The H1 Silicon Tracker. Benno List

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The H1 Silicon Tracker Benno List HERA and H1 The H1 silicon tracker Recent results Changes in 2003 Lessons from the Pit VERTEX 2003 15.9.2003 Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 1

The HERA ep Collider Located at DESY in Hamburg 27.5 GeV electrons/positrons on 920 GeV protons HERA I: 1992 2000, 120pb 1 2000: Luminosity upgrade HERA II: 2001 2007, 1000pb 1 expected Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 2

The H1 Detector Hadronic Lar Calorimeter Final State Forward Tr. Central Tracker Scattered Electron 27.5GeV Positrons 920GeV Protons SpaCal Forward Central Backward Silicon Tracker Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 3

FST: Extend tracking (with vertexing capability) into forward direction: high track density! => good pattern recognition CST: Physics Requirements (I) Provide vertexing capability in central region (charm, beauty) Resolution dominated by multiple scattering: thin detector! Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 4

BST: Physics Requirements (II) Measure and trigger scattered electron at low angles: suppress fake electrons from π 0 γγ Generally low track density in backward direction Separation of pions and elctrons by measuring energy E in the calorimeter and momentum p in BST. D. Eckstein, DESY THESIS 2002 8. Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 5

FST: Forward Silicon Tracker Collaboration of DESY Zeuthen, DESY, Prag, RAL Electronics Sensor Wheels 7 sensor wheels, 2 types: u/v and r 3384cm 2 silicon from CIS (Erfurt) 92160 channels Readout with APC (Analog Pipeline Chip) developed at PSI Proton Beam SACMOS: 1.2µm CMOS Manufactured by Faselec Connectors (Electrical + Cooling) Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 6

FST Sensor types 5 wheels with u/v coordinate: single sided silicon, back to back good signal/noise 2 wheels with r strips single sided silicon readout with 2nd metal layer reasonable S/N needed for pattern recognition in high multiplicity events (ambiguity resolution) r sensors u/v sensors Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 7

BST/FST Sensor Wheel Beamspot Synchrotron radiation fan Asymmetric hole to accomodate elliptical beampipe Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 8

FST Performance Signal/Noise: 30 for u/v detectors 15 for r detectors Resolution 12µm (from triplet sagitta) 6 tracks in 1 φ sector Drift chamber FST CST A multitrack event reconstructed in the FST Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 9

BST: Backward Silicon Tracker Sensor Wheels Electronics Electron Beam 6 wheels with u/v coordinates, same as in FST: tracking no r wheels needed, typically low multiplicity in backward direction 4 wheels with pad detectors: triggering Hit detection + track finding done on frontend, at 10.4MHz Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 10

BST 1, 2, 3 BST 1: Installed 1995: 4 wheels of r detectors 16 sensors = 64 sensors, 40960 channels BST 2: Upgrade 1998: 4 + 4 wheels of r detectors 16 sensors = 128 sensors, 81920 channels 8 prototype φ sensors (u coordinate): 5120 channels Upgrade 2001: 8 wheels of r detectors 12 sensors = 96 sensors, 61440 channels BST Pad: 4 wheels of pad detectors 12 sensors: 48 sensors, 1536 pads BST 3: Upgrade 2003: 6 wheels of u/v detectors 12 sensors = 132 sensors, 84480 channels BST Pad: 4 wheels of pad detectors 12 sensors: 48 sensors, 1536 pads Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 11

BST Pad Hit Detection ASIC PRO/A: 1.2µm CMOS process from IDE AS (Oslo) 32 channels per chip noise: 600e + 15e/pF shaping time 30ns Pad sensors: 8 4=32 pads Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 12

BST Pad Trigger Concept One motherboard for 2 sectors (8 sensors), mounted directly behind sensor volume Complex Programmable Logig Devices (CPLDs) from ALTERA for trigger Recognises tracks from IP Rejects tracks from outside interaction region Flexible, for shifted vertex runs Uses Content Adressable Memory (CAM) to compare hit patterns with predefined hit patterns from tracks Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 13

The CST 2 barrel layers, 12+20 ladders 192 sensors 3.4x5.9cm 2 3850cm 2 silicon 3 sensors read out together 81920 channels Very thin: 1.4% X 0 in radial direction Analog readout with rad hard DMILL APC manufactured by ATMEL Optical signal transmission Built by ETH Zurich, PSI, Uni. Zurich, DESY, RAL Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 14

Shutdown Work on CST March June 2003: 17 weeks shutdown CST: Repairs, upgrade to radhard readout: Last 12 of 64 half ladders were equipped with radiation hard (DMILL) readout chips; now all CST readout ASICs are DMILL chips Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 15

Backgrounds Silicon Trackers Collimator against backscattered synchrotron radiation 0.3m IP Proton beam Electron beam 43m Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 16

Radiation Damage to BST Dosimeters in BST showed up to 30kGy of dose High dose only in small region at z end (around collimator), FST, CST, forward region of BST received <100Gy Damages: APC chips of BST: do not hold charge long enough (1ms) for readout (same problem lead to installation of radhard chips in CST) BST slow control circuitry damaged line receivers, drivers damaged ALTERA CPLD chips survived! Voltage regulators for CST damaged (located at same z position as BST electronics) Proton beam Collimator BST radiation doses in Gy Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 17

Beam optimization using BST Pad Rates Use single pad rate to monitor beam conditions Very useful for beam tunig Problem: Large background spikes (from beam missteering) deprogram CPLDs This was an unforeseen application, shows advantage of CPLDs: can be easily adapted to new demands Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 18

Summary HERA II had a slow start, but is now on track Radiation damage occured mainly from an incident where synchrotron radiation directly hit a collimator Normal operation of HERA leads to doses ~100Gy/y BST and CST have been repaired CST now fully equipped with DMILL chips Looking forward to next data taking Benno List, ETH Zürich Vertex 2003, 14. 19.9.2003: The H1 Silicon Tracker Page 19