PROCESS STEPS Application Fields Portable Electronics (PC, PDA, - - PowerPoint PPT Presentation

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PROCESS STEPS Application Fields Portable Electronics (PC, PDA, - - PowerPoint PPT Presentation

PROCESS STEPS Application Fields Portable Electronics (PC, PDA, Wireless) IC Cost (Packaging and Cooling) Reliability (Electromigration, Latch- up) Signal Integrity (Switching Noise, DC Voltage Drop) Thermal Design


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SLIDE 1
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SLIDE 2
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SLIDE 3

PROCESS STEPS

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SLIDE 4

Application Fields

  • Portable Electronics (PC, PDA,

Wireless)

  • IC Cost (Packaging and Cooling)
  • Reliability (Electromigration, Latch-

up)

  • Signal Integrity (Switching Noise,

DC Voltage Drop)

  • Thermal Design
  • Ultra-low-power applications
  • Space missions (miniaturized

satellites)

Arun N. Chandorkar, IIT Bombay

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SLIDE 5

Different Constraints for Different Application Fields

  • Portable devices: Battery life-time
  • Telecom and military: Reliability

(reduced power decreases electromigration, hence increases reliability)

  • High volume products: Unit cost

(reduced power decreases packaging cost)

Arun N. Chandorkar, IIT Bombay

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SLIDE 6

Is Transistor a Good Switch?

On I = ∞ I = 0 Off I = 0 I = 0 I ≠ 0 I = 1ma/u I ≠ 0 I ≠ 0 Sub-threshold Leakage

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SLIDE 7

4 5

MOSFET Scaling Problem: Saturation of IDsat

200 400 600 800

0.1 0.2 0.25 0.3 0.4 0.6 0.8 1.0

NMOS PMOS IDsat (A/m) (drive current) Channel Length (µm)

Data from IBM, TI, Intel, AMD, Motorola and

Lucent

Low OFF current desirable

0.4 0.8 1.2 1990 1995 2000 2005 1 10 Supply Voltage (V) Drive Current (mA/µm)

Changhoon Choi, PhD Thesis, Stanford Univ., 2002

Constant OFF current Limit Relaxed OFF current Limit

Source: Intel

Low Vt High Vt

IOFF,hig h Vt IOFF,low Vt

Vg log Id

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SLIDE 8

Leakage Power

0% 10% 20% 30% 40% 50% 1.5 0.7 0.35 0.18 0.09 0.045

Technology (µ) Leakage Power (% of Total)

Must stop at 50%

Leakage power limits Vt scaling

  • A. Grove, IEDM 2002

INTEL

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SLIDE 9

Subthreshold Leakage (A/µµ) Operation Frequency (a.u.) e) 100 10 1

Source: 2007 ITRS Winter Public Conf.

The limit is deferent depending on application

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SLIDE 10

Gate Oxide is Near Limit

Poly Si Gate Electrode Si Substrate 1.5 nm Gate Oxide

70 nm Si3N4 CoSi2

130nm Transistor

Will high K happen? Would you count on it?

INTEL

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SLIDE 11
  • P. P. Gelsinger, “Microprocessor for the New Millennium: Challenges,

Opportunities, and New Frontiers,” Dig. Tech. 2001 ISSCC, San Francisco, pp.22-23, February, 2001

Microprocessors Trend expected in 2001

Today: 2002 (Intel) Lg sub-70 nm Tox 1.4 nm f 2.53 GHz P several 10 W N 50 M Heat Generation 2002 10W/cm2 Hot Plate 2006 100W/cm2 Surface of Nuclear Reactor 2010 1000W/cm2 Rocket Nozzle 2016 10000W/cm2 Sun Surface 2008 (Intel) Lg sub-25 nm Tox 0.7 nm f 30 GHz P 10 kW N 1.8B MIPS 1M MIPS (TIPS) Power Increase

  • Tr. Number increase

Clock Frequency increase Cause Solution: Low supply Voltage Past: 1972 (Intel) Lg 10,000 nm Tox 1200 nm f 0.00075 GHz P a few 100 mW N 2.25k Heat generation increase

