microstructured vertically aligned carbon nanotube composites

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Microstructured Vertically Aligned Carbon Nanotube Composites. Dr. Robert Davis & Group Brigham Young University Physics and Astronomy davis@byu.edu (presented by Prof. David Allred, BYU). Outline. Vertical aligned carbon nanotube (VACNT) growth Dense nanotube structures - PowerPoint PPT Presentation

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Microstructured Vertically Aligned Carbon Nanotube

Composites

Dr. Robert Davis & Group Brigham Young UniversityPhysics and Astronomydavis@byu.edu(presented by Prof. David Allred, BYU)

Outline

• Vertical aligned carbon nanotube (VACNT) growth• Dense nanotube structures• Filling in with Si by LPCVD

• Resistivity• Crystallinity of filler material • Density, Elastic Modulus

• Constraints/Engineering Design Rules

Vertical Nanotube Growth

VACNT growth details

Si

30 nm Al2O3 (Barrier Layer)

Pattern Fe by lift-off Heat to 750 °C in H2: Ar

Ar : H2 : C2H4 at 70 : 500 : 700 sccm

1-15 nm Fe

SEM - VACNT forest

30000X – edge

4500X – 3 µm holes

100X – 50 µm holes

Can top surface and edge roughness be improved?

Photoresist

VACNT growth process

Si

30 nm Al2O3 (Barrier Layer)

1-15 nm Fe

Light

PhotoresistPhotoresist

Photolithography & lift-off

Dependence on Fe Thickness15 nm

2 nm

5.5 nm

< 1 nm

Good repeatability Rate strongly dependant on thickness

2 nm Fe on Al2O3

Small voids (< 200 nm across) Sharp features (few stray tubes);

Sidewall roughness < 200 nm High growth rate ~50 µm/min

TEM Grid

Bistable Mechanisms

Nanotube “forest” growth

• Height: up to 1mm+• Feature size: a few microns• Speed: 10-100µm/min• Density:

Material Density (kg/m3)

Air

Silica aerogel: lowest density

Measured density

Silica aerogel: usual density range

Expanded polystyrene

1.2

1.9

9.0

5 – 200

25 – 200

Low density, weakly bound material

As-grown forests are flimsy and tear off the surface at the slightest touch

Dense Nanotube Structures

Liquid Induced Densification

Dried structureSubmerged nanotube structures

Vapor Condensation Induced Densification -- Lines

Longer exposure to vapor Shorter exposure to vapor

Surface forces dominates

Unequal angles become equal angles. Final structure depends on initial structure surface forces Difficult to control what results!

Horizontal Aligned CNT films

AIST Japan group working on in-plane aligned CNT MEMS

Yuhei Hayamizu, Takeo Yamada, Kohei Mizuno, Robert C. Davis, Don N. Futaba, Motoo Yumura, & Kenji Hata Nature Nanotechnology 3, 241 (2008).

Microstructured VACNT Composites

Leave the nanotubes vertical?

Filling in with Si by LPCVD

“floor layer”

VACNT Composite MEMS Process

Solid High Aspect Ratio Structures

A variety of materials?

Filled with amorphous Si:

Filled with amorphous C:

High aspect ratio structures in a variety of materials?

              

              

   

                  

                  

                  

         

        

     

FROM: Chemical Vapor Deposition, ed. Jong-Hee Park, ASM International (2001)

Properties: Resistivity

• Isolated nanotubes: Can exhibit ballistic conduction over distances of several microns

• Undoped poly-Si: ρ ~ 102 Ω cm• Si-coated nanotubes: ρ ~ ?

• Coat tubes with insulator Conductive MEMS made from insulating materials?

Properties: Resistivity

t

K

Kt

KRsheet

1

2

1

R0

K1 = 42.6 Ω mK2 = 0.04 μm

Sheet conductivity versus thickness

0

100

200

300

400

500

600

0 5 10 15 20 25

Thickness t (um)1

/R

Properties: Resistivity

R0

ρforest ~ 4 Ω cm

ρpoly-Si alone ~ 10000 Ω m

Resistivity of Si-coated forests

0

0.01

0.02

0.03

0.04

0.05

0.06

0.07

0.08

0 5 10 15 20

Thickness (μm)R

esis

tivi

ty (

Ω m

)

Properties: Resistivity

R0

ρforest ~ 4 Ω-cm

Resistivity of Si-coated (blue)and SiN-coated (red) forests

0

0.01

0.02

0.03

0.04

0.05

0.06

0.07

0.08

0 5 10 15 20

Thickness (μm)R

esis

tivi

ty (

Ω m

)

