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The Development of LargeArea PsecResolution TOF Systems

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Title: The Development of LargeArea PsecResolution TOF Systems


1
The Development of Large-Area Psec-Resolution TOF
Systems
  • Henry Frisch
  • Enrico Fermi Institute and Physics Dept
  • University of Chicago

With Harold Sanders, and Fukun Tang (EFI-EDG)
Karen Byrum and Gary Drake (ANL) Tim Credo
(IMSA, now Harvard), Shreyas Bhat, and David Yu
(students)
2
What is the intrinsic limit for TOF for rel.
particles?
Typical path lengths for light and electrons are
set by physical dimensions of the light
collection and amplifying device.
These are now on the order of an inch. One inch
is 100 psec. Thats what we measure- no surprise!
(pictures swiped from T. Credo talk at Workshop)
3
Major advances for TOF measurements
Micro-photograph of Burle 25 micron tube- Greg
Sellberg (Fermilab)
  • 1. Development of MCPs with 6-10 micron pore
    diameters

4
Major advances for TOF measurements
Output at anode from simulation of 10 particles
going through fused quartz window- T. Credo, R.
Schroll
Jitter on leading edge 0.86 psec
  • 2. Ability to simulate electronics and systems
  • to predict design performance

5
Major advances for TOF measurements
Simulation with IHP Gen3 SiGe process- Fukun Tang
(EFI-EDG)
  • 3. Electronics with typical gate jitters ltlt 1
    psec

6
Geometry for a Collider Detector
2 by 2 MCPs
Beam Axis
Coil
  • r is expensive- need a thin segmented detector

7
Generating the signal
  • Use Cherenkov light - fast

A 2 x 2 MCP- actual thickness 3/4 e.g. Burle
(Photonis) 85022-with mods per our work
8
Anode Structure
  • RF Transmission Lines
  • Summing smaller anode pads into 1 by 1 readout
    pixels
  • An equal time sum- make transmission lines equal
    propagation times
  • Work on leading edge- ringing not a problem for
    this fine segmentation

9
Tims Equal-Time Collector
4 Outputs- each to a TDC chip (ASIC) Chip to
have lt 1psec resolution(!) -we are doing this in
the EDG (Harold, Tang).
Equal-time transmission-line traces to output pin
10
Dummy 1
11
Anode Return Path Problem
12
Solving the return-path problem
13
Capacitive Return Path
14
Mounting electronics on back of MCP- matching
Conducting Epoxy- machine deposited by Greg
Sellberg (Fermilab)
  • dum

15
EDGs Unique Capabilities - Harolds Design for
Readout
Each module has 5 chips- 4 TDC chips (one per
quadrant) and a DAQ mother chip. Problems are
stability, calibration, rel. phase, noise. Both
chips are underway
  • dum

16
Tangs work in IHP (200 GHz) design tools
  • dum

17
Requirement Psec-Resolution TDC
Tang Slide
MCP_PMT Output Signal
Start
500pS
Reference Clock
Stop
Tw
1 ps Resolution Time-to-Digital Converter!!!
18
Approaches Possibilities
(2) Time Stretcher
1/4
Tang Slide
Zero-walk Disc.
Stretcher
Driver
11-bit Counter
Receiver
PMT
CK5Ghz
2 Ghz PLL
REF_CLK
psFront-end (Timing Module Option 2)
19
Time Stretcher Simulation Result
Tang Slide
x200 Stretched Time Interval (Output Signal )
Stretched Time 274ns (pedestal74ns)
1ns Time Interval (Input Signal)
0 50ns 100ns 150ns 200ns
250ns 300ns
20
VCO Submission of Oct. 2006
  • Ultimate Goal
  • To build TDC with 1 pSec Resolution for Large
    Scale of Time-of-Flight Detector.
  • Primary Goal
  • To build 2-Ghz VCO, key module of PLL that
    generates the TDC reference signal
  • Cycle-to-Cycle Time-jitter lt 1 ps
  • To evaluate IHP SG25H1/M4M5 Technology for our
    applications
  • To gain experiences on using Cadence tools
    (Virtuoso Analog Environment)
  • Circuit Design (VSE)
  • Simulation (Spectre)
  • Chip Layout (VLE, XLE, VCAR)
  • DRC and LVS Check (Diva, Assura, Calibre)
  • Parasitic Extraction (Diva)
  • Post Layout Simulation (Spectre)
  • GDSII Stream out
  • Validation
  • Tape Out