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SLIDE 12

20 40 60 80 100 120

  • 39.71
  • 25.27
  • 10.83

3.61 18.05 32.49

∆VTn(mv) # of Chips

~30mV

VT Distribution

0.18 micron ~1000 samples

Low Freq Low Isb High Freq Medium Isb High Freq High Isb

INTEL

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SLIDE 13

Impact on Path Delays

Path Delay

Path delay variability due to variations in Vdd, Vt, and Temp Impacts individual circuit performance and power Optimize each circuit for full chip objectives

Delay Probability

Objective: full chip performance, power, and yield Multivariable optimization of individual circuit—Vdd, Vt, size

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SLIDE 14

Towards the end of the (ITRS) Roadmap

  • Feature sizes approach

single-digit nanometers

  • Physical and economic

limits to scaling

Red Brick Wall!

New Technologies

– Chemically Assembled Electronic Nanotech. (CAEN) – Extreme Ultraviolet (EUV) Lithography

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SLIDE 15

Qi Xinag, ECS 2004, AMD

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SLIDE 16

Gate Oxd Channel

Electron wave length 10 nm Channel length?

Scaling limit?

Hiroshi Iwai

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SLIDE 17

5 nm gate length CMOS

  • H. Wakabayashi

et.al, NEC IEDM, 2003

Length of 18 Si atoms

Is a Real Nano Device!!

5 nm

Hiroshi Iwai

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SLIDE 18

Electron wave length 10 nm Tunneling distance 3 nm Atom distance 0.3 nm

Prediction at present

Practical limit because of off-leakage between S and D?

Lg = 5 nm?

MOSFET operation

Lg = 2 ~ 1.5 nm?

But, no one knows future!

Gate length

Prediction now!

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SLIDE 19

By Robert Chau, IWGI 2003 0.8 nm Gate Oxide Thickness MOSFETs operates 0.8 nm: Distance of 3 Si atoms!!

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SLIDE 20

So, we are now in the limitation Of Scaling? Do you believe this or do not????

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SLIDE 21

There is a solution! To use high-k dielectrics

Thin gate SiO2 Thick gate high-k dielectrics Almost the same electric characteristics However, very difficult and big challenge! Remember MOSFET had not been realized without Si/SiO2!

K: Dielectric Constant

Thick Small leakage Current

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SLIDE 22
  • R. Hauser, IEDM Short Course, 1999

Hubbard and Schlom, J Mater Res 11 2757 (1996)

  • Gas or liquid

at 1000 K

  • H

○ Radio active He

  • ● ● ● ● ●

Li B e

B C N O F Ne ①

  • ● ● ●

NaMg

Al Si P

S Cl Ar ② ① ① ① ① ① ① ① ① ① ① ● ● ● ● K Ca Sc Ti V Cr Mn Fc Co Ni Cu Zn Ga Ge As Se Br Kr

  • ① ①

① ① ① ● ① ① ① ① ① ● ● Rh Sr Y Zr Nb Mo Tc Ru Rb Pd Ag Cd In Sn Sb Te I Xe

① ① ① ① ① ● ● ● ● ① ① ○ ○ ○ Cs Ba ★ Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn ○ ○ ○ ○ ○ ○ ○ ○ Fr Ra ☆ Rf Ha Sg Ns Hs Mt ○

LaCe Pr Nd PmSmEuGdTbDyHo Er TmY bLu

○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ Ac Th Pa U Np Pu AmCm Bk Cf Es Fm Md No Lr ★ ☆

Candidates

Na

Al Si P

S Cl Ar ② ① ① ① ① ① ① ① ① ① ● ● ● ● K

Sc Ti

V Cr Mn Fc Co Ni Cu Zn Ga Ge As Se Br Kr

  • ① ①

① ① ① ● ① ① ○ ○ ○ ○ ○ ○ Ac Th Pa U Np Pu AmCm Bk Cf Es Fm Md No Lr ★ ☆

② ③

Unstable at Si interface

Si + MOX M + SiO2

Si + MOX MSiX + SiO2 Si + MOX M + MSiXOY

Choice of High-k elements for oxide

HfO2 based dielectrics are selected as the first generation materials, because of their merit in 1) band-offset, 2) dielectric constant 3) thermal stability La2O3 based dielectrics are thought to be the next generation materials, which may not need a thicker interfacial layer

