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1 Introduction to Terahertz The ins and outs of terahertz technologies, what it does and how it works Richard Dudley, Mira Naftaly National Physical Laboratory Teddington, UK [email protected] Aim: Introduce the history of terahertz science Understand what terahertz waves are, how they interact with matter, how they are generated, detected and manipulated. Look at common measurement systems and discuss what can and can’t be measurement. Please do ask questions and interrupt !

Introduction to Terahertz - National Physical · PDF file1 Introduction to Terahertz The ins and outs of terahertz technologies, what it does and how it works Richard Dudley, Mira

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1

Introduction to Terahertz

The ins and outs of terahertz technologies, what it

does and how it works

Richard Dudley, Mira Naftaly

National Physical Laboratory

Teddington, UK

[email protected]

Aim:

• Introduce the history of terahertz science

• Understand what terahertz waves are, how they

interact with matter, how they are generated, detected and manipulated.

• Look at common measurement systems and discuss what can and can’t be measurement.

Please do ask questions and interrupt !

2

What are you terahertz experiences ?

Outline

• What is terahertz (THz)

• Recent History

• How can we use terahertz waves ?

• Terahertz Components• Sources

• Detectors

• Other

• Measurement systems• Spectrometers

• Solid, liquid & gas measurement.

• Terahertz Measurements

3

The Electromagnetic Spectrum

• Terahertz EM RADIATION / Rays / Waves ?

• 1012 Hz = 300 µm = 33 cm-1 = 4 meV = 50 Kelvin

• Room temperature objects = 6 THz

• Half the Cosmic background from Big Bang is THz

• Terahertz Gap ?

Terahertz Gap ?

• Terahertz has always been here !• “Heat Rays of Great Wavelength”, H. Rubens & E. F.

Nichols, Phys. Rev. 4, 314 (1897)

• Generating terahertz has just been difficult.• “Short Electric Waves”, E. F. Nichols and J. D. Tear,

Physical Review21, 587 (1923) – spark gaps

• Townes† attributes some of his motivation for

creating a maser (leading to the laser) was to

create a ‘molecular generator’ for the terahertz

band. (1957)

† Townes, How the laser happened, Oxford Uni Press, 1999.

4

How can we use terahertz waves ?

Just like any other EM wave !

How can we use terahertz waves ?

• Spectroscopy / Absorption Spectra

• Organic molecules exhibit strong absorption from GHz to THz

through rotational and vibration transitions providing fingerprints

in the THz band.

• THz material ‘signatures’

• The crystalline or physical structure of materials provides further

terahertz absorptions.

K.Wayne THz OutTHz INMaterial Under Test

freq freq

5

Terahertz Spectrum

• Atmospheric Water Absorption

0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.5

0

2

1.415

1.230

1.208

1.166

1.096

1.113

0.989

0.558

Absorp

tion (

Arb

.)

Frequency (THz)

0.753

Raw THz Absorption Spectra

How can we use terahertz waves ?

• Communications

• High data rate but line of sight

• Current wireless communication systems utilise carrier waves

less than 5 GHz which restrict their maximum data rate, 100’s

Mbit/s typically.

• Higher frequency carriers enable high data rates and therefore

1000’s Gbit/s dates rates are on offer with terahertz carrier

waves.

NTT

6

How can we use terahertz waves ?

• To see through objects or layers.• Terahertz waves can penetrate through materials

opaque to other parts of the EM spectrum.

• Many non-metallic or non-polar materials are transparent to terahertz to some degree

• Many plastics, glasses, woods, cardboards, earth/soil,

fabric, ceramics are transparent to some degree.

• Hidden or buried layers can be observed in structures containing layers, packaging or clothing.

• Use in non-destructive testing (NDT)

A few terahertz limitations.

• Penetration depth into material• Penetration is limited in high-water content or metal objects.

• Most materials have terahertz attenuation and thus a finite thickness before they become opaque.

• Terahertz cannot travel large distances in earth atmosphere free space• Greater distances are possible in space.

• Terahertz cannot be focused to spot sizes below 100 µµµµm (diffraction limit) unlike optical waves• Near field techniques can get round the limit.

7

A few terahertz limitations.

• Spectral Features

• Terahertz is often sold as a mass spectrometer type

instrument, able to identify complex chemical substances

just by spectral absorption feature.

