Highly compact digital pixel structures developed for the ... · structures are about 29 e-with 6.5...

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A prototype named JadePix-2 comprising a matrix with 112×96 pixels has been designed and fabricated in a 0.18 μm CMOS Image Sensor process. It contains two digital pixel structures, both have been realized within 22 μm pitch size. The prototype operates in the rolling-shutter mode, with processing speeds of 100ns/row and 80ns/row, respectively, for the two pixel structures. Experimental results show the total ENC and power dissipation of the two structures are about 29 e - with 6.5 μA/pixel, and 31 e - with 3.7 μA/pixel respectively. ABSTRACT Specifications of JadePix-2 Performances of the in-pixel Amp. and dynamic Latch CONCLUSION AND PERSPECTIVES We proposed two pixel structures with balance between high precision and circuit simplicity to guarantee compact pixels (22 μm pitch size). Both versions operate in the rolling-shutter mode and take 100ns and 80ns, respectively, to process one row. Experimental results show the total ENC and power dissipation of the two structures are about 29 e - with 6.5 μA/pixel, and 31 e - with 3.7 μA/pixel respectively. The knowledge learned from JadePix-2 will guide the design of the next generation vertex detector for CEPC and achieve the desired high spatial resolution. Highly compact digital pixel structures developed for the CEPC vertex detector* Contact: [email protected] Y ang ZHOU 1 , Yunpeng LU 1 , Zhigang WU 1,2 , Tan SHI 3 , Xudong JU 4 , Jing DONG 1 , Hongbo ZHU 1 , Qun OUYANG 1,2 1 State Key Laboratory of Particle Detection and Electronics, Insitute of High Energy Physics, CAS, Beijing 100049, China 2 University of Chinese Academy of Sciences, Beijing 100049, China 3 Department of Nuclear Engineering and Raiological Sciences, University of Michigan, Ann Arbor, MI, 48109, USA 4 ShanghaiTech University, Shanghai 201210, China INTRODUCTION In-pixel architecture and signal treatment Some prototype specifications: 0.18 μm CMOS Imaging Sensor (CIS) technology; Quadruple well, 6 metal layers process; ~ 20 μm high resistivity (≥1 kΩ•cm) epitaxial layer 112×96 square pixels with 22 μm pitch size; 3×3.3 mm 2 layout size; 8 test sub-matrices for two pixel versions, D1-D4 with digital output, A1-A4 with analogue output; 8 Analogue output channels; 16 Column digital data serialized in one LVDS output pair; 7 LVDS pairs in total. Output data speed: 160 MHz Pixel version 1: 3.7 μA/pixel (power), ~31 e - (noise), 100ns/row (operation speed); Pixel version 2: 6.5 μA/pixel (power), ~29.5 e - (noise), 80ns/row (operation speed) Equivalent Cap. of the sensing node Figure 1: Layout (left) and architecture (right) of JadePix-2. The proposed CEPC (Circular Electron Positron Collider) will offer the measurements of the Higgs properties with a new level of precision. The precise determination of the charged particle tracks and reconstruction of the primary and displaced decay vertices, impose stringent requirements on the CEPC vertex detector, which somehow incompatible with each other, such as high spatial resolution (<3μm), low power consumption (<50mW/cm 2 ) and fast processing speed (<10μs/frame). CMOS pixel sensor with pixel level discrimination represents one of the most promising candidates. However, the complexity of in-pixel digital circuit always leads to increased pixel size, which is disfavored to obtain high spatial resolution. In this context, we propose two pixel structures with balance between high precision and circuit simplicity to guarantee compact pixels, yet with satisfying high signal over noise ratio. Both of the two structures are based on the DMAPS (Depleted Monolithic Active Pixel Sensors) concept, employ a high-voltage (up to 10 V) biased charge collection diode, AC-coupled to a comparator with OOS (Output Offset Storage) technique to mitigate pixel-to-pixel performance dispersion. The main difference between the two structures concentrates on the signal amplification stage used in the comparator. LATCH Out+ Out- AMP V ref1 V ref1 V ref_latch V ref_latch V ref2 Read Read Read Read Read Calib Calib Calib Clamp Latch V bias Power_on Buff Row_sel