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Electronically Tunable Terahertz Electronically Tunable Terahertz - - PowerPoint PPT Presentation

Electronically Tunable Terahertz Electronically Tunable Terahertz Detector Using Plasmons Plasmons Detector Using Jess Crossno Physics Santa Barbara City College Mentor: Greg Dyer Research Advisor: Dr. Jim Allen Undergraduate Researchers:


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Electronically Tunable Terahertz Electronically Tunable Terahertz Detector Using Detector Using Plasmons Plasmons

Jess Crossno Physics Santa Barbara City College Mentor: Greg Dyer Research Advisor: Dr. Jim Allen Undergraduate Researchers: Sean Haney, Bill Sowerwine

In Partnership with:

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SLIDE 2

Why the need for THz research? Why the need for THz research?

Technology Gap: Gap between Electronics and Photonics. Electronics fail to produce adequate power above several hundred GHz Photonics fail to produce adequate power below several THz

*THz = Terahertz = 1 Trillion Cycles per second

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SLIDE 3

Current technology

  • perates at ~1-10GHz
  • r ~1-10 billion bits per

second Terahertz frequencies

  • perate at ~1-10 THz
  • r ~1-10 trillion bits per

second

THz Applications THz Applications

Technology applications Information Ultra fast signal processing Massive data transmission Environment Atmospheric sensing Defense Chemical/Biological agent

detection

Digital radar Imaging Covert communication Space-space Short range battle field Unknown applications created

by new technology

Millimeter-wave radar images taken 9 km from a nuclear power plant can detect when the plant is

  • perating (upper image)
  • r idling (lower image).

http:// http://www.thznetwork.org www.thznetwork.org

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SLIDE 4

Final Goals

Goals:

Research and develop terahertz electronics

(300 GHz – 10 THz)

Objectives:

Nanoelectronics for THz sources and detectors. Detectors Tunable detectors for THz using plasmonic

resonance

Sources THz Bloch oscillator.

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SLIDE 5

Resonant Frequency

2 p

f n ∝

Plasmon frequency dependence

Electron Density

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SLIDE 6

Resonant Frequency

2 p

f n ∝

Plasmon frequency dependence

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SLIDE 7

The Split The Split-

  • Grating Gate Detector

Grating Gate Detector

Source Drain Grating gates Finger Gate AlGaAs GaAs Source Drain Grating gates Finger Gate

4uM 4uM | |----

  • ---|

|

1mm

FET

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SLIDE 8

Future Work

Continue to chart device’s behavior Determine optimized settings:

Source/Drain Current Wiring Temperature Frequency Range

Implement device into applications

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SLIDE 9

Acknowledgments

  • The Allen Group:
  • Dr. Jim Allen
  • Greg Dyer
  • Dr. Thomas Feil
  • Dr. Alex Kozhanov
  • Sean Haney
  • Bill Sowerwine
  • Sandia National Labs:
  • Dr. Eric Shaner
  • Dr. Mark Lee
  • Dr. Mike Wanke
  • Dr. John Reno
  • INSET:
  • Samantha Freeman
  • Dr. Nick Arnold
  • Liu-Yen Kramer
  • Luke Bawazer
  • Dr. Evelyn Hu
  • CUNY:
  • Greg Aizin
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SLIDE 10

Extra slides Extra slides

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SLIDE 11

Current Research Current Research

  • 8 .0 µ
  • 6 .0 µ
  • 4 .0 µ
  • 2 .0 µ

0 .0 2 .0 µ 4 .0 µ 6 .0 µ 8 .0 µ 1 0 .0 µ

  • 0 .0 3 0
  • 0 .0 2 5
  • 0 .0 2 0
  • 0 .0 1 5
  • 0 .0 1 0
  • 0 .0 0 5

0 .0 0 0 0 .0 0 5

V o lta g e R e sp o n s e G a te V o lta g e -5 0 0 m V C u rre n t 1 0 u A Voltage (V) T im e b a se (s)

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SLIDE 12
  • 70
  • 60
  • 50
  • 40
  • 30
  • 20
  • 10

10 20

  • 0.8
  • 0.6
  • 0.4
  • 0.2

0.0 0.2 0.4 1E-6 1E-5 1E-4

Signal response and relax tim e vs current Vg: -500 m V, 20 K

Signal Response (Unitless) Current (uA) Relaxation time (s)

Current Research Current Research

FEL .48 THz FEL .48 THz

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SLIDE 13

Wiring Diagram for Split Wiring Diagram for Split-

  • Grating Gate

Grating Gate Detector Detector

Polarization

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SLIDE 14

S D

Diagram

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SLIDE 15

0.6 THz image

Can see through visibly

  • paque objects

THz has no or minimal health risk Can use passive detection (QinetiQ, UK, US)

Why Image in THZ? Why Image in THZ?

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