• Often terahertz reveals more information about the chemical-

structure rather than the chemical make up of a test sample.

• The quality of any features deteriorates as you move from

gas to liquid to solid.

• Solutions and mixtures can create very difficult to interpret

absorption spectra.

Terahertz Components

Sources, detectors and everything else…

8

Terahertz Sources

• I like to categories sources into • Single frequency (c.w)

• Single frequency but tuneable

• Broadband or pulsed • Thermal

• Lamps/Black Bodies

• Electrical

• Gunn Diodes/Mixers

• Backward Wave Oscillators

• Optical / Laser Based

• CO2 Pumped Gas Laser

• Optical Parametric Oscillator

• Hetrodyne C.W Photo-mixing

• Terahertz Pulse Methods

Source Examples

The selected source will depend on your

application/measurement and possible power

requirement.

Terahertz Sources

Free Electron Laser (FEL)

• An ideal THz source: high power, large bandwidth, coherent

• But not portable!

p-Germanium laser

• 10-100 µW power.

• 1.5-5 THz tuning range

• A large cryogenic installation requiring a superconducting

magnet

ELRP, UK

Two of the more difficult sources to operate.

9

Terahertz Sources

CO2 Pumped Molecular Laser

• Narrow line width.

• Tuneable !

CO2 Difference Frequency Mixing

• Mix two stabilised CO2 with rf source.

• Appl. Phys. Lett. 44 576 (1984)

• 100 kHz resolution

• Needs careful stabilisation circuits

100 W @ 10um

CO2 Laser

FAR-IR Laser

Two high power options but difficult to operate and tune.

Terahertz Sources

Quantum Cascade Laser (QCLs)• Complex structures enable

population inversion

• High output powers, c.w operation

• Low temperature operation

• From 2 THz up, narrow line

• Not tuneable

R. Köhler et al., Nature417, 156 (2002)

TheEconomist,August 10th, 73 (2002)

Gunn & TUNNETT diodes• High power but limited frequencies

available and banded devices

• Multiplier can help extend band

• Heat and output power is a problem

Semiconductor, electrical devices are attractive but not fully developed for practical use fully as yet..

H. Eisele, University of Leeds

10

Terahertz Sources

Backward-wave oscillators• A vacuum tube that is used to

generate microwaves up to the

terahertz range.

• Some tuning, but limited in range

• High power output possible

• High voltages required and some operational difficulties.

AB Millimetre System

Terahertz Sources

Difference frequency generation

• Use two lasers, c.w or pulsed.

• Mix lasers optical beating in a non-linear material/device such as

• Photoconductir, GaP, GaSe, DAST

• Adjusting laser properties allows

tuning of terahertz frequencies generated

Optical Rectification

Probably, most commonly used method to generate 0.1 to 5 THz

• First observed by Austen et al, with

femtosecond optical pulses in an electro-optic material.

• Phys. Rev. Lett. Vol.53 p.1555 (1984)

• Basically required the illumination of a crystal or semiconductor with a very short optical laser pulse (sub-picosecond)

• Creates a terahertz pulse corresponding to the optical pulse.

11

Terahertz Optical Rectification

+-+-

+--

+

-

+

-

+

-

+

-

+

-

+Laser

SemiconductorBattery

- +Ultrafast Laser System

Terahertz Optical Rectification

0 2 0 4 0 6 0 8 0 1 0 0 1 2 0

- 0 . 0 0 5

- 0 . 0 0 4

- 0 . 0 0 3

- 0 . 0 0 2

- 0 . 0 0 1

0 . 0 0 0

0 . 0 0 1

0 . 0 0 2

0 . 0 0 3

0 . 0 0 4

0 1 2 3 4

0 . 0 0 0 0 1

0 . 0 0 0 0 2

0 . 0 0 0 0 3

0 . 0 0 0 0 4

0 . 0 0 0 0 5

f r e q u e n c y , T H z

t i m e , p s

F e m t o L a s e r

2 m i r r o r s y s t e m

Z n T e 1 / 1 m m , F S

5 N o v 2 0 0 4

• Example terahertz pulse created by optical

rectificationTHz Pulse generated by rectification

Fourier Transform of pulse gives frequency content

12

Ultra-broadband Optical Rectification

Terahertz Detectors

• Thermal

• Golay Cell

• Bolometer

• Pyroelectric device

• Electrical

• Photo-acoustic

• Diode

• Optical / Laser Based

• Terahertz Pulse Methods

Detectors

• Detector development lags source development !