Tang Slide
21
Diagram of Phase-Locked Loop
Tang Slide
CP
Fref
I1
Uc
PD
VCO
F0
LF
I2
1N
PD Phase Detector CP Charge Pump LF Loop
Filter VCO Voltage Controlled Oscillator
22
IHP (SG25H1) 0.25mm SiGe BiCMOS Technology
  • 0.25mm BiCMOS technology
  • 200Ghz NPN HBT (hetero-junction bipolar
    transistor)
  • MIM Capacitors (layer2-layer3) ( 1f/1u2 )
  • Inductors (layer3-layer4)
  • High dielectric stack for RF passive component
  • 5 metal layers (Al)
  • Digital Library Developing

Tang Slide
23
SG25 Process Specification
Tang Slide
24
2-GHz BiCMOS VCO Schematic
Tang Slide
Negative Resistance and Current-Limited Voltage
Control Oscillator with Accumulating PMOS Varicap
and 50W Line Drivers
25
V-F Plot (3 model cases _at_ 27C-55C)
Frequency
Tang Slide
Temperature 27C-55C Supply VDD2.5V
VControl varied 0.18V
VControl
26
Phase Noise ( 3 model cases _at_ 27C)
_at_100KHz offset
Worst
Tang Slide
Typical
Best
Tang Slide
Temperature 27C Supply VDD2.5V
27
Calculation of Cycle-to-Cycle Jitter
Tang Slide
28
Virtuoso XL Layout View
Tang Slide
29
Virtuoso Chip Assembly Router View
Tang Slide
30
Transit Analysis Comparison of Schematic and
Post Layout Simulations
Outputs_at_50W loads
Schematic
Post Layout
Tang Slide
31
Simulation for Coil Showering and various PMTs
(Shreyas Bhat)
  • Right now, we have a simulation using GEANT4,
    ROOT, connected by a python script
  • GEANT4 pi enters solenoid, e- showers
  • ROOT MCP simulation - get position, time of
    arrival of charge at anode pads
  • Both parts are approximations
  • Could we make this less home-brew and more
    modular?
  • Could we use GATE (Geant4 Application for
    Tomographic Emission) to simplify present and
    future modifications?
  • Working with Prof. Chin-tu Chen and students,
    UCHospitals Radiology- they know GATE very well,
    use it regularly

32
Possible Collider Applications
  • Separating b from b-bar in measuring the top mass
    (lessens combinatorics)
  • Identifying csbar and udbar modes of the W to jj
    decays in the top mass analysis (need this once
    one is below 1 GeV, I believe)
  • Separating out vertices from different collisions
    at the LHC in the z-t plane
  • Identifying photons with vertices at the LHC
    (requires spacial resolution and converter ahead
    of the TOF system
  • Locating the Higgs vertex in H to gamma-gamma at
    the LHC (mass resolution)
  • Kaon ID in same-sign tagging in B physics (X3 in
    CDF Bs mixing analysis)
  • Fixed target geometries- LHCb, Diffractive LHC
    Higgs, (and rare K and charm FT experiments)
  • Super-B factory (Nagoya Group, Vavra at SLAC)

33
Synergies- The ILC, RadiologyANL,Fermilab,SLAC,
BSD,Saclay, Photonis
  • ILC- met with Fermilab last week to discuss
    possible ILC applications- have propsed a
    workshop with them to explore physics of particle
    ID at the ILC
  • Positron-Emission Tomography have a draft of a
    proposal to UC for a program for applying HEP
    techniques to radiology -with Chin-Tu Chen,
    Radiology
  • Have agreed to write MOU with Saclay (Patrick
    LeDu)
  • Have agreed to write MOU with Photonis/Burle to
    develop new MCPs optimized for timing
  • We are working with Jerry Vavra (SLAC) on
    measurement setups (Karen and Gary at ANL have
    the setup).

