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Past and Future of Microelectronics in HEP A roadmap for R&D in microelectronics for Detector Builders A. Marchioro CERN/PH-ESE

Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

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Page 1: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Past and Future of Microelectronics in HEP

A roadmap for R&D in microelectronics forDetector Builders

A. Marchioro CERN/PH-ESE

Page 2: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Topics

• “Scaling”: the mantra for industrial microelectronics 1965-2015

– Where is industry going

• How did microelectronics benefit HEP for LHC 1.0

• How can microelectronics benefit HEP for the next 20 years

• Conclusions

A. Marchioro / TWEPP-2015 2

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SCALING AND TRENDS

The external environment

A. Marchioro / TWEPP-2015 3

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50th anniversary of G. Moore’s paper

A. Marchioro / TWEPP-2015 4

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A. Marchioro / TWEPP-2015 5

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50th anniversary of G. Moore’s paper

A. Marchioro / TWEPP-2015 6

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Who’s scaling

Moore’s Scaling Dennard’s Scaling

A. Marchioro / TWEPP-2015 7

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1965 statement still true in 2014

A. Marchioro / TWEPP-2015 8_____________________________from M. Bohr, Intel IDF 2014

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Scaling revisited

The fundamental objective that the microelectronics industry has pursued in the past 50 years may not have been:

“How to make transistors smaller and smaller at each new generation”

but rather:

“How to make transistors cheaper and cheaper at each new generation”

A. Marchioro / TWEPP-2015 9

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Strained Silicon

Timeline of significant innovations

A. Marchioro / TWEPP-2015 10

1997 1999 2001 2003 2005 2007 2009 2011 2013 2015

Node 180 130 90 65 45 32 22 14 [nm]

I n n o v a t i

o n s

High K-metal gate

Wet litho

FinFET

Cu metalization

SOI

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Abstract

A. Marchioro / TWEPP-2015 11

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Technologies around the corner

• FinFet

• FDSOI

• TSVs

• Wafer-to-wafer stacking

• Truly 3D monolithic CMOS

• New materials (III-IV, Ge, GaN, SiC, etc.)

• New phenomena: non kT/q controlled thresholds slopes

A. Marchioro / TWEPP-2015 12

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FinFET: a new device with a long incubation

13

IBM – IEDM 1992Hitachi – 1991

Toshiba– 1987Hitachi(?)– 1984

A. Marchioro / TWEPP-2015

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FinFET Detail

A. Marchioro / TWEPP-2015 14

Lg

Hfi

n

TfinS D

G

Lspacer

• Lg same for all devices

• Hfin >> Tfin

• Top Ox same as Lateral Ox -> Tri-Gate, – if >> Lateral Oxide -> FinFET

• Wfin = 2 * Lfin (+Tfin)

• W S,D >> Tfin

WD

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Multi-Gate variations

A. Marchioro / TWEPP-2015 15

Intel’s tri-gate

SOI tri-gate Gate-All-Around Omega-gate Si-bulk tri-gateSOI two-gate

BOX

Si

Ox

Gate

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Intel TRI-Gate

A. Marchioro / TWEPP-2015

Sou

rce:

Inte

l

42 nm

42

nm

14 nm

Metalization detail

16

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Typical FinFET dimensions

A. Marchioro / TWEPP-2015 17

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TSMC FinFET

A. Marchioro / TWEPP-2015

FinFET based SRAM,0.07 mm2 per bit,presented at ISSCC 2014

18

16 nm FinFET from TSMC

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FinFET @ TSMC

A. Marchioro / TWEPP-2015 19

TSMC: 16nm FinFET vs. 28nm HKMG TSMC: 16nm FinFET gain

TSMC: 16nm FinFET Low Intermetal C

IEEE Copyright License # 3713701218108

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STM FDSOI

A. Marchioro / TWEPP-2015 20

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28nm FDSOI from ST

A. Marchioro / TWEPP-2015 21

IEEE Copyright License # 3714120873338

Page 22: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Roche, ESA QCA Days

07’09’11’NSREC’14

Lowest (best) error rates against space ions in 28nm UTBB FDSOI

• 3 and 2 decades lower respectively than CMOS 65nmn and 28nm (no SEGR/SEL)

Soft Error Rate in SRAMs on 28nm FDSOI A

rbit

rary

un

its

28

nm

FDSO

I

No

rmal

ize

d h

eav

y io

n e

rro

r ra

tes

no

mit

igat

ion

Ion’s ionizing power22

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esy

of

P. R

och

e, S

TMic

roe

lect

ron

ics

A. Marchioro / TWEPP-2015

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Advanced pixel stacking Imager

A. Marchioro / TWEPP-2015 23

IEEE Copyright license # 3713700835455

Page 24: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Sensor 500mm

(edgeless)

Medipix Chip

thinned to 120mmWire bond for sensor HV bias

Sensor 200mm

Chip 750mm

ASIC wire bonds

TSVs on Medipix3

TSV: CEA-Leti, FR

Flip chip: Advacam, FI

A. Marchioro / TWEPP-2015 24 Co

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Alo

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al.,

CER

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OLD

Inte

rco

nn

ect

NEW

Inte

rco

nn

ect

Page 25: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Monolithic 3D for memories (1)

NAND Flash Architecture

A. Marchioro / TWEPP-2015

Sel

BitLine

BSel

WL < 3>

WL < 0 >

Flash Transistor has two gates, an external and a "Floating" gate.