13

Terahertz Detectors

Bolometer• Thermal device

• Frequency insensitive

• Operates at 4 Kelvin (close to -270 Centigrade)

• Excellent sensitivity

Golay Cell• Thermal device.

• Room temperature operation

• Vibration sensitive

• Easily damaged

• Ageing and linearity issues

Terahertz Detectors

Photo-acoustic

• A closed air-cell and a pressure transducer detects terahertz.

• Calibration can be provided byohmic heating of a thin metal film within the cell

• Good sensitivity, robust and easy to operate.

Pyroelectric

• Thermal detection converted into electrical signal.

• Limited sensitivity but easy to use.

14

Electro-Optic (EO) Detection

• Normally a pump-probe method and requires the laser pulse used in optical rectification generation to sample the detect the signal.

• Terahertz co-propagates with optical beam through a non-linear crystal and encodes a polarisation change on the optical beam proportional to the terahertz field strength

• Excelent bandwidth and sensitivity

• Appl. Phys. Lett. 67, 3523 (1995) & Appl. Phys. Lett. 71, 1285 (1997)

EO- Detection part

Detector Linearity

0 1 2 3 4 5 6 7 8 9 10

1E-4

1E-3

0.01

0.1

1

slope = 0.7

Spe

ctr

al a

mplit

ud

e (

a.u

.)

Number of plates

0.2 THz

0.5 THz

1.0 THz

1.5 THz

2.0 THz

2.5 THz

3.0 THz

slope = 0.7

0 1 2 3 4 5 6 7 8 9

1E-6

1E-5

1E-4

1E-3

Am

plitu

de (

a.u

.)

Number of plates

Frequency

(THz)

0.25

0.5

1.0

1.5

2.0

2.5

3.0

-1 0 1 2 3 4 5 6 7 8 9 10 11

0.01

0.1

1

Slope = 0.78

High power

Low power

Linear fit

Gola

y s

ign

al (V

)

Number of plates

Slope = 0.82

Golay • Not linear

• Behaviour differs at high and low powers

• Probable explanation: membrane has been over-stretched and lost elasticity

TDS System Linearity

TDS 1

TDS 2

NPL

LinCal

Kit

15

Other terahertz components

Optics, waveguides and materials….

Some Important Materials

• Silicon & the plastics PTFE, HDPE and TPX are key terahertz materials

• They exhibit low loss and dispersion over the 0.1 to 5 THz band.

• If you need to make

• Lenses

• beam splitters

• Windows

• sample holders etc…..

• You will probably need to use these materials to design it.

16

Free Space Optics

• Mirrors• Metal plane and curved can be used.

• Parabolic mirrors most commonly used to enable terahertz beam manipulation (focus, steering, collimating..)

• Lenses• Designs as with optics but silicon and plastic being

most common materials rather than glass.

• Polarising• Wire grids

• Filters• Metal grids

• Modulators• Phase modulation with wire grids

• Chopper type low frequency modulation.

Terahertz Waveguides

• Coax / Copper wire becomes too small and very high loss

above a few 100 GHz.

• Metallic waveguides can be used to many THz but become small, expensive and narrow band (typically only covering 100 GHz per physical structure).

• Metal and Polymer Wires have shown some promise

• Nature 432, 376-379 (18 November 2004)

• Surface modes so not tolerant of bending or being enclosed

THz Wire Waveguide

Metallic Waveguide

17

Terahertz Waveguides

• Dielectric Waveguide and Photonic Crystal Fibres are possible future directions• Fibres like optical containing mainly vacuum have shown promise

by having guiding abilities but with low loss.

• Coupling terahertz into the devices can be challenging

• Has potential to be used as a sensor too for long interaction lengths or flows.

• Appl. Phys. Lett. 80, 2634 (2002)

Terahertz Planar Waveguides

• Small metal lines are placed on a low loss material

called the substrate

• Terahertz waves can propagate over tens of millimetres.

• Coupling is very challenging and is generally done on/in

the substrate.

• Can also be used as an on chip test module.