Approximately the same resistivity as previously reported for other CNT-composites

Microstructure: Poly-Si

0.2 µm

Between tubes, dark field

Properties: Poly-Si

0.2 µm Si S

ubst

rate

Alum

ina

laye

r

Iron

Between tubes, dark field

Properties: Poly-Si

0.2 µm

Between tubes, dark field

Mechanical Characterization

Filled forests are solid and well adhered (can withstand the scotch tape test)

Beam Bending Measurement of Elastic Modulus

20um

1000um

38um

Young's Modulus of organ pipe vs deflection of end of singly clamped beam

000E+0

50E+9

100E+9

150E+9

200E+9

250E+9

000E+0 20E-6 40E-6 60E-6 80E-6 100E-6 120E-6

u'_op (m)

E'_

op

(P

a) Organ Pipe #1

Organ Pipe #2

Organ Pipe #2

Eop = 120 GPa

Reported bulk polySi modulus ~ 140-210 GPa, dependent on deposition conditions

Actuated device: thermomechanical in-plane microactuator (TIM)

Developing Engineering Design Rules

Height to width ratio for dimensional stability

Maximum feature width for filling of forest interior

Role of geometry LPCVD fill-factor

Researchers

BYU Physics • David Hutchison• Brendan Turner• Katherine Hurd• Matthew Carter• Nick Morrill • Dr. Richard Vanfleet

BYU Mechanical Engineering • Quentin Aten• Dr. Brian Jensen• Dr. Larry Howell

Nanocarbon Research Center

AIST Japan Dr. Kenji Hata

Funded by a Brigham Young University Environment for Undergraduate Mentoring Grant

Partial funding provided by Moxtek Inc.

High Aspect Ratio Micromachining

“High-aspect-ratio bulk micromachining of titanium,” Aimi et al., Nature Mat. 3, 103-5 (2004)

MARIO Process (Titanium)Deep Reactive Ion Etching (Si)

“C-MEMS for the Manufacture of 3D Microbatteries,” Wang et al., Electrochem.

Solid-State Lett. 7 (11) A435-8 (2004)

LIGA process (photoresist)SU-8 / C-MEMS (photoresist / carbon)

“Micromechanisms,” H. Guckel, Phil. Trans. R. Soc. Lond. 353, 355-66 (1995)

“Vertical Mirrors Fabricated by DRIE for Fiber-Optic Switching Applications,” C. Marx et al., J. MEMS 6, 277, (1997)

VACNT Growth Studies

Objective: Dimensional Control Stable uniform features Smooth straight sidewalls and top surface Minimum void dimension

Variables: Barrier layer material Fe catalyst thickness

Barrier layer study:

Al2O3 – 30 nm

Native - SiO2

Thermally grown SiO2 – 30 nmTitanium – 30 nm

Early growth 2 sec. of C2H4 flow

Barrier Layer Study

TEM analysis of barrier layers

Both oxides form barrier to Fe diffusion, Al2O3 results in smallest particles

Quantitative particle size analysis of barrier layers

Alumina

0%

5%

10%

15%

20%

25%

30%

35%

40%

1.5 4.5 7.5 10.5 13.5 16.5 19.5 22.5 25.5 28.5 31.5 34.5 37.5 40.5 43.5

Particle size (nm)

Native Si Oxide

0%

5%

10%

15%

20%

25%

30%

35%

40%

1.5 4.5 7.5 10.5 13.5 16.5 19.5 22.5 25.5 28.5 31.5 34.5 37.5 40.5 43.5

Particle size (nm)

Thermal Si Oxide

0%

5%

10%

15%

20%

25%

30%

35%

40%

1.5 4.5 7.5 10.5 13.5 16.5 19.5 22.5 25.5 28.5 31.5 34.5 37.5 40.5 43.5

Particle size (nm)

Titanium

0%

5%

10%

15%

20%

25%

30%

35%

40%

1.5 4.5 7.5 10.5 13.5 16.5 19.5 22.5 25.5 28.5 31.5 34.5 37.5 40.5 43.5

Particle size (nm)

Alumina has far more of the smallest particles.

Effects of Al2O3 barrier layer

Reduce Fe loss through diffusion

Controls Fe particle size during annealReduces CNT diameter Increases CNT density and growth rateIndicates reduces Fe surface diffusion

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