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Fully Depleted Low Power CMOS Detectors
Konstantin Stefanov
8 June 2015
Back side biased CMOS image sensor development
• We have a project to design back-side biased, thick sensitive area CMOS image
sensors achieving full depletion
– Funded by the UK Space Agency
– 1 year project
• Demand for thick (>100 µm), fully depleted CMOS sensors with high QE:
– Near-IR for astronomy, Earth observation, hyperspectral imaging, high
speed imaging, spectroscopy, microscopy and surveillance.
– Soft X-ray (up to 10 keV) imaging at synchrotron light sources and free
electron lasers requires substrate thickness >200 µm
• Low noise and high CVF are essential to most applications – pinned photodiode
is required
2
Konstantin Stefanov, 8 June 2015
Back side biased CMOS image sensor development
• Present experience with CMOS:
– ESPROS: bulk 10 kΩ.cm, 50 µm thick filly depleted
• We have designed a chip already
• CCD sense element with rather high dark current
• ESPROS has no plans to increase the thickness in the near future
– TowerJazz: 1 kΩ.cm epi, thickness up to 18 µm
• Good pinned photodiode available
• Epi thickness can be increased in principle to 100 µm – new (untested) advances
in epi manufacture
• Our goal is to design back-side biased CMOS demonstrator
– Initially on easily available substrates (e.g. 18 µm), with or without thinning
– Demonstrate successful operation
– Eventually move on to thicker substrates
3
Konstantin Stefanov, 8 June 2015
Back-side bias from the front
–20V
A
Deep P-well
Substrate ring
+3.3V
+VPPD
+VPPD
Deep N-well
Guard ring
DEPLETED
D
NOT
DEPLETED
Very shallow backside p+ implant
•
•
•
Reverse back side bias applied from the front to achieve full depletion
Additional guard rings may be required
A and D should be selected to maintain conductive path from the substrate
ring to the back side
4
Konstantin Stefanov, 8 June 2015
The substrate current problem
Diode
p-type
epi/bulk Si
Backside p+ implant
Diode
Diode
•
•
•
P-wells
An obvious problem is revealed
Front-to-back conductive path
– p+ p p+ resistor is formed
This current can be large and has to be
suppressed
–20V
5
Konstantin Stefanov, 8 June 2015
How to prevent the parasitic substrate current?
P-wells
•
Diode
Diode
Diode
•
Pinch-off
•
•
–20V
6
Expanding depletion regions around the
photodiodes join up
– Pinch-off is created under the p-wells
– Substrate current is eliminated
The pinch-off condition depends on:
– Doping and junction depth
– Photodiode and p-well sizes
– Bias voltages
– Stored signal charge
P-wells should be narrow and shallow
Photodiodes should be deep
Konstantin Stefanov, 8 June 2015
Substrate current simulations
Potential
Current could easily be
hundreds of milliamps!
Hole current
7
Konstantin Stefanov, 8 June 2015
Substrate current reduction
•
•
Diode
p-well
Diode
p-well
Additional implants
Diode
•
•
8
If the p-wells are deep, pinch-off may not
occur
Additional n-type implant:
– Under the p-wells
– Floating
– Not connected to the diode
– n-, doping around 1015 cm-3
– Called Deep Depletion Extension (DDE)
for now
Patent pending
There is only one more similar concept at
the moment (much more complex,
protected by a US patent)
Konstantin Stefanov, 8 June 2015
Potentials
Guard ring
p-well
Diode
p-well
DDE Implant
Diode
p-well
Diode
No implant
The DDE implant extends the diode
depletion sideways under the p-wells
9
Konstantin Stefanov, 8 June 2015
Potential profiles
•
•
•
•
•
1
0
Potential (V)
-1
-2
-3
Potential barrier along the cutline
– Barrier height ~1 V.
Incoming charge is re-directed
either left or right
“PPD model” 1 µm deep
P-well doping  1 µm deep
DDE implant doping:
– Too low – doesn’t achieve
pinch-off
– Too high – doesn’t deplete or
creates a potential pocket
-4
-5
-6
0
1
2
3
4
5
6
Depth (μm)
7
8
9
10
10
11
Konstantin Stefanov, 8 June 2015
Substrate current with DDE
Implant here:
no substrate
current
11
No implant
Konstantin Stefanov, 8 June 2015
Preventing substrate current from logic
Logic transistors
–20V
+3.3V
Deep P-well
+3.3V
+3.3V
Guard ring
Buried N-well
Substrate ring
Very shallow backside p+ implant
•
•
•
Buried N-well prevents substrate current
It also collects charge
Should be placed at the periphery of the chip
12
Konstantin Stefanov, 8 June 2015
New idea – buried pinned photodiode
•
•
•
•
The PPD is under the p-wells and pinned by them
Idea inspired by power trench MOSFET design
– “Vertical MOSFET”
– Current flows vertically: source is top, drain is
bottom
Similar approach can be used for the transfer of charge
between a buried PPD and the sense node
Buried PPD eliminates the front p-well conduction and is
great for back-side biasing
Image credit: Fairchild Corp.
13
Konstantin Stefanov, 8 June 2015
Trench transfer gate PPD Pixel
Ring FD
N-well
P
P
TG
TG
N
Deep P-well
N
P-well
Deep P-well
Graded pinned photodiode (N)
P-type high resistivity substrate
•
•
•
•
•
Pinned photodiode formed under the deep P-wells
Fast charge transfer due to the graded doping of the PPD
Fast charge collection – full depletion (thick sensor) with back side bias is natural
Both NMOS and PMOS in pixel over most of the pixel area
Combining the best of all!
14
Konstantin Stefanov, 8 June 2015
Conclusions
•
•
Fully depleted PPD pixel under development at the CEI
– Charge transfer from a large diode to a small sense node
– High sensitivity (large signal) required to reduce power consumption
• Low detector power will become even more important in the future (e.g. SPT)
– Full depletion is mandatory for good radiation hardness
– Only limited number of NMOS transistors in pixel
In the future – trench transfer gate PPD combining:
• Small sense node with low capacitance – large voltage signals for low power
• Full depletion
• Large number of NMOS and PMOS transistors in pixel
• Rival to hybrid APS?
15
Konstantin Stefanov, 8 June 2015