GaAs

18

Terahertz Measurement Systems

Source, detectors and optics selection for some measurement examples

Single Frequency Systems

• Imaging

• For x-ray type operation to reveal hidden structures

• CO2, Diodes or QCL good options as sources.

• Bolometer or Golay cell easy options but not ideal due to robustness or operational difficulties.

• Communications

• Industry demands electrical, easy to operate devices.

• Diodes based devices are current favourites

• Detectors are not ideal and are either the same diodes or thermal devices which have limited bandwidth.

• Modulation is a problem.

19

Broadband systems

FT Spectrometer

• Fourier transform spectrometer is a Michelson interferometer with a movable mirror and sample under test placed in one arm.

• Thermal source and golay or bolometer detection.

• Poor dynamic range below 10 THz.

Planar Circuits

• Optical rectification and EO detection

http://www.brucherseifer.com/html/dna_analysis.html

NPL DFTS

Broadband systems

Near-field systems

• Use metal tips to concentrate terahertz energy to nano-meter regions.

• Often uses optical rectification and EO detection but limited dynamic range

Time Domain Spectrometer• Has become the instrument/technique

of choice for the majority of terahertz spectroscopy and NDT applications.

• NPL Instrument

• Optical rectification and EO detection

• 10,000 dynamic range possible many sample measurement configurations.

20

Time Domain Spectrometer (TDS)

TDS - System

21

TDS – Delay Line

TDS Emitter

22

TDS EO Detector

TDS Measurement Space

Emitter Detector

23

Time Domain Spectrometer

• Parabolic metal mirrors, TPX lenses, lock-in techniques.

• Measurement systems built using the new method of

generation and detection to create systems with better

dynamic range than previously possible.

• Resolution can be issue.

Making Terahertz Spectroscopic Measurements

Higher frequency resolution requires longer acquisition time – few minutes to an hour is possible

for a single measurement

24

Measurement of Gas Samples

• Typically requires long interaction lengths to get good absorption, a

parallel beam is best here.

• Gas cell needed with transparent windows.

• Produces narrow line spectral features with few distortions or

errors, thus long delay lines scans for high resolution required.

• Knowledge of gas pressure and cell length for absorption

information.

0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.5

0

2

1.415

1.2301.208

1.166

1.096

1.113

0.989

0.558

Ab

so

rptio

n (

Arb

.)

Frequency (THz)

0.753

Measurement of Solid/Liquid Samples

Solid

• Spectra may show some features but not sharp as with gases.

• Ideally placement in collimated beam, but often done in focused beam region.

• Care must be taken to avoid internal pulse reflections within the sample.

• Pellets made from sample and PTFE powder can be made to aid measurement.

Liquid

• Spectra are often lacking in features and just show a general attenuation over

the band.

• Losses in water rich samples generally high so a thin cell is required.

• Techniques such as Attenuated Total Reflection can be used to measure

water samples but analysis is difficult.

25

Non-Destructive Testing

• Send terahertz pulse into a

multilayer structure and reflections will occur from each boundary.

• Timing the delay of each

reflection can revel its thickness / refractive index.

• TDS systems are universally used for this type of application.

• See Teraview presentation

Dynamic Range

• A key parameter for any measurement system which will

define if you can undertake a measurement or not.

M Naftaly, R A Dudley, Linearity calibration of amplitude and power measurements in terahertz systems and detectors, Opt. Lett., Vol. 34 (5), 2009, pp. 674-676.

26

Quantitative Terahertz Measurements

• Most terahertz measurements are made using

arbitrary units for the vertical scale.

• Absorption measurements are rarely quantitatively

and only comparable with the measured reference.

• Calibration of terahertz measurement systems is

rare even for basic parameters such as power,

frequency, linearity, spatial resolution ….

• Care must therefore be taken when comparing

data between measurement systems.

A few commercial measurement system examples

27

Teraview System

• Time-domain spectrometers

• Many configurations and

options available for

spectrometers, imagers and

testing.

Picometrix T-Ray

• Time-domain spectrometers

28

Thruvision

• Passive security imaging camera

Applications

• Historically Terahertz applications were dominated by,

• Astronomy

• Remote Sensing

• High energy experiments

• Terahertz Instrumentation has created applications in,

• Material Testing

• Medical Imaging

• Dentistry

• Drug Detection

• Security Scanning (People and Baggage)

• Non-destructive testing

• Communications