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A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
The PANDA Microvertex
Detector: Present Design and Opportunities for 3D Integration Technologies
Angelo Rivetti –
INFN-Sezione di TorinoOn behalf of the PANDA MVD group
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Strong Interaction Studies with AntiprotonsStrong Interaction Studies with Antiprotons
Darmstadt, GermanyDarmstadt, Germany
FAIRFAIR
Facility for Antiproton and Ion Research
antiProton
ANnihilation
at DArmstadt
PANDA @ FAIR
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
p
Hydrogen Pellet Target
Luminosity Luminosity Momentum Resolution (Momentum Resolution (δδp/pp/p))
High luminosity High luminosity modemode 2x1032 cm-2s-1 ~10-4 (stochastic cooling)
High resolution High resolution modemode 1031 cm-2s-1 ~10-5 (electron cooling < 8 GeV/c)
HESRHESR
= = HHigh igh EEnergy nergy SStorage torage RRingingMomentum: Momentum: 1.5 1.5 GeV/cGeV/c
--
15 15 GeV/cGeV/c
p
Center of
mass energy:
√s = 5.5 GeV
Antiproton beam
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Enhanced forward emission for light targets and distribution over full polar angle for particles momenta below 1 GeV/c.
Combination of colliding beam and fixed target geometry.
Simulated particle distribution
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
12m
4m
Target SpectrometerSurrounds the interaction region.Solenoidal
2T magnet.
Forward
SpectrometerWith a second magnet provides angular coverage for the most
forward
angles. 1T dipole
p
The PANDA detector complex
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Four barrels:-
Two Inner
layers: pixels.-
Two outer
layers: strips.Six forward disks:-
4 pixels + 2 mixed disks.
Read-Out channels and area coverage:
Pixels : 12M channels, 0.14 m2.Strips : 200k channels, 0.5 m2.Strips are double sided
The MVD is the closest detector to the interaction point The MVD is the closest detector to the interaction point
Primary function: vertexingPrimary function: vertexing
Additional task: dE/dx
for dE
up to 2.3 MeVAdditional task: dE/dx
for dE
up to 2.3 MeV
The MicroVertex
Detector (MVD)
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Pixel detector specifications
Baseline technology : hybrid pixel detectors.A dedicated front-end chip under development in 0.13 μm.Custom front-end development motivated by high track density (12.3
MHz/cm2) and trigger-less operation.
Pixel cell specificationsPixel cell specifications
Pixel Pixel SizeSize 100100μμm x 100m x 100μμmm
NoiseNoise LevelLevel 200 e200 e‐‐ rmsrms
Linear Linear dynamicdynamic rangerange Up Up toto 100fC100fC
PowerPower consumptionconsumption < 20< 20μμWW
Input Input polaritypolarity SelectableSelectable
LeakageLeakage insensitiveinsensitive Up Up toto 50 nA50 nA
Pixel cell specificationsPixel cell specifications
Pixel Pixel SizeSize 100100μμm x 100m x 100μμmm
NoiseNoise LevelLevel 200 e200 e‐‐ rmsrms
Linear Linear dynamicdynamic rangerange Up Up toto 100fC100fC
PowerPower consumptionconsumption < 20< 20μμWW
Input Input polaritypolarity SelectableSelectable
LeakageLeakage insensitiveinsensitive Up Up toto 50 nA50 nA
ASIC specificationsASIC specifications
TriggerTrigger SelfSelf triggeringtriggering
Active areaActive area O(1cmO(1cm22))
Data rateData rate O(0.8 O(0.8 GbitGbit/sec.)/sec.)
Radiation toleranceRadiation tolerance ˜̃ 10101414 nneqeq /cm/cm22
Simultaneous time stamping andSimultaneous time stamping andcharge measurementcharge measurement
Good time resolution Good time resolution rmsrms 1.8 ns (at 160 MHz 1.8 ns (at 160 MHz clock) clock) withwith 22∙∙101077 annann/s/s
ASIC specificationsASIC specifications
TriggerTrigger SelfSelf triggeringtriggering
Active areaActive area O(1cmO(1cm22))
Data rateData rate O(0.8 O(0.8 GbitGbit/sec.)/sec.)
Radiation toleranceRadiation tolerance ˜̃ 10101414 nneqeq /cm/cm22
Simultaneous time stamping andSimultaneous time stamping andcharge measurementcharge measurement
Good time resolution Good time resolution rmsrms 1.8 ns (at 160 MHz 1.8 ns (at 160 MHz clock) clock) withwith 22∙∙101077 annann/s/s
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
100
100 μμ mm
100
100 μμmm
Pixel module
concept
Geometrical constraints dictates the use of four differentmodule size.
