Title: Custom IC Development for SNAP
1Custom IC Development for SNAP
- Jean-Pierre Walder
- Lawrence Berkeley National Laboratory
- July 2002
2Outline
- Introduction
- Custom ICs RD goals
- Front end readout block diagram
- SNAP IC plan
- Front end readout requirements
- Signal processing
- Front end dynamic range and resolution
- Multi slope ADC concept
- ADC architecture study
- Technology survey
- Behavior of sub micron CMOS at cold temperature
- Radiation tolerance
- Conclusion
3Introduction
- SNAP instrument consists of CCDs and HgCdTe
sensors for wide-field imaging and spectroscopy
? We have identified areas where custom
integrated circuits are a viable solution to meet
SNAPs requirements - Custom ICs allow power, noise optimization
compared to a discrete solution. - ? We envision a readout scheme that focuses on
CCD devices, keeping in mind the characteristics
of the HgCdTe in case Rockwell is not sucessful. - RD are required to mitigate technical schedule
risk - Sensor front-end (correlated double sampler)
- Analog-to-digital converter
- CCD controller (maybe commercial parts or custom)
4Custom ICs RD Goals
- The RD goals are to provide thorough and
complete answers in the following areas - Readout noisenoise optimization and signal
processing study - Power optimizationIn general, low power is
required for space, and very low power is
mandatory if we want to locate the front end
electronics close to the CCDs. Its power
consumption should be a small fraction of the CCD
power. - Operation at cold temperatureEvaluate current
technology performances at cold temperature
(140K) and verify/modify the model for a reliable
design. - Radiation hardness Evaluate current technology
performances in radiation environment especially
at low temperature - PrototypeDesign and test a reliable prototype
before construction -
5Front end readout block diagram
Mixed mode front end custom IC Multi channel chip
Clocks, control
Front end IC
CCD
Analog input
Analog signal processing
ADC
Digital out
Amplification
(One channel)
6SNAP IC plan
- Implementation of a signal processing test chip
containing - 4 channels
- Input amplifier
- Correlated double sampling
- Integrator
- Multi gain amplifier (multi slope)
- Individual test structures
- Test transistors
- This is to verify
- Noise performance
- Power consumption
- Multi slope concept
- Operation at 140K and 300K
- Radiation tolerance
- A second iteration implementing an integrated ADC
with a low noise front end is planned.
- This is to verify
- Noise performance
- Power consumption
- Resolution/linearity
- Sampling rate
- Electronic system noise
7Front end readout requirements
- Low noisePhotometry CCD electronic noise ?
4e rms HgCdTe electronic
noise ? 5e rmsSpectrograph CCD electronic
noise ? 2e rms HgCdTe
electronic noise ? 5e rms - Large dynamic range96dB from noise floor to
130ke well depth - Readout frequency ? 100 kHz
- Radiation tolerant 10 kRad ionization (well
shielded) - Low power ? 200mJ/image/channel
- Operation at 140K and 300KAllow normal operation
at 140K and chip testing at room temperature - Compact
- Robust, space qualified
8Signal processing (1/4)
CCD output stage
Floating diffusion capacitor
Serial register
Reset FET
Output stage
Source follower
Timing
RG (reset)
(Summing Well)
SW
Output signal
Reset signal
Video signal
9Signal processing (2/4)
CCD noise sources
Thermal and 1/f noise of the output transistor
Thermal noise of the output resistor
Thermal and 1/f noise
KTC noise
Frozen noise charge, with a variance of KTC,
stored in Cfd just after reset.
Thermal noise
Signal processing is needed to reduce the CCD
noise
- Correlated double sampling ( Vsignal Vreset)
remove the KTC and 1/f noise. - Integration remove the thermal noise.
10Signal processing (3/4)
C (100pF)
CCD noise only
R
t
Out
X1
CCDnoisesource
(Noiseless)
Integrator
t
-X1
CCD conversion gain 3.5mV/e
Correlated Double Sampler
Integration time t
Input referred noise (e)
Out
4ms (R20KW)
2.6
t
t
8ms (R40KW)
1.86
time
1.8
10ms (R50KW)
Reset integration
Signal integration
Real integration during 2t. Good rejection of the
CCD thermal noise.
11Signal processing (4/4)
CCD noise first stage noise
C (100pF)
R
t
Out
X1
CCDnoisesource
(Noiseless)
t
-X1
CCD conversion gain 3.5mV/e
Input referred noise (e)technology A / B
Integration time t
Out
4ms (R20KW)
2.8 / 2.9
t
t
8ms (R40KW)
2.1 / 2.2
10ms (R50KW)
1.92 / 2
time
Reset integration
Signal integration
The 1/f noise of the input stage is reduced by
the CDS The thermal noise from the input stage is
negligible compared to the CCD thermal noise
12Front end dynamic range and resolution
- The dynamic range for the signal is 96dB (16
bits) - From 2 electrons (CCD noise) up to 130000
electrons - The Signal/Noise ratio of the sensor/readout
chain is less due to the Poisson process of the
light interacting in the sensor. - dN/N 1/ (N)½ where N is the number of
photons. - The readout chain should digitize the signal with
an LSB size which depends of the signal amplitude
such that the quantization noise is still below
the Poisson noise.
CCD electronic noise
Poisson
Quantization noise area
13Multi slope ADC concept
Gain 1
Digital out
Input
Signal processing
MUX
12 bits ADC
Gain 2
Gain 32
½ of (Poisson ? elec noise)
Poisson elec noise
Gain 32 quantization noise referred to the
input
Gain 1
Gain 2
The dynamic range is covered using 3 slopes and a
12 bit ADC
14ADC architecture study
- Several architecture were investigated.
- In the range of the required resolution (12 bits)
and sampling rate (lt100kHz), we have identified
two types - Pipeline ADC
- Single ramp ADC
Single ramp ADC
Pipeline ADC (1 bit cell)
X m
S/H
X2
Input
Digital out
Input
-
X nb of bits
cmp
Digital
DAC
ADC
Ramp
Counter
Digital out (1 bit)
Sampling rate ltlt Clock frequency Number of stage
1 Multi channel one ramp generator could
supply m comparators.
Sampling rate Clock frequency Number of stages
number of bits
15Technology survey
- 10 commercial CMOS sub micron processes where
investigated. - Selection criteria
- Noise
- Matching, precision
- Transistor performances
- Passive components availability and precision
- Expected production life time
- Radiation tolerance
Technologies studied for noise and power
performance
Minimum feature size
16Behavior of sub micron CMOS at cold temperature
One option is to locate the front end readout IC
close to the CCD. But, the operating temperature
then will be 140K. Does deep submicron technology
work at 140K?
Several studies of sub micron CMOS operating at
temperatures ranging from 77K to 300K have been
done and are reported in the literature (IEEE
transactions on electron devices).
- Increase of mobility, m(100K)/m(300K) 4 to
6 m T-a, a 1.5
- Increase of gm
- gm(100K)/gm(300K) (am.aI)½ (usually 2 to 3)
- With, am m(100K)/m(300K) aI
Id(100K)/Id(300K)
- Increase of threshold voltage Vth dVth/dT
-1mV/K
17 Measurement at the lab of a TSMC 0.25mm CMOS
testchip
Measurement set up
18Measurement of TSMC CMOS at cold temperature
- DC characteristic measurement of TSMC MOS
transistors - Both N Mos and P Mos.
- Nmos W17.5mm L0.39mm Enclosed gate.
- Pmos W40mm L0.39mm Enclosed gate.
- Performed on transistors using a LBNL TSMC test
chip. - Measurement of Id-Vd and Id-Vg for T 300K,
250K, 200K 150K, 100K and 77K. (Temp sensor
attached to the package) - Extraction of Vth and mobility ratio versus
Temp. - Comparison with simulation using the HSpice TSMC
models.
19Threshold voltage PMOS
Slope -1mV/K
20Mobility ratio NMOS
Minimum size transistor
Spice parameter UTE -1.3
21Mobility ratio PMOS
Spice parameter UTE -0.7
22Radiation tolerance
Irradiation of deep sub micron test transistors
were performed at the lab.
- No significant change of threshold voltage was
observed (lt50mV) - Enclosed geometry prevents leakage at high dose
(10 Mrad) - Standard geometry could be used for dose lt100kRad
Standard geometry
Standard geometry
Enclosed geometry
Enclosed geometry
Dashed line Id versus Vgs before irradiation
Solid line Id versus Vgs after irradiation
(10MRad)
23Conclusion
- The RD has to provide thorough and complete
answers on identified areas. (power, noise, cold
temperature, radiation) - The technology and signal processing needed to
achieve the SNAP requirements have been selected. - The multi slope concept has been chosen to limit
the ADC resolution. - A test chip design, implementing the signal
processing building blocks has started. - The ADC architecture study is planned.
- Deep sub micron CMOS works at low temperature
and the behavior is predictable by Spice
simulation. - Good radiation tolerance of deep sub micron
processes have been observed.