Out LATCH Out+ Out- AMP V ref3 V ref1 V ref_latch Clamp Calib Latch V bias AMP RST1 V ref2 V ref2 RST2 Power_on Power_on Buff Row_sel Out Figure 3: Two pixel structures with a differential amplifier + Latch (version 1, left), and two stage Common-Source amplifier +Latch (version 2, right). D1 D2 D3 D4 A1 A2 A3 A4 v Sequence Analogue out buffer (×8) PISO 16 in 1 (×7) v IHEP logo 100 ns Power_on Latch Read Calib Clamp Sel_b Pre_Power on A_D conversion Read_out Pre_Power on A_D conversion time Read_out Clock_160MHz Next row A_D conversion Reset & Read_out Power_on Latch RST1 RST2 Calib Clamp Sel_b 80 ns Pixel version TN FPN Version 1 negligible ≈ 4 e - Version 2 negligible negligible Input DC level: 520 mV Gain: ~ 52 RMS of Gain distribution: ~ 15 Input DC level: 600 mV Gain: ~ 6.9 RMS of Gain distribution: ~ 0.4 In-pixel Architecture: High-voltage biased N-well/p-epi collection node (V bias up to 10V) AC coupled to the following electronics. Comparators designed with the Output Offset Storage (OOS) technique; Thresholds adjusted externally at the differential amplifier (Version 1) and at the dynamic Latch (Version 2) ; Signal and Noise treatment: The useful signal (amount of e - collected by the diode) is translated into a ΔV on the diode; AC coupled structure transmit this ΔV to the following comparators where signal is amplified and digitalized; digital signal is then stored in the Latch and output to column through a digital buffer row by row; The offsets of the amplifiers are compensated by the combined offset cancellation technique; Figure 4: operation timing of the pixel version 1 (left) and version 2 (right). Figure 5: schematic of the signal transmission used for the 55 Fe source test (while it was not an good option for this test) Figure 9: Fix Pattern Noise (left) and Temporal Noise (right) of the in-pixel dynamic Latch. (test results) Table 1: ENC of the in-pixel latch. Figure 2: Layout of the two pixel versions, both pitch sizes are 22μm. Differential amplifier in pixel version 1: Single-end CS Amplifier in pixel version 2: Figure 7: Gain distribution of the in-pixel differential amplifiers; the value includes 6.4 amplitude on the PCB and 0.8 of two-stage source followers on the sensor. Performances of the pixel matrix * This study was supported by the National Key Program for S&T Research and Development (2016YFA0400400) and the National Natural Science Foundation of China (11605217) C= ≈ 4.9 1640 e - collection peak - 4 stage Amp.: limit only ~ 10 mV linear response range on the sensing node; leave other situation either no gain or saturated. - the Amp. was tuned to let the input signal ~ 1600e - in the linear response range, while no response for smaller signals and saturate for larger ones. - Events only with S/N > 10 was recorded. Threshold Distribution Entries 1536 Mean 0.575 Std Dev 0.00108 0.566 0.568 0.57 0.572 0.574 0.576 0.578 0.58 Threshold [V] 0 50 100 150 200 250 300 350 400 Numbers per entry Threshold Distribution Entries 1536 Mean 0.575 Std Dev 0.00108 Temporal Noise Entries 1536 Mean 0.0004174 Std Dev 0.0002302 0 0.0005 0.001 0.0015 0.002 0.0025 0.003 0.0035 0.004 Noise [V] 0 50 100 150 200 250 300 350 Numbers per entry Temporal Noise Entries 1536 Mean 0.0004174 Std Dev 0.0002302 Num. of events Figure 8: Gain distribution of the in-pixel two stages single-end CS amplifiers; the value includes 0.8 of two-stage source followers on the sensor. Gain in-pixel = Mean value/(0.8*6.4) Gain in-pixel = Mean value/0.8 FPN = 1.15 mV TN = 0.1 mV FPN = 1.08 mV TN = 0.4 mV FPN = 53.3/52 = 1.03 mV TN= 10.27/52 ≈ 0.2 mV Figure 10: Noise (equivalent at the sensing node) of pixel matrix version 1: FPN (left) and TN (right) Matrix version TN FPN Total Noise Version 1 11 e - 29 e - ~31 e - Version 2 5.5 e - 29 e - ~29.5 e - Figure 11: Noise (equivalent at the sensing node) of pixel matrix version 2: FPN (left) and TN (right). Table 2: ENC of the pixel matrix. Figure 6: Charge collection response peak of 55 Fe source: the X-axis value shows the ΔV on the sensing node while the whole 1640 e- were collected by one pixel. Pixel level Column level Chip level P+/Nwell Nwell/Psub V_diode AMP AMP NMOS-SF Output PMOS-SF Set-up conditions:

