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Tunable CW THz Source
Principles of Operation andApplication Data
Gregor KupkaJoachim Sacher
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Outline
CW THz Generation via Frequency Mixing of Tunable Diode Lasers Motivation
Selected Application Examples
Instrument Layout Principles of CW THz Generation Coherent CW THz Detection Method
Technical Data THz Generation
Frequency Mixers
Laser Sources Frequency Tuning Fast Frequency Scanning Frequency Stability
Laser Controller Electrical Noise Characterization Optical Noise Characterization Relative Intensity Noise
Software
Application Examples
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Motivation
Selected Application Examples Airport Screening for weapons
explosives, drugs or other contrabands
Secure wireless communication Cancer detection, wound
inspection and other medical imaging
Biochip analysis of DNA, proteins, and other biological materials
Biological warfare agents Detection of land mines and
buried explosive devices Monitoring manufacturing
processes Measuring water content of food
to detect spoilage Inspection finished production
through packaging
Determining the thickness of a layer of paint while it is still wet
Quality control of insulated wires during manufacture
Inspecting semiconductors wavers for defects
Inspecting (and reading) of unopend mail
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Principles of CW Tera Hertz Generation
Generation of Tunable CW Tera Hertz Radiation There are no room temperature operational CW THz radiation sources
Quantum cascade based developments still require a decade of development
Technical realization of CW THz radiation Difference frequency generation of two CW lasers
Schematic Layout of a CW Tera Hertz measurement setup
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Principles of CW Tera Hertz Generation
Higher Power Options for future THz Frequency Mixers Solutions with optical amplifiers
More than 300mW power for beat frequency generation available
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Coherent CW Tera Hertz Detection Method
Setting the THz Frequency via the Wavelength of the Pump Lasers The THz Frequency setting is performed via the temperature of the DFB
Lasers The THz Frequency may be verified via a Spectrometer
Changing the Phase between THz Sender and the THz Receiver The Phase is changed via the fiber-optical Delay line. Alternatively, a Phase change can be performed by the current of the DFB
Lasers
Phase Changes causes Interference Pattern within the Receiver The THz radiation of the Sender and the Receiver interfere within the
Receiver unit Absorption of THz Radiation within the Sample can be detected via the
Change of the Amplitude of the Interference Pattern
Lock-In Detection of the THz The Lock-In Detections allows the Measurement of the THz Absorption Improved Signal to Noise Ratio
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CW Tera Hertz Generation
CW THz Frequency Mixers Technology Requirements
Low carrier lifetime for high frequency THz radiation generation High carrier mobility for high intensity THz radiation generation
Fiber Coupled Design High coupling efficiency No alignment issues Easy to use
THz Beam Performance Precollimated THz beam
via Silicon Lens
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CW Tera Hertz Generation
Performance Data
Frequency Dependence:100GHz 1.5µW (spec.)500GHz 0.5µW (spec.)
1000GHz 0.1µW (spec.)1500GHz 0.05µW (spec.)
760 770 780 790 800
-50
-40
-30
-20
-10
0
Sidemode supression 39 dB
Sig
nal [
dBm
]
Wavelength [nm]
without Master Laser
with Master Laser
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Laser Souces for CW Tera Hertz Generation
Fiber Coupled Laser Solution for CW Tera Hertz Generation
Laser System Tuning Performance
DFB Wavelength Tuning
851,5
852,0
852,5
853,0
853,5
854,0
854,5
855,0
855,5
15 20 25 30 35 40 45 50
Temperature / °C
Wav
elen
gth
/ nm
Wavelength DFB 1
Wavelength DFB 2
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Laser Souces for CW Tera Hertz Generation
Fast THz Frequency Scanning Capability via DFB Temperature Scanning
0 20 40 6018
20
22
24
26
28
30
32
779,800
779,900
780,000
780,100
780,200
780,300
780,400
780,500
Periodic Temperatur Scan Setpoint Dither 20°C
Tem
pera
ture
/ °C
Time /sec
10sec periodic temperature scan
Wav
elen
gth
/nm
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Laser Souces for CW Tera Hertz Generation
Long Term Stability without external stabilization
Video
http://data.sacher-laser.com/video/mov01178-smaller.wmvhttp://data.sacher-laser.com/video/mov01178.mpg
Free Running Stability better than 50MHz
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Laser Controller for CW THz Generation
Experimental Setup
Sub 500nA Noise Figure
Reference Modulation
10 ResistorΩ
DC Current
Electrical Spectrum AnalyzerLaser Controller Bias-Tee
0,0 20,0k 40,0k 60,0k 80,0k 100,0k0,0
12,8
25,6
38,4
51,2
64,0
76,8
89,6
102,4PilotOEM 500, Battery operated
ES
A A
mpl
itude
/ dB
m
Frequency / Hz
500nA RMS
0,0 200,0k 400,0k 600,0k 800,0k 1,0M0,0