The Floating gate modifies the Vt of the transistor

(from negative to positive if programmed)

Vg = 0 QFG = 0 ID = 0

Vg = 0 QFG = qP ID > 0

Vg =Vh QFG = X ID > 0 (transistor is conductive)

VG

¯ ID

QFG

25

Page 26: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Monolithic 3D for memories (2)

A. Marchioro / TWEPP-2015Co

urt

esy

of Chipworks

Note:Each memory bit is stored as trapped charge on the gate of a transistor.

Today a “1” is represented by something like 500-1000 e- trapped,implying a leakage current of << 1 e-/month for a 10 years retention.

26

Page 27: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Monolithic 3D for memories (2’)

A. Marchioro / TWEPP-2015 27

IEEE Copyright License # 3714760945230

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Future Devices: Steep Swing FETs

A. Marchioro / TWEPP-2015

(Notice that unfortunately the SS is steep only for high VDS!)

28

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Conclusion: Is scaling really finished in industry?

• If one calls “scaling” only the (2D) miniaturization of transistors, then definitively Dennard’s scaling is closer to saturation than Moore’s.

• If instead one calls scaling the reduction in cost (somehow) of the $/transistor on a chip, then surely several more generations are ahead of us.

A. Marchioro / TWEPP-2015 29

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MICROELECTRONICS IN HEP 1.0

The early benefits

A. Marchioro / TWEPP-2015 30

Page 31: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Major benefits

• Functionality– The ¼ um generation made the integration of 128 FE

channels and relative (analog/digital) buffering in a single chip much easier and more economical.

– Signal processing FE chips with 16+ ADCs, true DSP and buffering have also been realized (e.g. SALTRO for Alice).

• Speed– Gbit/sec class links also required a fast and low power

technology

• RH– Magically (LITERALLY) gate oxides of ~ 5 nm thickness

appeared in this generation and this (and another little layout trick) saved the day with respect to Total Dose damaging effects.

A. Marchioro / TWEPP-2015 31

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RH ADCs, circa 2002Commercial

• Bipolar tech• 595 mW, one channel

Custom

• CMOS• 120 mW / channel• No need for input and

output adapters

A. Marchioro / TWEPP-2015 32

Page 33: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

Tracker FE chips: APV

A. Marchioro / TWEPP-2015 33

100

80

60

40

20

0

Me

an

Yie

ld (

%)

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23

Lot Number

Technology “infancy”problems.

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of

G. H

all,

IC, U

K

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High Speed Links: The GOL {$}

High density, low power CMOS allowed not only to implement a high speed serializer in a chip, but

actually three to combat SEU effects

A. Marchioro / TWEPP-2015 34_____________________________________{$} Paper presented at LEB 1999

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Radiation Hardness of DSM

A. Marchioro / TWEPP-2015 35

0.001

0.01

0.1

1

10

100

1 10 100

tox (nm)

V

th/M

rad

(SiO

2)

[V/r

ad

(SiO

2)]

1.6

1.2

0.8

0.7

0.5

0.5 - A

0.5 - B

0.35

0.25 - A

0.25 - B

tox^2

N.S. Saks et al., IEEE TNS, Dec. 1984 and Dec. 1986

TEM of MOSFET gate in 130 nm technology

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MICROELECTRONICS IN HEP 2.0

The future

A. Marchioro / TWEPP-2015 36

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3 Questions to draw a roadmap

1. Can functionality be improved (invented?) with new technologies in more integrated chips?

2. Can we substantially reduce the $/channel figure with more advanced chips?

3. Can sub 65nm CMOS take us to the GRadregime?

A. Marchioro / TWEPP-2015 37

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QUESTION 1

Can functionality be improved (invented?) with more integrated chips?