Transcript of Highly compact digital pixel structures developed for the ... · structures are about 29 e-with 6.5...

Page 1: Highly compact digital pixel structures developed for the ... · structures are about 29 e-with 6.5 μA/pixel, and 31 e-with 3.7 μA/pixel respectively. The knowledge learned from

A prototype named JadePix-2 comprising a matrix with 112×96 pixels has been designed

and fabricated in a 0.18 μm CMOS Image Sensor process. It contains two digital pixel structures,

both have been realized within 22 μm pitch size. The prototype operates in the rolling-shutter

mode, with processing speeds of 100ns/row and 80ns/row, respectively, for the two pixel

structures. Experimental results show the total ENC and power dissipation of the two structures

are about 29 e- with 6.5 μA/pixel, and 31 e- with 3.7 μA/pixel respectively.

ABSTRACT

Specifications of JadePix-2

Performances of the in-pixel Amp. and dynamic Latch

CONCLUSION AND PERSPECTIVES

We proposed two pixel structures with balance between high precision and circuit simplicity to guarantee

compact pixels (22 μm pitch size). Both versions operate in the rolling-shutter mode and take 100ns and 80ns,

respectively, to process one row. Experimental results show the total ENC and power dissipation of the two

structures are about 29 e- with 6.5 μA/pixel, and 31 e- with 3.7 μA/pixel respectively. The knowledge learned

from JadePix-2 will guide the design of the next generation vertex detector for CEPC and achieve the desired

high spatial resolution.

Highly compact digital pixel structures developed for the

CEPC vertex detector*

Contact: [email protected]

Yang ZHOU1, Yunpeng LU1, Zhigang WU1,2, Tan SHI3, Xudong JU4, Jing DONG1, Hongbo ZHU1, Qun OUYANG1,2

1State Key Laboratory of Particle Detection and Electronics, Insitute of High Energy Physics, CAS, Beijing 100049, China2University of Chinese Academy of Sciences, Beijing 100049, China3Department of Nuclear Engineering and Raiological Sciences, University of Michigan, Ann Arbor, MI, 48109, USA4ShanghaiTech University, Shanghai 201210, China

INTRODUCTION

In-pixel architecture and signal treatment

Some prototype specifications: 0.18 µm CMOS Imaging Sensor (CIS) technology;

Quadruple well, 6 metal layers process;

~ 20 μm high resistivity (≥1 kΩ•cm) epitaxial layer

112×96 square pixels with 22 µm pitch size;

3×3.3 mm2 layout size;

8 test sub-matrices for two pixel versions, D1-D4

with digital output, A1-A4 with analogue output;

8 Analogue output channels;

16 Column digital data serialized in one LVDS

output pair; 7 LVDS pairs in total.

Output data speed: 160 MHz

Pixel version 1: ~3.7 μA/pixel (power), ~31 e-

(noise), 100ns/row (operation speed);

Pixel version 2: ~6.5 μA/pixel (power), ~29.5 e-

(noise), 80ns/row (operation speed)

Equivalent Cap. of the sensing node

Figure 1: Layout (left) and architecture (right) of JadePix-2.

The proposed CEPC (Circular Electron Positron Collider) will offer the measurements of

the Higgs properties with a new level of precision. The precise determination of the charged

particle tracks and reconstruction of the primary and displaced decay vertices, impose stringent

requirements on the CEPC vertex detector, which somehow incompatible with each other, such

as high spatial resolution (<3μm), low power consumption (<50mW/cm2) and fast processing

speed (<10μs/frame). CMOS pixel sensor with pixel level discrimination represents one of the

most promising candidates. However, the complexity of in-pixel digital circuit always leads to

increased pixel size, which is disfavored to obtain high spatial resolution.

In this context, we propose two pixel structures with balance between high precision and

circuit simplicity to guarantee compact pixels, yet with satisfying high signal over noise ratio.

Both of the two structures are based on the DMAPS (Depleted Monolithic Active Pixel Sensors)

concept, employ a high-voltage (up to 10 V) biased charge collection diode, AC-coupled to a

comparator with OOS (Output Offset Storage) technique to mitigate pixel-to-pixel performance

dispersion. The main difference between the two structures concentrates on the signal

amplification stage used in the comparator.

LATCH

Out+

Out-AMP

Vref1

Vref1

Vref_latch

Vref_latch

Vref2Read

Read

Read

Read

Read

Calib

Calib

Calib

Clamp

LatchVbias

Power_on

Buff

Row_sel

Out

LATCH

Out+

Out-AMP

Vref3

Vref1

Vref_latch

Clamp

Calib

LatchVbias

AMP

RST1

Vref2 Vref2

RST2

Power_on Power_on

Buff

Row_sel

Out

Figure 3: Two pixel structures with a differential amplifier + Latch (version 1, left), and two stage Common-Source amplifier +Latch (version 2, right).

