there's plenty of room at the bottom 12/29/1959

37
1 Professor N Cheung, U.C. Berkeley Lecture 26 EE143 S06 There's Plenty of Room at the Bottom 12/29/1959 Feynman asked why not put the entire Encyclopedia Britannica (24 volumes) on a pin head (requires atomic scale recording). He proposed to use electron microscope to “write” the words, and to “read” the words. He also thought that biological systems were already writing and reading information at the molecular (or nano) scale.

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Page 1: There's Plenty of Room at the Bottom 12/29/1959

1Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

There's Plenty of Room at the Bottom

12/29/1959Feynman asked why not put the entire Encyclopedia Britannica (24 volumes) on a pin head (requires atomic scale recording).

He proposed to use electron microscope to “write” the words, and to “read” the words.

He also thought that biological systems were already writing and reading information at the molecular (or nano) scale.

Page 2: There's Plenty of Room at the Bottom 12/29/1959

2Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

The Nanometer Sizescale

Nanotube

Page 3: There's Plenty of Room at the Bottom 12/29/1959

3Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Fabrication Techniques for Nano-Scale Structures

• ‘Top-down” Approaches– Lithography (E-beam,EUV)– Nano Imprint– Dip-Pen Nanolithography

• ‘Bottom-up' Approaches– Selective growth – Self-assembly – Scanning Tip Manipulation

Page 4: There's Plenty of Room at the Bottom 12/29/1959

4Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06 e-beam lithography resolution factors

• beam quality ( ~1 nm)

• secondary electrons ( lateral range: few nm)

performance records

organic resist PMMA ~ 7 nm

inorganic resist, b.v. AlF3 ~ 1-2 nm

Page 5: There's Plenty of Room at the Bottom 12/29/1959

5Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

The benchmark of Top-down Approach5nm-Gate Nanowire FinFET

2004 Symposium on VLSI Technology, p.196

Page 6: There's Plenty of Room at the Bottom 12/29/1959

6Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Technology Gap for Top-Down Approach

Page 7: There's Plenty of Room at the Bottom 12/29/1959

7Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

How to make a single-Crystal Si Nanowire

Page 8: There's Plenty of Room at the Bottom 12/29/1959

8Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Y.Ono et al., “Si complementary single-electron inverter”, IEDM, pp.367-370, 1999

Oxidation rate slows down withmechanical stress induced by surrounding oxide

Si Nanowire by thermal oxidation

Page 9: There's Plenty of Room at the Bottom 12/29/1959

9Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Prober et al, APL, 94 (1980)

30-nm wire fabrication by directional thin-film deposition

Triangular cross-section

Rectangular cross-section

Page 10: There's Plenty of Room at the Bottom 12/29/1959

10Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

dummystep

SiO2Si

Substrate

dummystep

SiO2Si

Substrate

SiO2Si

Substrate

SiO2

Substrate

Conformal CVD film 10-20nm spacer

Spaceras etching mask

Sidewall Spacer to define nm wires

nm Si

~10nm

(1) (2)

(3) (4)

Page 11: There's Plenty of Room at the Bottom 12/29/1959

11Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Twin nanowiresWith anisotropic etching of SOI

Page 12: There's Plenty of Room at the Bottom 12/29/1959

12Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

• Sacrificial layer method, deposition method, etc.• Cheaper and mass-productable methods• Soft mat’l vs. hard mat’l

Tas et al., Nano Letters, 2, 1031 (2002)

Nanochannel fabrication

Page 13: There's Plenty of Room at the Bottom 12/29/1959

13Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

www.nanonex.com

Page 14: There's Plenty of Room at the Bottom 12/29/1959

14Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

D. Piner, J. Zhu, F. Xu, and S. Hong, C. A. Mirkin, "Dip-Pen Nanolithography", Science, 1999, 283, 661–63.

* as small as 15 nm linewidths and ~5 nm spatial resolution

Dip-Pen Nanolithography

Page 15: There's Plenty of Room at the Bottom 12/29/1959

15Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Cutting window through a thin layer of Si oxide

Line dose: 3.3, 2.5, and 1.7 x 10-3 C/cm,

for the three lines from top to bottom;

“Local” E-beam

Etching an 8-nm Ag thin film

on Si(100) using the LEEB/STM

Page 16: There's Plenty of Room at the Bottom 12/29/1959

16Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

By E-Beam

Page 17: There's Plenty of Room at the Bottom 12/29/1959

17Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Growth Modes

* Au nanoparticles as catalyst

Nanowire Growth byVapor-Liquid-Solid Method

Page 18: There's Plenty of Room at the Bottom 12/29/1959

18Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

1D Functional HeterojunctionsLOHNs

• NanoElectronics•Thermoelectrics

COHNs

•NanoOptics•NanoFludics

Nanotape

•Selective sensors

Si/SiGe AlGaN/GaNTiO2/SnO2GaN/AlGaN

Prof. P. Yang, Chemistry

Page 19: There's Plenty of Room at the Bottom 12/29/1959

19Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Page 20: There's Plenty of Room at the Bottom 12/29/1959

20Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Step Coverage(Al2O3)

Page 21: There's Plenty of Room at the Bottom 12/29/1959

21Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Chemical Modification of Single Walled Nanotubes

Page 22: There's Plenty of Room at the Bottom 12/29/1959

22Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Silicon probe with a conductive single walled carbon nanotube (<2 nm diameter). The tip is at the end of a flexible cantilever designed for the atomic force microscope.

http://www.media.mit.edu/nanoscale/research/sensors.html

A nanotube-bundle tip was used as thenegative electrode to locally oxidize silicon and write the oxide pattern ‘C-Tube’. OH- ions (from condensed H2O on tip) are driven by the strong field into the solid and induce the oxidation by reacting with Si holes in bulk Si.

Page 23: There's Plenty of Room at the Bottom 12/29/1959

23Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

http://www.almaden.ibm.com:80/vis/stm/gallery.html

Title : Carbon Monoxide Man

Media : Carbon Monoxide on Platinum (111)

Title: Atom

Media: Iron on Copper (111)

Page 24: There's Plenty of Room at the Bottom 12/29/1959

24Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06Probe Manipulation Technique

Page 25: There's Plenty of Room at the Bottom 12/29/1959

25Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

The smallest transistor

-60 -40 -20 0 20 40 60

-200

-100

0

100

I (pA

)

Vsd(mV)

Vg = 6.4 VVg = 6.9 VVg = 7.4 VVg = 7.7 V

Operation onlyat low temp

Page 26: There's Plenty of Room at the Bottom 12/29/1959

26Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Potassium Doping of CNT (n-type)

Javey et al, Nano Lett. 2005

Page 27: There's Plenty of Room at the Bottom 12/29/1959

27Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Field Assisted Assembly

metallic particle+-V +V

Long-range forces attract nanowires to substrate

particle moves in gradientof field towards region of

highest field strength

dielectric medium

Theresa MayerEE Dept.

Page 28: There's Plenty of Room at the Bottom 12/29/1959

28Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Field Assisted Assembly

Nanowires attracted and aligned totop electrodes

Alignment process is self limiting

SiO2+V -V

+ -

∆V = 0V

Siliconsubstrate

SiO2+V -V

+

-

Page 29: There's Plenty of Room at the Bottom 12/29/1959

29Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

•Nanowires serve dual purpose: both active devices andinterconnects.•All key nanoscale metrics are defined during synthesis andsubsequent assembly.•Crossed nanowire architecture provides natural scaling andpotential for integration at highest densities. •No additional complexity (with added material).

Crossed Nanowire Architecture

Page 30: There's Plenty of Room at the Bottom 12/29/1959

30Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

E-field Enhanced Fluidic Alignment

Page 31: There's Plenty of Room at the Bottom 12/29/1959

31Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Surface Programmed Assembly M. Lee et al Seoul National Univ 2004

Page 32: There's Plenty of Room at the Bottom 12/29/1959

32Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06Logic Gates and Computation from Assembled NanowireBuilding Blocks

Huang et al, SCIENCE VOL 294 9 NOVEMBER 2001

*p-Si and n-GaN NWs

The OR and AND gates has no signal gain

AssemblyY. Huang,, Science 291,630 (2001).

Page 33: There's Plenty of Room at the Bottom 12/29/1959

33Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Applied Physics Letters, 82 2491(2003)

Carbon Nanotube Interconnects

Page 34: There's Plenty of Room at the Bottom 12/29/1959

34Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Empirical : Resolution (in Å) ~ 23 Areal Throughput (in µm2/hr) 0.2

Page 35: There's Plenty of Room at the Bottom 12/29/1959

35Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Principle and Practice of Top-Down Integration

* A sequence of Additive and Subtractive steps with lateral patterning

•Planarization is used to control critical dimensions (lithography, etching, and thin-film deposition)•Self-aligned structure used whenever possible•Alignment is done for ALL lithography steps (registration marksalways available on substrate)

Si wafer

ProcessingSteps

Page 36: There's Plenty of Room at the Bottom 12/29/1959

36Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

Grand Challenges of The Bottom Up Approach

Bocheva et al, PNAS April 16, 2002 vol. 99 no. 8 4937–4940

What is the optimum functional building block using self-assembly ?

How do we align the different functional blocks for integration ?

- Alignment marks- 2D or 3D alignment

Page 37: There's Plenty of Room at the Bottom 12/29/1959

37Professor N Cheung, U.C. Berkeley

Lecture 26EE143 S06

0.001

0.01

0.1

1

10

100

0 10 20 30 40

curr

ent (

nA)

time (min)

A)

Light Emitting Sensing Magnetic Assembly

Wavelength Conversion

Thermoelectronics BimorphMechanics

Catalysis

20 nm

Finite size effect.. Chemical/thermal stability issue for devices

Interface/complexity/functionalityThe integration issue: nano-micro-macro continuum.