Red circles=parts that might benefit from a 3D approach
Module controller or more cables…
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Pixel module
types
Minimal set of modules to have adequate coverageSame width, four different lengths
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Pixel sensors
Baseline choice: epitaxial silicon substratep-in-n sensor implementationepitaxial thickness: 50-100 μm.Inert substrate: 50 μm.Alternative: oxygen enriched silicon
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
In each
pixelThe
control
logic
receives
the
signal
from
the
comparator
and
stores
the
value
on
the
time
stamp
bus
(Gray
encoded)
at
the
rising
and
falling edge in two 12 bit registers.It is present also a 12 bit configuration register.SEU tolerant logic (based on the DICE cell)
Each
column
The
readout
logic
made
in
a
fixed
priority scheme
to
read
the timestamps
of
the
pixel
cells
and
to
read/write
the
configuration
bits.
Master clock @160 MHzMaster clock @160 MHz
Pixel read-out
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
The analog Front-End generates a pulse whose width is proportional to the charge injected by the sensor.
ToTo
the the digitaldigital
partpart
ToT
Front-end
cell
Single Pixel Power dissipation of 15 μW from a 1.2 V power supply.
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Chip prototyping: ToPiX
2.0
31 032 6395 6496 127
31 032 6395 6496 127
31 031 0
128 pixel column length: 12.8 mm.
384 pixel cell
in four columns:
• Two folded columns with 128 pixels.• Two short column with 32 pixels.
• Simplified end‐of‐column logic.
• Sixteen pixels with wire bonding pad.
ToPix 2.0 is a reduced scale prototype front-end chip for the hybrid pixel sensors.It has been designed in a CMOS 0.13 μm technology and tested.
The final version of ToPiX will consist of a matrix of 116x110 cells with a pixel size 100 μmx100 μm, thus covering a 1.28 cm2 active area.
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Pulse shape reconstruction using ToTinformation for different loads at the input.
Some experimental results
0.8
0.7
0.6
0.5
0.4
0.3
Thre
shol
d vo
ltage
(V)
543210Time (µs)
Unbonded Wire-bonded to pixel Wire-bonded to board, 1pF cap
400
300
200
100
0
0.200.150.100.050.00TOT (clk) * tail slope (V/clk)
Topix2Am241 (γ 60keV)
ch 019 ch 020 ch 023
Americium 60 keV signal in 300 thick μm standard silicon (pixel size 300 μm x 300 μm)
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Signal to noise ratio is limited by parasitics capacitance due the external connections. Bonding pad+wirebonding+protection diodes.
Epitaxial
sensor 50 μm thick, size: 125μm x 325 μmSource: Am241, γ
at 60keVEpitaxial
sensor 50 μm thick, size: 125μm x 325 μmSource: Am241, γ
at 60keV
Tests with an epi-sensor
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Silicon microstrip
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Silicon microstrip modules
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
Silicon microstrip modules
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
AnalogAnalog DigitalDigital
100
100 μμ mm
70+30 70+30 μμmm
Do we need extra-dimensions?
Each cell incorporates:Front-end amplifierLeakage compensation5 bit DACs for threshold tuningComparator12 bits configuration registerOne register for leading edgeOne register for trailing edge
In the present implementation, most of the space reserved to the analog part, but…
3D approach mostly interesting for the pixel part of the MVD
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
DICE cell in 0.13μm technology improves SEU resistance,
but not as much as for previous technologies.Improved radiation hardness=more space for the digital
part and less for the analog one, with adverse affect on
matching
Test performed
at Laboratori Nazionali Legnaro, using
Silicon
Radiation
(SIRAD) facility
Ions
used
in the beam
test: 16O, 19F, 28Si, 35Cl, 58Ni, 79Br
Weibull
distribution
Dice cell
SEU performance
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
A two tiers approach?
In the present design only 2/3 (1/2 in the next prototype) of the pixel area is available for the routing of the analog power rails.
No room for local tuning of the feed-back current (no space for DACs and registers) ⇒ relatively large ToT spread (12% rms).
Further reduction in density in the next prototype due to the (necessary) migration to a different flavor of the process.
Need to make some compromise on analog performance and on the possibility of adding very desirable features (e.g. protection against “monster hits”).
In 1D
Obvious partitioning: One tier for the analog and one for the digital part. Analog tier: preamplifier, comparator, DACS.Digital tier: all the rest…Room for more sophisticated digital processing: no controller chip and less cables!Room for significant amount of on chip decoupling capacitors…
In 2D
A. Rivetti VIPS workshop-Pavia, April 23rd, 2010
In summary…
The MVD is a compact but complex detector designed by a relatively small collaboration (compared to LHC detectors).
Rely on well established technologies and minimize custom developments.
In the R&D phase monitoring other developments that may bring significant advantages in term of cost/performance.
3D integration particularly appealing for the hybrid pixel part.Points that will be of interests
Cheap alternatives to bump bondingThinner electronics/sensorsBetter front-end electronics (increased functionality due
to multi-layers chips)