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SLIDE 23

Intel’s announcement, January 26, 2007, and IEDM Dec 2010 Hafnium-based high-k material by ALD: EOT= 1nm Specific gate metals ( Intel’s trade secret) Different Metals for NMOS and PMOS Use of 193nm dry lithography From 45 nm to 32 nm Tech. Tr density: 2 times increase Tr witching power: 30% reduction Tr witching speed: 20% improvement S-D leakage power: 5 times reduction Gate oxide leakage: 10 times reduction 45nm processors (Core™2 family processors "Penryn") running Windows* Vista*, Linux* etc. 11nm production in the First half of 2015 or Early 2016.

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SLIDE 24

PMOS

High-k gate insulator MOSFETs for Intel: EOT=1nm EOT: Equivalent Oxide Thickness

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SLIDE 25

EOT = 0.48 nm

Transistor with La2O3 Gate Insulator

TIT results

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SLIDE 26
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SLIDE 27 back-gate channel isolation buried oxide channel top-gate Source Drain Gate

Time

Conclusion: Technology Progression

Well doping channel Depletion layer isolation halo

Bulk CMOS

Si0.8Ge0.2 Si Si (tensile) Si1-xGex

Strained Si High k gate dielectric Metal gate 3D ICs

2 nm

Cu interconnect Low-k ILD FD SOI CMOS

channel depletion layer isolation buried oxide raised source/drain

Optical interconnect Molecular device Detectors, lasers, modulators, waveguides Spin device

B + =

Ge on Si hetroepitaxy Ge on Insulator Wafer bonding Crystallization Nanowires Ge/Si Heterostrcture Double-Gate CMOS Nanowire Single e transistor Nanotube

Feature Size

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SLIDE 28

Carbon Nanotubes

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SLIDE 29

Graphene Device

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SLIDE 30

Graphene Device Electronics(??)

  • A study of how electrons behave in

circuitry made from ultrathin layers of graphite – known as graphene – suggests the material could provide the foundation for a new generation of nanometer scale devices that manipulate electrons as waves – much like photonic systems control light waves.

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SLIDE 31

Graphene 3D structure and Band Diagram

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SLIDE 32

In 2004 two scientists, Andre Geim and Konstantin Novoselov, both of whom would later receive the Nobel Prize for their work In preparation of Graphene

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SLIDE 33

Graphene based (2D Material)Transistor

Standard NMOSFET Graphene Based Transistor

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SLIDE 34

Graphene transistor and new possible Ballistic Device

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SLIDE 35

Tunneling Effect

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SLIDE 36

Coulomb Blockade

  • a Coulomb blockade

is the increased resistance at small bias voltage of an electronic device comprising at lease

  • ne low-capacitance

tunnel junction.

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SLIDE 37

Bottom-Up

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SLIDE 38

Self Assembly

  • Applicatoins: solar cell, light-emitting

diodes, capsule in drug delivery system

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SLIDE 39

Chemical Colloidal Method

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SLIDE 40

Lithography and Etching

  • Lithography: electron beam, ion beam,

nanoimprint, dip pen nanolithography

  • Etching: wet etching, dry etching, plasma,

implantation, photo etching

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SLIDE 41

Split-gate Approach

  • Use additional voltage to create 2

dimensional confinements to control the shape and size of the quantum dot’s gate.

  • It’s a combination of e beam lithography,

evaporation, lift off, contact annealing

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SLIDE 42

Limitations of CMOS in ~ 10 years

  • Fundamental physical limit
  • 8 electron per bit

(today 1000 e/bit)

  • Manufacturing cost
  • $50 Billion/FAB

Moore’s law scaling to an end ??????

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SLIDE 43
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SLIDE 44

Never Give Up! There would always be a solution!!!! Think, Think, and Think! Or, Wait for the time! when Some one will think for you As No one knows future!

Do not believe a text book statement, Or Researcher’s statement, Blindly!