zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA Baratunde Cola - - PowerPoint PPT Presentation

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zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA Baratunde Cola - - PowerPoint PPT Presentation

Some of our work zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA Baratunde Cola Heat Lab (heat.gatech.edu) NanoEngineered Systems and Transport (NEST) Lab George W. Woodruff School of Mechanical Engineering School of Materials Science and


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zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA

Some of our work

Baratunde Cola

Heat Lab (heat.gatech.edu) NanoEngineered Systems and Transport (NEST) Lab George W. Woodruff School of Mechanical Engineering School of Materials Science and Engineering Institute for Electronics and Nanotechnology Georgia Institute of Technology

Sponsors: DARPA, NSF, Georgia Research Alliance, Samsung Students: P. Pour Shahid Saeed Abadi, T.L. Bougher, J. Taphouse, V. Singh, M.K. Smith

10 May 2017 National Science Board Meeting

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For private discussions only. Company proprietary and confidential

Carbon nanotubes (CNT)

Technology - Highlights

  • High thermal conductivity
  • Billions of aligned nanoscale thermal paths
  • Demonstrated >30% improvement over

alternative solutions

Aluminum foil (layer) Carbon nanotubes (CNT)

20 μm

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Real interface ‘Ideal’ interface Solid 1 Solid 2 Gas gap Solid 2 k → ∞ Solid 1 Filler material

Characteristics desired for thermal interface materials

  • High thermal conductivity
  • High conformability
  • Chemically and mechanically robust in diverse

environments

  • Major challenge: soft materials with high thermal

conductivity are rare in nature

Slide 3 Bara Cola 5/8/2017

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zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA 10 µm

Resolving CNT Interfaces: One-Sided

  • Resolution enabled by photoacoustic thermal measurement

B.A. Cola et al., J. Appl. Phys. 101, 054313 (2007)

copper copper silicon silicon Ag

10 µm

Si

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B.A. Cola et al., ASME S

ng Desi Gold coated CNTs Wax coated CNTs

5 µm

ummer Heat Transfer Conference 2008

  • R. Cross et al., Nanotechnology, (2010)

Sprayed on Polymer Bondi gner Surface Modifiers

EtO P OEt Si Br , rt EtO i) 130 °C ii) MeOH: H2O (20:1), rt I EtO P O HO P O OEt OH

J.H. Taphouse et al., Advanced Functional Materials, 2014 Collaboration with organic chemist Dr. Seth Marder (GT)

Growth substrate Bonding substrate

J.H. Taphouse et al., Nanotechnology, 24:105401, 2013

~100% resistance reductions with each approach, but reliability and scalability continues to improve

Slide 5 Bara Cola 5/8/2017

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CORPORATION

Funding to date: >$2 million grants $1.4 million in angel and VC funds

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zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA

PRO TO Y PE SC A LE RE S E A RC H

First Thermally Conductive Amorphous Polymer

  • V. Sing h, e t a l. Nat Nano te c no l (5), 2014
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DVR BOX CE L L PHONE T CPo ly Pla stic Sta nda rd Pla stic Ma x: 48°C Ma x: 74°C L E D BUL B

PLA STIC S FO R C O O LER ELEC TRO NIC S

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Rectifying Antenna or ‘Rectenna’

Microwave rectenna Solar rectenna (born 1963, Raytheon and Purdue) (proposed 1972) Demonstrated efficiencies > 80% Predicted efficiencies > 80%

Slide 9 Bara Cola 5/8/2017

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Rectification Physics (Classical)

Cutoff frequency Diode resistance

Diode Junction

e

  • V

t V t

Diode responsivity

Antenna

EM field

Rectenna voltage and power output

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MWCNT Rectenna: Structural Detail

10 nm 100 nm Al2O 3 c oate d CNT s T

  • p me tal

1 µm

  • 8 nm conformal alumina coating
  • CNT tip field enhancement
  • ~ 10 nm junction diameter (C~1 aF)
  • Ca/Al low work function top contact

(semi-transparent, ~10% transmission) ~ 6 CNT walls

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How the Tunneling Diode Works

e-

MWCNT tunneling diode ~ 5 ev MWCNT work function

φCNT

φM’

E

F

E

F

Afte r c o nta c t F E e -

φCNT

E

F

φM’

E

F

F

  • rwa rd b ia s

φM’ φCNT

e

  • E

F

E

F

Re ve rse b ia s

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2.9 ev WF 4.3 ev WF

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Device Capacitance

Length and time scale for rectification cutoff frequency is different from length and time scale of device operation!

Fermi velocity < 106 m/s, so R( t≈10-15 s) = ∞ R(t) R(t)

Slide 13 Bara Cola 5/8/2017

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Impedance Matching

Poor impedance matching in a single junction is compensated by larger number of junctions, which allows power production. Collective antenna effects reduce coupling resistance to single CNT antenna.

R(t) R(t) Collective CNT antenna array – approximately in phase

  • Phys. Rev. B 87, 161401(R), 2013

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Rectification Photoresponse

Predicted physics

  • J. Phys. D: Appl. Phys. 46 (2013) 135106

Slide 15 Bara Cola 5/8/2017