12,8
25,6
38,4
51,2
64,0
76,8
89,6
102,4 Pilot OEM 500, Battery operated
ES
A A
mpl
itude
/ d
Bm
Frequency / Hz
500nA RMS
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Laser Controller for CW THz Generation
Experimental Setup
Sub 700nA Noise Figure
Reference Modulation
Laser Diode
DC Current
Photo Diode
Laser Controller Bias-Tee
Electrical Spectrum Analyzer
-20k 0 20k 40k 60k 80k 100k 120k 140k 160k 180k-100-95-90-85-80-75-70-65-60-55-50-45-40-35-30-25-20-15-10
-50
7µA RMS Noise Level
Noi
se V
olta
ge /d
B
Frequency/ Hz
Optical Noise Measurement PilotOEM 500
0.7µA RMS Noise Level
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Laser Controller for CW THz Generation
Relative Intensity Noise Experimental Results in Cooperation with TU Darmstadt
Excellent Noise Figure of Sacher Laser Controller Noise Figure determines the Linewidth of DFB Lasers Controller defines Stability of THz Frequency
0 200 400 600 800 1000 1200 1400
-80
-75
-70
-65
-60
-55
-50
Other Manufacturer 24V Batterie Pilot OEM
Cur
rent
Noi
se (
dBm
)
Injection Current (mA)
0 10 20 30 40 50 60 70 80 90 100 110 120-170
-160
-150
-140
-130
-120
-110
RIN
(dB
/Hz)
Injection Current (mA)
24V Batterie Pilot OEM Other Manufacturer
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CW THz System Software
Complete Measurement Software
Programmed in LabView
Auto-Calibration of System Data
Calibration Data stored in Status File
Fully Automated Measurement Algorithmn Frequency Scan of Samples Phase Scan of Samples 2D Position Scanning of Samples
Flexible Storage of MeasurmentResults on Hard Drive
Programmstart
EingabemaskeProbe, Scanbereich
Eingabemaske Lasersystem
Auslesen / Ändern
Eingabemaske Lock-In VerstärkerAuslesen / Ändern
Probe X-Positionanfahren
Probe Y-Positionanfahren
THz Frequenzanfahren
PhasenscanStartposition
anfahren
Lock-In Verstärkerauslesen
Daten abspeichern
PhasenscanEndposition erreicht ?
THz ScanEndposition erreicht ?
Y-PositionEndpositionerreicht ?
X-PositionEndpositionerreicht ?
Programmende
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CW THz System Software
Selftest Procedure
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CW THz System Software
Frequency Calibration
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CW THz System Software
THz Tuning AlgorithmnTHz Tuning Algorithmn
15
20
25
30
35
40
45
50
0 5 10 15 20 25 30 35
Tuning Parameter
Lase
r Tem
pera
ture
/ °C
Temperature DFB 1
Temperature DFB 2
DFB Tuning
851,5
852,0
852,5
853,0
853,5
854,0
854,5
855,0
855,5
856,0
0 5 10 15 20 25 30 35
Tuning Parameter
Wav
elen
gth
/ nm
Wavelength DFB 1
Wavelength DFB 2
Frequency Tuning
350,4
350,6
350,8
351,0
351,2
351,4
351,6
351,8
352,0
352,2
352,4
0 5 10 15 20 25 30 35
Tuning Parameter
Fre
que
ncy
/ T
Hz
Frequency DFB 1
Frequency DFB 2
Frequency Tuning
0
0,2
0,4
0,6
0,8
1
1,2
1,4
1,6
1,8
0 5 10 15 20 25 30 35
Tuning Parameter
TH
z F
req
uen
cy /
TH
z
THz Frequency
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CW THz System Software
THz Frequency Tuning
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CW THz System Software
THz Phase Tuning
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Optional Schemes for Improved Stability
Frequency Stability with Temperature Stabilized DFB Lasers Temperature stabilized DFB lasers achieve a frequency stability of better than
50MHz Application which require a better frequency stability require an active frequency
stabilization
Active Frequency Stabilization of DFB Lasers DFB Lasers can be locked either to an atomic reference as Rubdium, Caesium or
other atomic references DFB Lasers can be locked to a technical reference as an etalon cell or a Fabry Perot
Interferometer
Locking Schemes Sacher Lasertechnik offers various locking schemes for tunable diode lasers. Several schemes as used for Side of Fringe and Top of Line type of lock
Advantages of Frequency Locking for THz Generation Minimization of Frequency drift Minimization of Phase noise Work presented at THz Workshop Kaiserslautern 2008
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Optical Tera Hertz Setup
THz Setup
CAD Layout
Realization
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Optional Schemes for Improved Stability
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Selected Application Examples
Impurity of a Chocolate Bar
in Cooperation with TU Braunschweig, Martin Koch
10 20 30 40 50 60
10
20
30
40
50
60
X position [mm]
Y p
ositi
on [m
m]
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Selected Application Examples
Mirror Reflectivity: 13 layers of alumina (A) + 12 layers of alumina-zirconia ( AZ) sintered together to a solid ceramic block
in Cooperation with TU Braunschweig, Martin Koch
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Award Winning Product
PhAST/Laser Focus World 2006
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Thank You For Your Attention!
Sacher Lasertechnik GmbHRudolf-Breitscheid-Str. 1-535037 MarburgGermany
Sacher Lasertechnik LLC .5765 Equador WayBuena Park, CA 90620United States
http://www.sacher-laser.com© 2009 Sacher Lasertechnik GmbH. All rights reserved.