henda and patara a solid state neutron detector and a prototype readout chip for the sns
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HENDA and Patara A solid state neutron detector and a prototype readout chip for the SNS. Steven C. Bunch, Jonathan L. Britton, Benjamin J. Blalock The University of Tennessee Charles L. Britton, Jr. The University of Tennessee/Oak Ridge National Laboratory - PowerPoint PPT PresentationTRANSCRIPT
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HENDA and PataraA solid state neutron detector and a prototype readout chip for the SNS
Steven C. Bunch, Jonathan L. Britton, Benjamin J. BlalockThe University of Tennessee
Charles L. Britton, Jr.The University of Tennessee/Oak Ridge National Laboratory
Douglas S. McGregor (P.I.), Russell Taylor, Tim Sobering, David Huddleston, Walter McNeil, Troy Unruh, Blake Rice, Steven Bellinger, Brian Cooper
Kansas State University
Lowell CrowSpallation Neutron Source/Oak Ridge National Laboratory
A research project funded by the National Science Foundation
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Outline
• Spallation Neutron Source (SNS) Overview
• Neutron Detector Overview (HENDA)
• Chip Architecture (Patara)
• Measurements
• Next Steps
• Conclusion
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SNS Overview
The Spallation Neutron Source (SNS)
• Accelerator-based neutron source being built in Oak Ridge, Tennessee, by the U.S. Department of Energy.
• It will provide the most intense pulsed neutron beams in the world for scientific research and industrial development.
• At a total cost of $1.4 billion, construction began in 1999 and will be completed in 2006.
• The construction of SNS was a partnership of six U.S. Department of Energy national laboratories: Argonne, Brookhaven, Jefferson, Lawrence Berkeley, Los Alamos, and Oak Ridge.
• This collaboration was one of the largest of its kind in U.S. scientific history and was used to bring together the best minds and experience from many different fields.
For more information see http://www.sns.gov
The SNS at ORNL is changing from a project into a facility! The first spallation neutrons were produced on April 28, 2006
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SNS InstrumentsVULCAN is a compound diffractometer for engineering applications
PSD
ElasticallyBent Si Xtal
Sample
Bragg focusing can achieve spatial resolution of 0.1 mm, but a 1D high resolution neutron detector is required to use it efficiently.
SNAPSNAP (Spallation Neutrons and Pressure) is a Neutron (Spallation Neutrons and Pressure) is a Neutron Diffraction Instrument Dedicated to High Pressure ResearchDiffraction Instrument Dedicated to High Pressure Research
Diamond anvil cell samples may be very small, so high resolution detectors are needed to resolve the diffraction pattern.
Motivates development of a 2D version
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Neutron Detector Overview
High Efficiency Neutron Detector Array (HENDA)
• Semiconductor linear thermal neutron detection imaging array• Reaction - n + 6Li 4He + 3H + 4.79 MeV• Pixel dimensions are 80 microns wide, and 4 cm long, with a 100 micron pitch• Contains 1000 pixels, each with expected intrinsic thermal neutron detection efficiency of
>20%• Millions of holes filled with neutron reactive material increase the detector efficiency
Linear pixels and bonding pads Etched holes >170
microns deep30 micron diameter holes with 6LiF
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Measured results show that the efficiency is greatly increased with the perforated design
6LiF Film Thickness (microns)
0 5 10 15 20 25 30 35 40
Per
cent
The
rmal
Neu
tron
Det
ectio
n E
ffici
ency
0123456789
10111213
Holes Unfilled Predicted for Planar Device
Holes Filled with 6LiF
With the perforated surface coated with 6LiF material, with holes not yet filled, already shows improvement over basic planar designs
With the holes backfilled with 6LiF, the thermal neutron detection efficiency is greatly increased
Detector Measurements
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Prototype Chip Architecture “Patara”
Specifications– Pulse-Processing Requirements
• Pulse rate – 10 kcps
• Pulse-Pair Resolution – 1s
– General Signal-Processing Requirements• For 10B detector coatings
– 300 keV – 1.47 MeV or 12.8 fC – 65.6 fC
• For 6Li detector coatings– 300 keV – 2.7 MeV or 12.8 fC – 120 fC
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Chip Design Specifications
• Preamplifier– Noise dominated by input FET < 1000 rms electrons
• System uncertainties of a few keV necessary for lower-level gamma discrimination threshold of ~300 keV
– Accept positive or negative input– Detector leakage current compensation– Able to handle detector capacitance up to 10 pF– Pole/Zero compensation network– Full gain or half gain adjustment
• Shaper– Adjustable polarity– Four complex conjugate poles– Low noise < 10% of preamplifier (low-gain system)– FWHM ~ 270 ns– Settling time ~ 600 ns
• Baseline Restorer– “Ground sensing” inputs
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Preamplifier
• Regulated cascode topology
• M1 designed to optimize noise for detector capacitance of 5 pF using Cgs = method
3detC
• M2 & M3 sized to contribute < 10% of M1 noise
• Cc of 0.3 pF used to control stability of negative feedback loop between M2 & M3
• Feedback network needed to allow Cf to discharge after a charge pulse
VDD
Qin
Vout
M1
M2
M3
Cc
Ibias
CfFeedbackNetwork
M4
M5M6 M7 M8 M9
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Final Preamplifier Pole/Zero Compensation
Ibias
2 x Ibias
Vref
A
Vdd
Vdd
V-
Cf
15 x Ibias
30 x Ibias
Vref Vdd
Vdd
15 x CfA
Cf2
Rf2
To Shaping Circuit
15x
15x
• Based on MOSFET feedback network and pole/zero compensation – Ludewigt, et al., TNS, vol. 41, no. 4, 1994.