D1 D2

D3 D4

A1

A2

A3

A4

v

Seq

uen

ce

Analogue out buffer (×8)

PISO 16 in 1 (×7)

vIHEP logo

100 ns

Power_on

Latch

Read

Calib

Clamp

Sel_b

Pre_Power on A_D conversion Read_out

Pre_Power on A_D conversion time Read_out

Clock_160MHz

Next row

A_D conversion Reset & Read_out

Power_onLatch

RST1

RST2

Calib

Clamp

Sel_b

80 ns

Pixel version TN FPN

Version 1 negligible ≈ 4 e-

Version 2 negligible negligible

Input DC level: 520 mV

Gain: ~ 52

RMS of Gain distribution: ~ 15

Input DC level: 600 mV

Gain: ~ 6.9

RMS of Gain distribution: ~ 0.4

In-pixel Architecture: High-voltage biased N-well/p-epi collection node (Vbias up to 10V) AC coupled to the following electronics.

Comparators designed with the Output Offset Storage (OOS) technique;

Thresholds adjusted externally at the differential amplifier (Version 1) and at the dynamic Latch (Version 2) ;

Signal and Noise treatment:

The useful signal (amount of e- collected by the diode) is translated into a ΔV on the diode; AC coupled

structure transmit this ΔV to the following comparators where signal is amplified and digitalized; digital

signal is then stored in the Latch and output to column through a digital buffer row by row;

The offsets of the amplifiers are compensated by the combined offset cancellation technique;

Figure 4: operation timing of the pixel version 1 (left) and version 2 (right).

Figure 5: schematic of the signal transmission used for the 55Fe source test (while it was not an good option for this test)

Figure 9: Fix Pattern Noise (left) and Temporal Noise (right) of the in-pixel dynamic Latch. (test results)

Table 1: ENC of the in-pixel latch.

Figure 2: Layout of the two pixel versions, both pitch sizes are 22μm.

Differential amplifier in pixel version 1: Single-end CS Amplifier in pixel version 2:

Figure 7: Gain distribution of the in-pixel differential amplifiers;

the value includes 6.4 amplitude on the PCB and 0.8 of two-stage

source followers on the sensor.

Performances of the pixel matrix

* This study was supported by the National Key Program for S&T Research and Development (2016YFA0400400) and the National Natural Science Foundation of China (11605217)

C= 𝑄

𝑉≈ 4.9𝑓𝐹

1640 e- collection peak

- 4 stage Amp.: limit only ~ 10 mV linear response range on the sensing node; leave other situation either no gain or saturated.

- the Amp. was tuned to let the input signal ~ 1600e- in the linear response range, while no response for smaller signals and saturate for larger ones.

- Events only with S/N > 10 was recorded.

Threshold Distribution

Entries 1536

Mean 0.575

Std Dev 0.00108

0.566 0.568 0.57 0.572 0.574 0.576 0.578 0.58

Threshold [V]

0

50

100

150

200

250

300

350

400

Nu

mb

ers

pe

r e

ntr

y

Threshold Distribution

Entries 1536

Mean 0.575

Std Dev 0.00108

Temporal Noise

Entries 1536

Mean 0.0004174

Std Dev 0.0002302

0 0.0005 0.001 0.0015 0.002 0.0025 0.003 0.0035 0.004

Noise [V]

0

50

100

150

200

250

300

350

Num

bers

per

ent

ry

Temporal Noise

Entries 1536

Mean 0.0004174

Std Dev 0.0002302

Nu

m. o

f ev

ents

Figure 8: Gain distribution of the in-pixel two stages single-end CS

amplifiers; the value includes 0.8 of two-stage source followers on

the sensor.

Gainin-pixel = Mean value/(0.8*6.4) Gainin-pixel = Mean value/0.8

FPN = 1.15 mVTN = 0.1 mV

FPN = 1.08 mV TN = 0.4 mV

FPN = 53.3/52 = 1.03 mV TN= 10.27/52 ≈ 0.2 mV

Figure 10: Noise (equivalent at the sensing node) of pixel matrix version 1: FPN (left) and TN (right)

Matrix version TN FPN Total Noise

Version 1 11 e- 29 e- ~31 e-

Version 2 5.5 e- 29 e- ~29.5 e-

Figure 11: Noise (equivalent at the sensing node) of pixel matrix version 2: FPN (left) and TN (right).

Table 2: ENC of the pixel matrix.

Figure 6: Charge collection response peak of 55Fe source: the X-axis value shows

the ΔV on the sensing node while the whole 1640 e- were collected by one pixel.

Pixel level Column

level

Chip level

P+/Nwell

Nwell/ Psub

V_diode

AMP AMP NMOS-SFOutput

PMOS-SF

Set-up conditions: