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R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 [email protected] 18 July 2008

R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 [email protected]

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Page 1: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

R. Barry Johnson, D.Sc.Research Professor

Physics Department (A-145)Alabama A&M University

P.O. Box 1268Normal, Alabama 35762

[email protected]

18 July 2008

Page 2: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Terahertz Detectors

• Bolometers– Conventional– Electrostatic– Golay

• Pyroelectric

• Diodes

Page 3: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

vis

ibleRadio wave

X-raysUVmicrowaves Infrared

0.01 0.1 1 10 100

1 10 100 1000

frequency / THz

wavenumber / cm -1

Low frequency bond vibrations

Hydrogen-bonding stretches and torsions (liquids)

Crystalline phonon Vibrations (solid)

Molecular rotations (gas)

NIR

Terahertz Spectral Region0.06 – 10 THz ; 2 – 300 cm-1; 5000-30 μm

Typical Range: 300 GHz - 3 THz; 1000-100 μm

Page 4: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Bolometer

• Samuel Langley invented the bolometer in 1878.• Any radiation absorbed by the bolometer raises

its temperature above that of its heat sink. Temperature change causes a change in some parameter, such as device resistance, that can be measured directly or indirectly.

• Often used in a Wheatstone configuration with a “hot” and a “cold” detector.

• Can be made very sensitive, but have low frequency response.

• Used from mm-wave to beyond visible light.

Page 5: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Principle of Bolometer

Page 6: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Electrostatic Bolometer

• Broad spectral coverage.• MEMS structure, which allows arrays to be easy

fabricated.• Cantilevered configuration electrostatically

charged.• Incident flux converted to heat which then

discharges the electrostatic charge on the device.

• Good sensitivity and modest speed possible.

Page 7: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Cryogenically Cooled Bolometer

The cryogenically cooled silicon bolometers offer excellent signal to noise ratio and nearly flat response for THz wavelengths from15 µm to 2 mm.

RadiaBeam Technologies BLIS-03-BLM

Page 8: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Silicon Bolometer

Page 9: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Golay Cell Detector

• A Golay Cell is a room temperature bolometer, which is a convenient choice for the moderate to high intensity THz signal measurements.

• Cell is a metal cylinder having a blackened metal plate at one end and a flexible metalized diaphragm at the other. It is filled with an inert gas and then sealed. Radiation incident upon the blackened metal plate is absorbed and heats the gas which increases the pressure thereby deforming the deforms the diaphragm.

• Light is reflected by the diaphragm motion onto a detector to measure the incident flux.

• Wide spectral range of 0.02-20 THz

RadiaBeam Technologies BLIS-03-GYCand

Microtech Instruments, Inc.

Page 10: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Pyroelectric Detector

• Convert the changes in incoming flux to electric signals.

• Pyroelectric materials are characterized by having spontaneous electric polarization, which is altered by temporal temperature changes( ) when irradiated by flux.

• High sensitivity, • Room temperature operation• Low cost• Robust under severe environmental conditions• Suffers from microphonics (minimal for SBN)

/T t

Page 11: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

LiTaO3 Pyroelectric Detector • Large area to 9 mm diameter • Broad spectral response 0.1 to 1000 µm • Current and Voltage hybrid circuits • NEP 3x10-10 W/(Hz)1/2 • High bandwidth to 20 MHz • High voltage output, 50KV/W

Spectrum Detector Inc.

Page 12: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Superconducting Hot Electron Bolometer

• Operates at superconducting transition region.

• Small temperature change yields large change in device resistance.

Page 13: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

B-field Tuned InSb Detectors • Magnetic Resonance Enhanced

Indium Antimonide (InSb) Hot Electron Bolometer Type QFI/XB

• Fast and sensitive detection from below 100 GHz to 3 THz

• In the type QFI/XB device, the detector is mounted within a quasi-uniform magnetic field geometry so that magnetic resonance effects can be used to enhance free carrier absorptivity at much higher frequencies.

• Speed: Approx. 1MHz (-3dB) at 4.2K.

• Detector Optical N.E.P is below1 x 10-12 W Hz-1/2

QMC Instruments Ltd

Page 14: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Zero-Bias GaAs SchottkyDiode Detectors

“Responsivity and Noise Measurements of Zero-Bias Schottky Diode Detectors” http://www.virginiadiodes.com/VDI/pdf/VDI%20Detector%20Char%20ISSTT2007.pdf

Page 15: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

THz Source

J. Hesler, D. Porterfield, W. Bishop, T. Crowe, A. Baryshev, R. Hesper and J. Baselmans, "Development and Characterization of an Easy-to-Use THz Source", Proc. 16th Intl. Symposium on Space Terahertz Technology, May, 2005, Goteborg, Sweden. http://www.virginiadiodes.com/VDI/pdf/Hesler%202005%20stt%20thz%20source%20and%20measurements.pdf

Page 16: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Applications of THz Sensors

• Pharmaceutical

• Medical

• Industrial

• Security

Page 17: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Terahertz Spectral RegionMolecular Vibrations

Terahertz Spectral Region

• Intermolecular bond vibrations

• Directly affected by crystal changes

Infrared Spectral Region

• Intramolecular bond vibrations

• Indirectly affected by crystal changes

Page 18: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

THz Pulsed Imaging Basics

• THz Pulsed Imaging– Time-of-flight analysis– Production of spectral

information

• Refractive index discontinuities reflect back a part of the incident pulse

• Imaging– Depth profiling using

multiple detected pulses– 3D image created by raster

scanning

Page 19: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

TeraView Ltd. Terahertz Pulsed Imaging and Spectroscopy

Page 20: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Photoconductive THz Generator

Zhang, J.; Hong, Y.; Braunstein, S.L.; Shore, K.A., “Terahertz pulse generation and detection with LT-GaAs photoconductive antenna,” Optoelectronics, IEE Proceedings, Vol. 151, Issue 2, 26 April 2004 (98 – 101). The characteristics of optically induced teraherz (THz) radiation from a biased low-temperature-grown GaAs (LT-GaAs) photoconductive antenna were investigated using a femtosecond Ti:sapphire laser.

Page 21: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Photoconductive THz Detection

J. Zhang et al., “Terahertz pulse generation and detection with LT-GaAs photoconductive antenna,” IEE Proceedings – Optoelectronics, April 2004, Vol.151, Issue 2, (98-101 ).

Page 22: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Applications of Terahertz Sensorsto Pharmaceutical Analysis

With Courtesy ofDr. Philip F TadayTeraView LimitedCambridge, UK

Page 23: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Pharmaceuticals

• Applications– Process improvement– Polymorph screening– Tablet Inspection

• Early stage of application

• Commercial instrumentation available

Page 24: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Consequences of Bad Coating Quality

• Unpredictable dosing rate• Dose dumping – life threatening• Legal and commercial implications

Page 25: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Coating Integrity Investigation using Terahertz Pulsed Imaging

Reflected Thz pulses probe coating structures.

Page 26: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Non-Destructive Mapping of Coating Thickness in Tablets

• Terahertz pulses reflect from each coating layer.

• Mapping of coating layers accomplished by time of flight and x-y scanning.

Page 27: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

TPI - Coating Layer Thickness

Page 28: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

16% w.g. enteric coating10% w.g. enteric coating

15% solids level

Enteric Coated Tablets

Page 29: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Single incidentTHz pulse

multiple return pulses Coated

tablet

Terahertz Pulsed ImagingPenetration through most pharmaceutical excipients.

Non-destructive coating analysis.Fully automated process.

Page 30: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Initial Setup for Measuring Water Ingress

HPMC tablet

10 l water

~900 microns

Time Delay (mm)

B-scan

y-d

ire

cti

on

(m

m)

-1 0 1 2 3

-6

-4

-2

0

2

4

6

-0.1

-0.05

0

0.05

Page 31: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

30 minutes

40 minutes 50 minutes 60 minutes

30 minutes

K4M – Change In Terahertz Image with Time After the Addition of Water

Page 32: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

TPI Tablet EvaluationTablet

Coating Structure

Comparison ofX-ray CT & TPIGood vs. Poor

Tablet Coatings

Page 33: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

THz Medical Imaging

• Applications– Skin cancer: basal cell

carcinoma– Aid for surgeon in

tissue typing– Endoscopy: prostrate

& other cancers

• In use for clinical trials

Page 34: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Non-Destructive Testing3D THz Imaging of IC Package

Page 35: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Security Applications

• Checkpoint screening of people to locate hidden weapons and explosives.

• Stand-off detection of explosives.

• Baggage screening for explosives.

• Screening for biological and chemical agents.

• Drug detection.

Page 36: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Issues RegardingTerahertz Technology for Security

• Signatures– Do threat materials have characteristic signatures?– Are they distinct from non-threat materials?

• Shielding/Barriers– Can terahertz flux penetrate clothing and other barriers?

• Mode– Can signature be detected in reflection?

• Performance– Can systems be used at distance up to 10 m?– Source power and detector sensitivity– Atmospheric absorption

• Practical Systems Achievable?

Page 37: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Terahertz Spectra of Explosives

• Energetic compounds and explosives

• Most features above 500 GHz.

• Barrier material absorption limits upper frequency to < 3 THz.

Kemp et al., Proc. SPIE 5070, 44 (2003)

Page 38: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Water Windows Correspond to Spectral Features of Explosives

Page 39: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Possible Confusion Materials

• Large data base of materials has been collected.

• No significant confusion found between explosives and harmless materials.

Tribe et al., Proc SPIE 5354, 168 (2004)

Page 40: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Clothing and Barrier Materials

• Clothing materials are partially transparent.

• Absorption increases with frequency.

• Useful frequency range limited to< 2-3 THz.

Tribe et al., Proc SPIE 5354, 168 (2004)

Page 41: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Detecting Materials Hidden Under Clothing

Page 42: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Terahertz Image of Shoe with Hidden Ceramic Knife & Plastic Explosive

Page 43: R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama 35762 256.372.8148 ralph.johnson@aamu.edu

Conclusions• Terahertz technology has made significant progress in recent years and is

being exploited for a variety of applications. • Instrumentation is becoming available commercially.• Components are available for various vendors. • Research continues to improve performance and lower cost of terahertz

components and systems.• Terahertz pulsed imaging and spectroscopy has been shown to be of use in

a number of key areas.– Understanding of the thermodynamics of polymorphic systems– Process understanding of complex coating structures– Techniques are fast enough to be used in environments where tablets have fast

random motions• Advances in medical applications have been demonstrated and expected to

be further exploited.• Industrial applications for examining a variety of products is expanding.• Terahertz systems have demonstrated definitive capability is addressing

important security applications. Initial deployment of screening systems in airports around the world.