Transcript
Page 1: Development of the DEPFET Sensor with Signal … · 1 AIS Seminar SLAC, 26.10.12 Development of the DEPFET Sensor with Signal Compression: a Large Format X-ray Imager with Mega-Frame

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AIS Seminar SLAC, 26.10.12

Development of the DEPFET Sensor with Signal Compression: a Large Format X-ray Imager with Mega-Frame Readout Capability for the

European XFEL

SLAC, 26.10.2012

Matteo Porro on behalf of the DSSC Consortium

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M. Porro1,2, L. Andricek2,3, S. Aschauer8, L. Bombelli4,5, A. Castoldi4,5, G. De Vita1,2, I. Diehl7, F. Erdinger6, S. Facchinetti4,5, C. Fiorini4,5, P. Fischer6, T. Gerlach6, H. Graafsma7, C. Guazzoni4,5, K. Hansen7, H. Hirsemann7, P. Kalavakuru7, A. Kugel6, P. Lechner8, G. Lutz8, M. Manghisoni10, D. Mezza4,5, D. Moch1,2, U. Pietsch9, E. Quartieri10, V. Re10, C. Reckleben7, C. Sandow8, S. Schlee1,2, J. Soldat6, L. Strueder1,2, A. Wassatsch2,3, G. Weidenspointner1,2, C. Wunderer7

1) Max Planck Institut fuer Extraterrestrische Physik, Garching, Germany 2) MPI Halbleiterlabor, Muenchen, Germany 3) Max Planck Institut fuer Physik, Muenchen, Germany 4) Dipartimento di Elettronica e Informazione, Politecnico di Milano, Milano, Italy 5) Sezione di Milano, Italian National Institute of Nuclear Physics (INFN), Milano, Italy 6) Zentrales Institut für Technische Informatik, Universitaet Heidelberg, Heidelberg, Germany 7) Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany 8) PNSensor GmbH, Muenchen, Germany 9) Fachbereich Physik, Universitaet Siegen, Siegen, Germany

10) Dipartimento di ingegneria industriale, Università di Bergamo, Bergamo, Italy  

DSSC Consortium

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  Introduction

  DSSC Concept overview

•  Requirements and Design Parameters •  Focal Plane overview •  Non-linear DEPFET working principle •  Non-linear system properties •  Readout ASIC

  Main Achievements

  System simulation

  Conclusions

Outline

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Up to ~2700 bunches in 600 µs, repeated 10 times per second producing 100 fs X-ray pulses (~27 000 pulses/second).

max bunch rate: 4.5 MHz

We want to readout 1024 x 1024 pixel

frames every 220 ns

Bunch structure of the European XFEL

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2D detectors for EuXFEL

Three Detector Developments at the European XFEL (coordinator: M. Kuster)

  Adaptive Gain Pixel integrating Pixel Detector Consortium (AGIPD) (Project Leader: H. Graafsma) o  DESY o  PSI / SLS Villingen o  Universität Hamburg o  Universität Bonn

  Large Pixel Detector Consortium (LPD) (Project Leader: M. French)

o  Rutherford Appleton Laboratory / STFC o  University of Glasgow

  DEPFET Sensor with Signal Compression Consortium (DSSC) (Project Leader: M. Porro)

o  Max Planck Halbleiterlabor Munich o  DESY o  Universität Heidelberg o  Politecnico di Milano / INFN o  Università di Bergamo o  Universität Siegen  

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DSSC – Design Parameters

Parameter  

Energy  range   op+mized  for  0.5  …  6  keV  

Number  of  pixels   1024  x  1024 Sensor  Pixel  Shape Hexagonal Sensor  Pixel  pitch ~  204  x  236  µm2

Dynamic  range  /  pixel  /  pulse

~5000  ph  @  0.5  keV  >  10000  ph  @  E≥1  keV

Resolu+on Single  photon  detec+on  also  @  0.5  keV

Frame  rate   0.9-­‐4.5  MHz Stored  frames  per  Macro  bunch ≥  640

Opera+ng  temperature

-­‐20˚C  op+mum,  RT  possible

1 Mpixel camera with:

•  Single photon sensitivity event at 0.5 keV

•  high-dynamic range (>10000 ph/pixel)

•  Frame rate up to 4.5 MHz (1 image every 220 ns)

All the properties have to be achieved simultaneously

DSSC will be the first instrument to fulfill this requirement

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DSSC Overview - Concept

●  DEPFET Active Pixel Sensor

●  Readout Concept   Fast analog shaping   Immediate 8 Bit digitization (9 bit for f ≤ 2.2 MHz)   In-Pixel SRAM   Readout during macro bunch gaps

●  Power cycling

Focal  Plane  

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•  1024x 1024 pixels

•  16 ladders/hybrid boards

•  32 monolithic sensors 128x256 6.3x3 cm2

•  DEPFET Sensor bump bonded to 8 Readout ASICs (64x64 pixels)