34
Status
  • Have a simulation of Cherenkov radiation in MCP
    into electronics
  • Have placed an order with Burle- have the 1st of
    4 tubes and have a good working relationship
    (their good will and expertise is a major part of
    the effort) 10 micron tube in the works
    optimized versions discussed
  • Have licence and tools from IHP working on our
    work stations- Tang is adept and fast working
    with them. Excellent support from Cadence.
  • Have modeled DAQ/System chip in Altera (Jakob Van
    Santen Sr)
  • ANL has put together a test stand with working
    DAQ, has bought a very-fast laser, has made
    contact with advanced accel folks(students)
  • Have established strong working relationship with
    Chin-Tu Chens PET group at UC source of good
    students common interests (with Saclay too).
    Hope can establish a program in the application
    of HEP to meds
  • Harold and Tang have a good grasp of the overall
    system problems and scope, and have a top-level
    design plus details
  • Have found Greg Sellberg at Fermilab to offer
    expert precision assembly advice and help
    (wonderful tools and talent!).
  • 9. Are working closely with Jerry Vavra (SLAC)
    will work with Saclay

35
Next Steps
This was the text on my penultimate slide at the
workshop at Arlington TX in April
  • Start testing the MK-0 device we have (ANL)
  • Understand the electrical circuit in the MCP and
    specify the next model (MK-I) we want
  • Finish the design and place the order to IHP for
    the 1st chip.

THE END (not really)
Substantial Progress on all 3 See
hep.uchicago.edu/frisch For more documents and
links
36
The Electronics Development Groupof the EFI
  • Over a million dollars of software tools from a
    number of vendors- built up by Harold. Nowhere
    else I know of
  • Major impact on CDF,Atlas, KTeV, Quiet,
  • Serves not just UC- other institutions send folks
    here- systems are collaborative
  • Student involvement- we train students in
    cutting-edge electronics (grad and underg)
  • Highly innovative designs -

37
DOE-ADR Funds
  • First chip submission was last week-ADR
  • Tang leaves tomorrow for Germany for IHP
    Workshop-ADR
  • Starting on next submission design
  • Will seed collaborative work with ANL, SLAC
    (Vavra), and, hopefully, Fermilab
  • Would like to discuss longer-term support for a
    program of Applications of HEP Techniques to
    Radiology, and also some EDG support.

38
Backup Slides
  • Miscellaneous..

39
Got Burle MK-0 (our name)- many thanks!
  • Paul Mitchell has done nice things- wonderful
    test bed for understanding

40
V-F Plot Comparison of Schematic and Post Layout
Simulations
Frequency
Post Layout
Schematic
Vcontrol
41
Phase Noise Post Layout SimulationsVDD2.5V
Temp.27C, 55C
Phase Noise _at_100KHZ offset
42
A real CDF event- r-phi view
  • Key idea- fit t0 (start) from all tracks

43
Conclusion
  • (1) VCO time-jitter met our requirement.
  • (2) Post layout simulation matched schematic
    simulation very well.
  • (3) Some problems we have encountered with pcell
    library, layout, DRC, LVS and auto-routing
    functionalities.
  • (4) Ready for October Submission.

44
Shreyas Bhat slide
p Generation, Coil Showering GEANT4
  • Input Source code, Macros Files
  • Geometry
  • Materials
  • Particle
  • Type
  • Energy
  • Initial Positions, Momentum
  • Physics processes
  • Verbose level

Have position, time, momentum, kinetic energy
of each particle for each step (including upon
entrance to PMT)
  • Need to redo geometry (local approx.? cylinder)
  • Need to redo field
  • Need to connect two modules (python script in
    placefor older simulation)

PMT/MCP GEANT4 - swappable
Pure GEANT4
Get position, time
45
Shreyas Bhat slide
p Generation GATE
  • Input Macros Files - precompiledsource
  • Geometry
  • Materials
  • Particle
  • Type
  • Energy
  • Initial Positions, Momentum
  • Verbose level

Physics processes macros file
Solenoid Showering GATE
But, we need to write Source code for Magnetic
Field, recompile
PMT/MCP GATE - swap with default
digitization module
GATE
Get position, time
46
The Hard Parts- Reality
  • Havent yet plugged in a device- all simulation
  • Harold and Paul Mitchell (Burle) have taught us
    that the hard part is the return path from
    MCP-OUT to the Gd
  • Havent yet submitted a design to IHP- dont know
    the realities of making chips (in progress as we
    speak)
  • Have no equipment to test these chips when we get
    them
  • Have no experience on how to measure device
    performance when we actually get them.
  • We are a small group- lots to do!
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