Title: G. Drake Electronics for Next-Generation Telescopes Oct. 21, 2005 p. 1
1(No Transcript)
2Instrumentation Concepts
- Present Photo-Detectors are Typically
Single-Anode PMTs - Telescope Mirrors Focus Light onto Photo-Cathodes
- PMT Signals are Digitized (8-12 Bits) using FADCs
- Veritas 500 MHz FADC Provides 2 nS Timing
Veritas Telescope 1 Images Courtesy of Liz Hayes
Veritas
3Instrumentation Concepts
- Photo-Detectors for Next Generation Telescopes
- It is Desirable to Increase the Angular
Resolution of the Images - Measure Lower Energies
- Reduce Background
- Implies
- Smaller Pixels 0.15 ? lt
0.05 - More Channels for Same FOV
500 - 1000 ? 10,000 - The Technology is Here Now, and Continues to
Advance - Multi-Anode PMTs
- Multi-Channel Plates
- Silicon PMTs
- APDs
Hamamatsu H8500 64 anode PMT
Pixel (5.8mm)2
Burle Planacon Micro-Channel Plate
85011-501 64 anode
PMT Pixel (6mm)2
- Common in HEP, Need RD for Future Telescopes
4Instrumentation Concepts
- Photo-Detectors for Next Generation Telescopes
Teststand at Argonne
5Instrumentation Concepts
- Photo-Detectors for Next Generation Telescopes
- High-Density Photo-Detectors
- Will Require High-Density
- Electronics
- More Circuitry per Unit Volume
- Short Connections to Detector to Enhance
Performance - Level 0 Triggering -
Zero-Suppress at Front End - Data Stream Out to Back-End
- Need Low Power
- High Channel Count
The Present
Front-End Electronic Packaging for HESS
- Circuitry On-Board Photo-Detector
The Future
Front-End Electronics Mounted on Base
- Need for Custom Integrated Circuit
6Instrumentation Concepts
- Application-Specific Integrated Circuits
(ASICs)
- Mature Technology
- ASICs Have Been Around Since Mid-1980s
- 7 micron ? 0.12 micron
- CMOS, Mixed Bipolar/CMOS,
Silicon Germanium, Gallium Arsenide - Multi-Project Submission Services Cater to
Teaching Prototyping ? MOSIS - Foundries Cater to Production
7Instrumentation Concepts
- The Pros Cons of Using an ASIC
- The Pros
- High-Performance Circuitry
- Small Size
- Low Power
- Inexpensive for Large Quantity
Production - The Cons
- Long Learning Curve for Tools
- High Cost of Tools (0 for Educational
Institutions) - Development Time 1-2 yrs.
- Need Special Test Facilities
- Cost-Effective Only for Very Small Quantities
(Prototype) or Very Large Quantities
Photo of DCAL ASIC for Linear Collider
Courtesy of Ray Yarema, Fermilab
- Telescope Instrumentation Project
- is in On-Par with
- Large HEP Experiments,
- Where ASICs are Used Routinely
- Significant Capital Investment
8Instrumentation Concepts
- Traditional Pulse-Height Digitization
- Good Pulse-Height Resolution
- Complex Circuitry
- High-Speed High Power
- Lots of Bits to Read Out
- Difficult to Trigger
- Correction Overheads Pedestals, Calibrations,
Linearity
- A New Idea Digital Imaging / Photon
Discrimination (Swordy) - Assume Small Pixel Size (Required)
- Most of Time, Single pes Will Hit Individual
Pixels, True For Signal,
Noise, and Background - Instrumentation Each Pixel Has A Discriminator,
Efficient at 1 pe
9Instrumentation Concepts
- A New Concept Digital Imaging
Pulse-Height Temperature Plot
Hit Map
(Artists Conception)
10Instrumentation Concepts
- A New Concept Digital Imaging (Cont.)
Low Energy Signals
Pulse-Height Temperature Plot
Hit Map
(Artists Conception)
11Instrumentation Concepts
- A New Concept Digital Imaging (Cont.)
Noise (Dark Current NSB) Rejected by Level 0
Trigger
(Artists Conception)
12Instrumentation Concepts
- A New Concept Digital Imaging (Cont.)
- Strengths in Approach
- Greatly Reduced Background per Pixel
- Very Simple Electronics
- Greatly Reduces Data Volume
- Relatively Easy to Trigger
- Difficulties, Additional Thoughts, Ideas,
Studies - Shape of Hit Pattern as a Function of Energy?
- Time Over Threshold for Crude Pulse Height?
- Fold in View from Multiple Telescopes (Yes)
- Pulse Height Digitization of Dynode?
- Use of Out-Riggers for Pulse Height Measurement?
- Issues with QE, Gain Uniformity, Single pe
Response
- Simulations Studies in Progress
13Instrumentation Concepts
- Basic System Requirements Design Choices
- Nature of Data Timestamp Hit Pattern (Chip ID
Appended Later) - Timing Resolution 1-2 nS
- Raw Data Rate 1 - 10 MHz per Pixel
- Overall Output Data Rate 1-10 KHz (After
L0/L1 Trig) - Live Time 100 (_at_ Max Event Rate)
- Triggering
- Level 0 1. More Than 1 Pixel Hit in a Time
Window - 2. Geometrical Constraints
- Level 1 Trigger from Neighboring
Photo-Detectors - Data Output High-Speed Serial Link, Possibly
Fiber - Event Selection Filtering High-Level
Triggering in Back-End, - Using
Timestamps and Geometrical Mapping -
14Conceptual Design of ASIC
- Front End Amplifier Discriminator Senses Hits
Above Threshold - 30-Bit Timestamp Counter Runs at 500 MHz
- Comparator States Clocked into Shift Register -
Buffer for Trigger Decision, 1000 Stages (2 usec) - Save States Timestamp on Ext. Trig. or
Self-Trigger - Counters Reset Once per Sec, Synchronously Across
System - Serial Data Output 100 Mbit/sec, 94
Bits/Event, 1 uSec/Event - Serial I/O Separate Data, Control, Trigger
- Services 64 CH
15Conceptual Design of ASIC
- Similar in Concept to Chip Development in
Progress for Linear Collider ? DCAL - Collaboration with FNAL ASIC Design Group
- Design Work Being Done by Abder Mekkaoui Jim
Hoff
- New Chip Must be Faster
- 0.13 micron SiGe
16Conceptual Design of ASIC
Draft
- Discussions with FNAL ? They are Interested!
- Work in Progress on Establishing Another
Collaboration with FNAL ASIC Design Group - Design Work Could Begin in 2006
- First Stage Develop Models, Sims, Basic Design
- Proof-of-Principle for 2nd Stage Funding
17Summary
- Photo-Detector Technology is Advancing,
- From Which Future Telescopes Can Benefit
- New Telescopes Will Need Smaller Pixels,
- Higher Level of Electronics Integration
- Custom ASICs Are Common Now in
- High-Performance Instrumentation
- Preliminary Design Work RD to Begin Soon
- Leverages Resources of National Labs
- High-Level Integration, High Channel Count, Low
Power