•  2 DEPFET sensors wire bonded to a hybrid board connected to regulator modules

•  Dead area: ~15%

x-y Gap

128 x 256 Pixel Sensor

21 c

m (1

024

pixe

ls)

DSSC  Overview-­‐  Focal  Plane  Overview  

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DSSC overview – ladder module

~3 mm

  1-2 mW/pixel peak power (SENSOR+FRONT-END) 1-2 kW peak power

  Power cycling about 1/100

  <400 W mean power inside vacuum

I/O  Board  

Regulator  Bo

ard  

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DSSC DEPFET

4.5  MHz  frame  rate  

Every DEPFET pixel provides detection and amplification with:

  Intrinsic low noise due to the small anode capacitance single photon

sensitivity even at 0.5 keV

  Signal compression at the sensor level thanks to the special internal

gate topology high dynamic range

  Charge collection time ~ 60 ns

  Cu layer for bump-bonding allowing

full parallel readout

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DSSC DEPFET Principle

Standard  DEPFET  principle  

o  p-­‐FET  on  depleted  n-­‐bulk  

  All    signal  charge  collected  in  poten+al  minimum  below  FET  channel    "internal  gate"  

all signal charges cause an equal effect on the FET current

linear ΔI/Qsig characteristics

o  reset  via  ClearFET  

o  low  capacitance  &  noise  

DSSC adaptation

signal charges at high levels also stored under source

less/no effect on FET current

non-linear ΔI/Qsig characteristics

gain curve engineering by dose & geometry of implantations

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DSSC DEPFET – Simulation and Layout

236 µ

m

272 µm Pitchx: 204 µm Pitchy: 236 µm

DEPFET  

Dri_  rings  

•  hexagonal shape

- side length 136 µm (A=48144 µm2)

- compatible with C4 bumping @ IBM

•  technology

- 2 polySi layers

- 2 + 1 metal layers

- 12 implantations

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  In the linear region the noise is dominated by electronics noise of the sensor and the readout electronics

  Single photon detection properties are given by the electronics noise of the system with empty internal gate

  For a high input signals more photons fall within one ADC bin. The quantization noise is dominant.

  The quantization noise is always below the poisson noise of the photon generation process

Analog to digital conversion – single photon detection and quantization noise

Electronics noise ADC  bin  size  

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Dynamic range

1  ph  @1keV  Dynamic  range  for  3keV  

ph  –  8  bits  (~8300  ph.)    

256  x  bin  size  @3  keV  

The achievable dynamic range depends on: • The shape of the DEPFET non-linear characteristic • The number of bits of the ADC • The number of bins of the ADC associated to the signal produced by the first collected photon • The photon energy.

• The dynamic range increases with the photon energy. This is because as the photon energy increases, the number of photon falling in the low-gain region of the DEPFET response also increases: it is possible to allocate more photons in the same number of bins

Dynamic  range  for  1keV  ph  –  8  bits  (~2400  Ph.)  

256  x  bin  size  @1  keV  

8  bit    28  bins  =  256  bin  

Bin  size  

Bin  size  

1  bin  /  ph.  

1  ph  @3keV  

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Dynamic range

1  ph  @1keV  Bin  size  

Dynamic  range  for  1keV  ph  –  8  bits  (~2400  Ph.)  

256  x  bin  size  @1  keV  

The  achievable  dynamic  range  depends  on:  •  The  shape  of  the  DEPFET  non-­‐linear  characteris+c  •  The  number  of  bits  of  the  ADC  •  The  number  of  bins  of  the  ADC  associated  to  the  signal  produced  by  the  first  collected  photon  •  The  photon  energy.  

•  The  dynamic  range  increases  with  the  number  of  bits  

1  bin  /  ph.  

Dynamic  range  for  1keV  ph  –  9  bits  (~12080  ph.)    

512  x  bin  size  @1  keV  

9  bit    29  bins  =  512  bin  

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DSSC overview - ASIC

Every ASIC pixel comprises in 206 x 236 µm: •  A trapezoidal analog filter (optimum filter for white series noise) •  A single slope 8 bit ADC (9 bit for f≤2.2 MHz) •  An SRAM able to store ≥640 frames

Gain  and  offset  can  be  adjusted  pixel-­‐wise  

Single  slope  ADC  ASIC  final  format  :  64  x  64  pixels  130  nm  CMOS  Process  C4  Bumps  

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MAIN  ACHIEVEMENTS  (on  sensor  and  readout  ASIC)  

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Sensor - Measured Non-linear 7-cell DEPFET Prototype

