glast lat readout electronics marcus zieglerieee 2005 1 scipp the silicon tracker readout...
Post on 21-Dec-2015
218 views
TRANSCRIPT
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 1
SCIPPSCIPP
The Silicon Tracker Readout The Silicon Tracker Readout Electronics of the Gamma-ray Electronics of the Gamma-ray Large Area Space TelescopeLarge Area Space Telescope
Marcus Ziegler
Santa Cruz Institute for Particle PhysicsUniversity of California at Santa Cruz
GLAST LAT Collaboration
Gamma-ray Large Gamma-ray Large Area Space Area Space TelescopeTelescope
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 2
SCIPPSCIPPGLAST LAT Tracker OverviewGLAST LAT Tracker Overview
e+ e–
The LAT Tracker is divided into:
- 16 Tracker Towers
- Each stack is composed of 19 trays.
Tray:
- Carbon-composite panel
- Si-strip detectors on both sides
- On the bottom side of the tray, is glued an array of tungsten foils.
- Adjacent trays are rotated by 90o, with a 2mm gap in between, to form an x,y measurement plane.
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 3
SCIPPSCIPPOne Tracker TowerOne Tracker Tower
Requirements for GLAST:
Power < 200 W/channel
Efficiency > 98%
Noise occupancy < 5x10-5
Self triggering
Trigger rate up to 10 kHz
Minimal dead area
Minimize single point failures
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 4
SCIPPSCIPPCharacteristics of the Si-TrackerCharacteristics of the Si-Tracker
• 9126 Si-strip detectors from 6” wafers
• 74 m2 of Si (228m pitch)
• 884 736 readout channels
• 160 Watt power consumption
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 5
SCIPPSCIPPReadout SchemaReadout Schema
GTFE GTFE GTFE GTFE GTFE GTFE
GTRC
GTFE GTFE GTFE GTFE GTFE GTFE
GTRC
GTFE GTFE GTFE GTFE GTFE GTFE
GTRC GTRC
GTRC
GTRC
Data and trigger signalsControl signals
• 9 MCMs per side of the tower and 24 GTFE chips per MCM board • All front end chips can be programmed at any time from both sides• The layer OR is used as a trigger primitive (6 layer in a row form the usual tracker trigger)• The strip hits can be latched in one of the four GTFE readout buffers and be read out to both sides• Measure of the deposited charge by counting the clock ticks the layer OR is high
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 6
SCIPPSCIPPRight Angle InterconnectRight Angle Interconnect
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 7
SCIPPSCIPPDetail of an MCM, at One EndDetail of an MCM, at One End
Omnetics connector
Pitch-adapter flex circuit with 90° radius
GTRC ASIC
GTFE ASIC
Polyswitch
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 8
SCIPPSCIPPMechanical ChallengesMechanical Challenges
Flex Circuit
Internal Cu Planes
ASIC and Conductive Glue
Wire Bond
Encapsulation FillEncapsulation Dam
Fiberglass
Fiberglass Riser
• X-ray cross section of the edge of the MCM with the right angle interconnect.
• 1-layer Kapton flexible circuit that is glued over 1mm radius machined into the edge of the polyimide-glass PWB.
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 9
SCIPPSCIPPSystem PerformanceSystem Performance
Power consumption:
A low (<200 W / channel) power consumption was achieved by keeping the amplification and digitization schemes very simple.
→ The power consumption of a typical tracker tower during data taking is measured to be 9.9 W
Noise Performance:
The shaper output peaking time is about 1.5 s.
For 36 cm long Si strips (about 41 pF load) the noise charge is about 1500 electrons.
The most probable signal is 32,000 electrons for a MIP passing through 400 m silicon.
Noise Occupancy:
The average fraction of channels above threshold at any snapshot in time.
For a typical integrated tracker module we measured a noise occupancy of 4.7x10-7
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 10
SCIPPSCIPPDetection efficiencyDetection efficiency
The fraction of active area within one plane of 16 SSDs is 95.5 %
Taking into account the dead area between the towers the active fraction of the over all tracer is 89.4 %
Hit efficiency
The overall efficiency was measured for each layer using cosmic-ray tracks.
We obtained efficiencies for the individual towers of about 99.6%
Inefficiency comes from dead channels and low fluctuations in the ionization.
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 11
SCIPPSCIPPPhoton event Photon event
GLAST LAT Readout Electronics
Marcus Ziegler IEEE 2005 12
SCIPPSCIPPCurrent statusCurrent status
All 16 tracker towers (TKR and CAL) are installed into the lat (next is ACD)
LAT integration completion in Jan 2006
Environmental testing at NRL until June 2006
Launch in August 2007