected for pitch/root(12): 500x25 : 500/√12 = 144.3 250x50 : 250/√12 = 72.17 500x25 : 25/√12 = 7.217 250x50 : 50/√12 = 14.43 Width of distribution 500 for 500x25 and about 250 for 250x50 Efficiency = 0.99673% Efficiency = 0.999369% H. Hayward, "Hiroshima" Symposium – HSTD-9, 2013 Residuals Y [μm] IPRD13 - 7-10 Oct. 2013, Siena

  16. Geometry optimisation:slim or active edges • Reduce need for overlap or inactive gaps (depending on system geometry and location) IPRD13 - 7-10 Oct. 2013, Siena

  17. Slim or Active Edges: Introduction Reducing the distance from the cut edge to the active area can be implemented by guard ring design and edge passivation or by active edges. • Two approaches for active edges • DRIE (Deep Reactive Ion Etching) and side • implantation • DRIE trenching, filling and doping by diffusion • Two approaches (with several variants) to edge isolation • SCP: Scribe-Cleave-Passivate Technology • Backplane Guard-Rings (n-in-n only) Active edge Passivated edge IPRD13 - 7-10 Oct. 2013, Siena

  18. Active edges with planar n-in-p sensors - MPP joint project n-in-p pixels at VTT: active edge process with back-side implantation extended to the edges 100μm thickness Vbreak~120V Vdepl ~7-10 V Charge ~ 6±1 ke A. Macchiolo, "Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at HL-LHC", PIXEL2012 CCE with 90Sr scans IPRD13 - 7-10 Oct. 2013, Siena

  19. Active edges with planar n-in-p sensors FE-I3 MPP - 50 μm edge sensor Vbias=15 V FE-I4 MPP - 125 μmedge sensor Vbias=15 V • Edge pixels show the same charge collection properties as the central ones • Plan to study the hit reconstruction efficiency at the edges with test-beam before and after irradiation A. Macchiolo, "Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at HL-LHC", PIXEL2012 IPRD13 - 7-10 Oct. 2013, Siena

  20. Active Edges Deep trench diffusion (electric field stabilisation) 10 mm width 220 mm depth Polysilicon filling IPRD13 - 7-10 Oct. 2013, Siena

  21. Slim Edges: n-in-n Design Approach • Project by TU Dortmund • Guard Rings are shifted beneath the outermost pixels • Least possible inactive edge ∼ 200μm • Less homogeneous electric field, but charge collection dominated by region directly beneath the pixel implant • Approach adopted in IBL Bottom right: Test design with stepwise shifted pixels, this shows how collected charge is affected due to a less homogeneous electric field when pixels are shifted under the GR’s, bottom left: shows the effect on efficiency for same structure. A. Rummler, Silicon n-in-n pixel detectors: Sensor productions for the ATLAS upgrades, first slim-edge measurements and experiences with detectors irradiated up to SLHC fluences, 6ThTrento Workshop on Advanced Radiation Detectors IPRD13 - 7-10 Oct. 2013, Siena

  22. Slim Edges: SCP • Project by SCIPP (UCSC) and NRL Post-Processing approach • SCP: Scribe-Cleave-Passivate • For n-in-p: ALD deposition of alumina • Relies on: • Low damaged sidewall due to cleaving. • Controlled potential drop along sidewall due to fixed interface charge from passivation. P. Weigell,   "Recent Results of the ATLAS Upgrade Planar Pixel Sensors R&D Project", PIXEL2012 IPRD13 - 7-10 Oct. 2013, Siena

  23. Dry Etch and Alumina Process Y. Unno, 2013/10/01 PPS meeting at Paris Similar process developed By HPK IPRD13 - 7-10 Oct. 2013, Siena

  24. Geometry optimisation:other design variations • Punch-through or resistor (polysilicon) bias of the pixel matrix from a common rail. Mitigation of the inefficiency induced by the bias dot (or resistor). IPRD13 - 7-10 Oct. 2013, Siena

  25. FE-I4 Module Hit Efficiencies Hit efficiency of the module projected in one single pixel cell, Eudet telescope, 120 GeVpions at CERN-SPS (one of many examples from the testbeam activity of PPS groups. Design of the FE-I4 pixel F=4x1015 neq cm-2 400 V Global eff.= 96.5% F=4x1015neq cm-2 500V Global eff.= 96.9% • Main loss of efficiency in the bias dot and in the bias rail  problem is relevant only for perpendicular tracks. A. Macchiolo, "Thin n-in-p pixel sensors and the SLID-ICV vertical integration technology for the ATLAS upgrade at HL-LHC", PIXEL2012 IPRD13 - 7-10 Oct. 2013, Siena

  26. Bias Grid Design To overcome the efficiency loses in the punch through structure for perpendicular tracks, different designs are under investigation: “Bias rail” is a metal over insulator, no implant underneath Dortmund (right) Bias rail routed differently 2 alternative designs KEK (below) PolySilicon resistor (encircling pixel implant) 3 different designs Liverpool (CERN Pixel V mask, mentioned before) PolySilicon resistor (above pixel implant) IPRD13 - 7-10 Oct. 2013, Siena

  27. Summary • The ATLAS Inner Tracker at the HL-LHC will require a whole new detector, with pixel sensors covering an area exceeding 8 m2. Planar pixels are the obvious solution for most of the layers. The PPS project is making exciting progresses in the various issues posed by this extremely demanding detector. LIKE: • Radiation hardness • Diode geometry (n- or p-type substrates) • Study of different pixel geometries that could be part of the ATLAS ITK • Reduced edges • Quad detectors (not mentioned here, at the moment the likely choice for modules) • Cost reduction IPRD13 - 7-10 Oct. 2013, Siena

  28. Summary The PPS groups use simulation, laboratory measurements and test beams to design and test the advanced solutions proposed. A huge effort is performed and here I only mentioned a few highlights of the common activity. IPRD13 - 7-10 Oct. 2013, Siena

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