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spectroscopy

o  Fe55 source

linear region of the gain curve

noise peak ~ 10 el. ENC

Mn-Kα line ~ 150 eV FWHM @ 5.9 keV

Response to a pulsed laser/electrical charge injection

increasing number of identical pulses

peaks are equidistant in terms of signal charge

signal compression @ large charge amount

"energy" calibration using Fe55 spectrum

non-linear gain of DEPFET prototype

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non-­‐linear  gain  DEPFET  (pxd-­‐7)  

signal compression

o  seven cells of a cluster

o  standard variant (W/L = 25/3)

o  sensitivity in the linear region

gq ≈ 600 pA/el.

o  compression factor

~ 17.5

o  current dispersion

ΔI/I ≈ 10 %

non-linear vs. spectroscopy type DEPFET

o  equal gate dimensions

W/L = 25/3

o  performance at small energy

equal within sample-to-sample variation

o  spectroscopy-type DEPFET stays linear

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13sep11  

  The full format sensors in the final technology are in production

  3 sensors in final 128 x 256 format

  7 prototypes in 128 x 64 format

  small test structures

- 8 x 8, bump-bonded matrices - 7 pixel clusters wire bonded

structures

 Only the Cu layer is still missing PXD-­‐8  wafer  –  layout  program  screenshot  

Full size sensor production

1st probe station measurements

DEPFET characteristics IS(VGS)

  threshold voltage

Vth = 1.9 V

  transconductance

gm ≈ 100 µA/V @ IS = 100 µA

  all measured paramters are within specs

•  We expect a successful end of the production by spring 2013

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•  UBM  –  third  metal  layer  Cu  

–  Cu  electro-­‐pla+ng  process  installed  and  commissioned  –  sensor  dummies  and  test  structures  produced  –  Tests  on  double-­‐sided  diodes  and  MOS  caps  in  the  DSSC  technology  

–  No  altera+on  of  the  electrical  proper+es    Leakage  current  of  double  sided  diodes    CV  curves  of  MOS  structures  

~6µm  of  Cu,  on  SiO2  

interconnection – Cu deposition

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Flip-chip at HLL

Bumped chips with daisy chains:

:- Al-BCB-Cu (~4µm) technology

:- PacTech SAC305 bumps, ~200 µm pitch, ~4000

bumps/chip

:- 1.4x1.5 cm²

Test substrates:

:- landing pattern for chips, daisy chains

:- Al-BCB-Cu (~4µm) layer, no solder stop

:- two chips/substrate

Segmentation of the daisy chains:

max: 2048 solder connections

min: 32 solder connections

SAC305:  Sn96.5Ag3.0Cu0.5,  Liquidus:  220  °C,  Solidus:  217  °C  

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flip chip – daisy chains

“Perfect”  (self)  alignment  (for  this  pitch  at  least)  

  Daisy chain results   Chip 1: all of 4096 good   Chip2 : 1 line of 32 bumps faulty

»  1 or 32 bumps bad??? Bump??

  If 32/8196 bad: 99.6 % yield   If 1/8196 bad: 99.99 % yield

  profiler measurements show that the chips and substrate are almost perfectly plane-parallel on the 5µm level

  gap between chips: 150 µm (left), 148 µm(right)

150  µm  

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8 x 8 Mini-ASIC prototype

229  x  204  µm  

13.0 el

1 MHz

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~15  e   250ns filtering

Noise fully compatible with expectations

55Fe  

8 x 8 Matrix ASIC measurements

  ADC characteristic   Monotonic, no missing codes   INL~ 0,5 LSB, DNL~16%

  Full readout chain measurements:

  55Fe spectrum acquired with the full chain and standard DEPFET

  Non-linear DEPFET characteristic

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System  Simula+on  

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DSSC simulation:   1 keV photons   1 keV calibration: one bin per photon   noise as estimated for 4.5 MHz operation   Split events   ASIC measured parameters

[pho

tons/pixel]  

[pho

tons/pixel]  

input  photon  distribu+on  

reconstructed  photon  distribu+on  

   System  Simula+on  

T4 virus diffraction pattern S. Kassemeyer, “Femtosecond free-electron laser x-ray diffraction data sets for algorithm development,” Opt. Express, vol. 20, no. 4, pp. 4149–4158, Feb 2012.

False  photon  detec+on:  P(1|0)  =  0.003  

False detection

Difference  smaller  than  Poisson  error  of  input  signal  

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Summary & Conclusions

  We are developing a Pixel Detector system for the European XFEL based on innovative non-linear DEPFET devices

  In our fully parallel readout scheme, the signals coming from the pixels are filtered, digitized and stored in the focal plane

  The DEPFET signal compression principle has been experimentally verified

  An 8x8 readout ASIC comprising the whole pixel readout chain has been produced and tested.

  Estimations based on the first experimental result show that it will be possible to achieve single photon detection and high dynamic range also for low energies.

  The first DSSC Sensor full format sensors will be available in spring 2013. One working quadrant (512 x 512 ) will be available in 2015

  The full camera will be available in the middle of 2017

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Thank  You  

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