• Adapted from Low Frequency Feedback Loop topology
• Increase Ibias to compensate for detector leakage up to 15 nA
• Adjustable Vref sets dynamic range for either polarity input
• Approximately 1.6 mW/channel
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Preamplifier Feedback Network Biasing
Ibias
Vdd
2 x Ibias
To Feedback Network
DS0 DS1 DS2 DS3 DS0 DS1 DS2 DS3
W 2 x W 4 x W 8 x W 16 x W2 x W 4 x W 8 x W
Henri J. Oguey and Daniel Aebischer, “CMOS Current Reference Without Resistance,” IEEE Journal of Solid-State Circuits, Vol. 32, No. 7, pp. 1132-1135, 1997.
• Nanoampere current reference
• Switchable bias current for detector leakage current compensation
• Allows pole/zero compensation network to track feedback bias
To Pole/Zero Compensation Network Bias
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Shaper Design Process
• Shape pulse using 5-pole complex-conjugate semi-Gaussian filter
• Pole-zero constellation optimized using MATLAB to approximate Gaussian shape
• MATLAB script iterations using ‘radial variation’ and sensitivity analyses
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Shaper Fundamentals
• Semi-Gaussian pulse response with 1 real, 4 complex poles• 1 μ-sec pulse-pair resolution with gated baseline restoration (SNS synchronous)• Current-mode quasi-linear operation
Real Pole 2
Real Pole 3
Real Pole 4
Real Pole 5H(s) = G
323
2
2
11)(
ss
KsH
545
2
3
11)(
ss
KsH
V to I Converter Localized Feedback Localized Feedback
VoutReal Pole 1(Op-Amp)
Ideally, G
1 Real Pole
1
1
1)(
s
KsH
Vbaseline
Vin
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Complex Conjugate Topology
• Modified R-lens magnification
• Intrinsically low-noise
• R magnification allows small physical R to give low-frequency pole
• At higher signal levels, circuit is dynamic, but magnified small physical R dominates 1/gm for improved linearity over Gm-C filters
Vdd
Iout(to next CC stage)
Ibias
Iin
Vout(last stageonly)
R RC2C1
G. Bertuccio, et al., “‘R-lens filter’: An (RC)n current-mode lowpass filter,” Electronics Letters, vol. 35, no. 15, 22nd July 1999.
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Noise MeasurementsSingle Channel Noise vs Detector Capacitance
300
400
500
600
700
800
900
1000
1100
1200
1300
0 5 10 15 20 25
Cdet (pF)
Noi
se (r
ms
elec
tron
s)
Measured
Simulated
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Noise MeasurementsSingle Channel Noise vs Input FET Bias
300
500
700
900
1100
1300
1500
60 80 100 120 140 160 180 200 220
Bias Current (uA)
Noi
se (r
ms
elec
tron
s)
0pF Detector Capacitance
Simulated
Measured
Measured
Simulated
15pF Detector Capacitance
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Gain MeasurementsSystem Gain vs Channel
4
5
6
7
8
9
10
1 4 7 10 13 16
Channel
Gai
n (m
V/fC
)
Full Gain Setting
Half Gain Setting Positive Polarity Input
Positive Polarity Input
Negative Polarity Input
Negative Polarity Input
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• Pulse shape matches simulations very closely
• FWHM ≈ 290 nsec
• Full analysis of ‘dynamic noise’ upcoming
• End-to-end nonlinearity < 5% in range of interest
• Approximately 2.1 mW/channel
Linearity - End-to-end (all)
0
100
200
300
400
500
600
700
0 100 200 300 400 500 600 700
Vin (mV)
Vout
(mV)
Shaper Measurements
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Next Steps
• Discriminator, zero suppression, “SNS standard interface”
• 64-128 channels
• Interface with KSU HENDA
• Integrate with SNS system for tests
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Conclusions
• Prototype chip fully functional on first-cut silicon with 3.7mW/channel power dissipation
• Second fabrication pass in July 2006 for BLR offset improvements
• Test at SNS in late summer 2006 with 252Cf sources
• Submission of large final chip late in 2006