A. Marchioro / TWEPP-2015 38

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SRAM Density Comparison

Node SRAM Cell Area[um2] {$}

KBits/mm2 Relative Density Gain

130nm 1.2 814 1.0

65nm 0.55 1776 2.2

28nm [bulk] .1 ~10K 12

14nm [Finfet] 0.05 ~20K 25

A. Marchioro / TWEPP-2015 39

______________________________{$} From various published sources

Page 40: Past and Future of Microelectronics in HEP...TSMC Finfet Based SRAM @ IEDM 2014 Cell size: 0.07 um2 Min Operating Voltage: 0.45V Access time @1V is 0.6ns Used in FE Size of a 128Kbit

FE memory with FinFET

TSMC Finfet Based SRAM @ IEDM 2014

Cell size: 0.07 um2

Min Operating Voltage: 0.45V

Access time @1V is 0.6ns

Used in FE

Size of a 128Kbit buffer:

128 103 * 0.07 um2 = 8.9 103 um2

=> 94x94 um

Operation @ 0.5V => ¼ of the power

A. Marchioro / TWEPP-2015 40

from Shien-Yang Wu et al: An Enhanced 16nm CMOS Technology Featuring 2nd Generation FinFET Transistors and Advanced Cu/low-k Interconnect for Low Power and High Performance Applications, IEDM 2014

IEEE Copyright License # 3713701218108

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Advanced pixels: 28nm

A. Marchioro / TWEPP-2015 41

IC-PIX28: a 28nm read-out channel for pixel detector F. Resta, G. Rota, A. Pezzotta, A. Pipino, A. BaschirottoPhysics Department University of Milano-Bicocca, Italy

To be presented at ICECS2015

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MI,

IT

Parameter Value

Tech Hi-K metal Gate

Power 4.2 uW

Input signal < 30 ke-

Detector capacitance 100 fF

Min detectable signal 1 ke-

Peaking time 11 ns

Noise level 200 e-

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High complexity FE: the MPA

• Functionality– two layers sensor to find promptly “stiff”

tracks through prompt combinations of hits in FE chips

A. Marchioro / TWEPP-2015 42

MPA Proto (3x16 channels)

• One macro pixel (1500x100 um) contains:– normal analog FE for

amp/shaping/discriminating

– clustering logic

– re-alignment logic

– pixel-strip trigger logic

– storage for L1 2,000 logic gates + 512 bit SRAM/pixel

– 3,000 gates common logic/pixel

___________________________________________For details see talk 57 by D. Ceresa on Wednesday

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QUESTION 2

Can we reduce substantially the $/channel figure with more advanced chips?

A. Marchioro / TWEPP-2015 43

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A. Marchioro / TWEPP-2015 44

A 500m2 calorimeter “could” have 5 106 chips

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Cost reduction hints

• Do not reinvent the hot water over and over– Use qualified IPs

• Reward those in the community that make them• Buy from industry (it is cheaper!)

• Complexity is in the systems– Design your system top-down, not the other way around

• Strengthen design groups – More training and education

• Today’s tools are much more capable and still largely underused• Look at what others are doing!

– Create the conditions to retain and motivate experienced designers

• Create a reward mechanism for good engineering (and not just “academic inventing”)

A. Marchioro / TWEPP-2015 45

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QUESTION 3

Can sub 65nm CMOS take us to the GRad regime?

A. Marchioro / TWEPP-2015 46

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TID @ 1 GRad

• Thin gate oxides and enclosed transistor have solved the problems of charge trapping in gate oxides and in shallow trench borders.

• Complex problems remain with:– Trapping in sidewalls, spacers, shallow tranches

– Transport mechanism of traps in different materials

– Interfaces Si-SiXX

– Holes mobility degradation

– Non SiO2 materials

– Difficulty in accessing detailed process information from “huge” foundries

A. Marchioro / TWEPP-2015 47

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Can 65nm survive 1 GRad

• Issue is much more complex than RH of ¼ um in 1996

• Discordant effects related to:– N/P

– Total dose

– Dose rate

– Size of devices

– Temperature

– Biasing conditions

– Interplay of items above

• RH > Grad is unlikely to be relevant outside HEP

• R&D Investment (manpower) required >> than what was done previously.

• See talk of Federico @ MUG

A. Marchioro / TWEPP-2015 48

65nm PMOSW=120nm, L=1umT = 25C|Vgs|=|Vds|=1.2V

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Conclusions

• Innovation is not constrained by availability of technologies!

• Their higher complexities require much stronger collaboration and coordination between players in our small community.– Only workable model:

• Ride commercial mainstream technologies• Single supplier• Common qualified library of high level, well constructed, truly portable IPs• Strictly controlled and documented design flow

• Design costs are rising (but not cost/function !), but possibilities are unbounded.

• Perhaps TID robustness > 1 Grad is “beyond physics”, therefore we might want to consider making “disposable modular detectors”. – Already done in some detectors: can wee extend the idea?

A. Marchioro / TWEPP-2015 49

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THANK YOU

A. Marchioro / TWEPP-2015 50