スライド 1

Ultrabroadband terahertz generation
using DAST single crystal
APPLIED PHYSICS LETTERS 97, 021105-1
I.Katayama, R.Akai, M.Bito, H.Shimosato, K.Miyamoto, H,Ito and M.Ashida
Ashida lab.
Takuya Iwasa
Contents
•
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•
•
•
•
Introduction
Motivation
Experimental setup
Results & discussion
Summary
My work
THz Spectroscopy System
Time Domain Spectroscopy(THz-TDS)
• THz-TDS uses short pulses of broadband THz radiation.
• The transmitted THz electric field is measured coherently,
which provides both high sensitivity and time-resolved
phase information.
E
THz
wave
t
Probe laser
t
Time delay
THz-TDS pump probe system
Principle of THz-TDS
Electromagnetic wave
Wavelength
30mm
Micro wave
10GHz
Frequency
3mm
300μm
Submilimeter
wave
0.1THz
1THz
THz region
30μm
Far
infrared
10THz
3μm
Near
infrared
100THz
300nm
optical
1PHz
broader
• THz radiation is from 1011 to 1013Hz
approximately.
• If we generate broader radiation, we can
measure from THz region to optical region in
continuity.
THz emitter
Difference frequency generation
Nonlinear crystal
THz wave
fs laser
Intensity
Intensity
Fourier
transform
ω2 ω1
frequency
3  1  2
• A 400-μm-thick DAST
crystal was used as
nonlinear crystal.
• A DAST crystal is an
organic compound
crystal and has large
nonlinear optical
coefficient.(非線形光学係数)
ω3
frequency
DAST crystal
THz detector
Photoconductive antenna
Current
meter
A

J (t )  e  E (t ' ) N (t 't )dt'

μ: mobility of electron
fs
laser
N: the number of carrier
THz
wave
Motivation
• To generate the terahertz wave using a
DAST crystal by considering the refractive
index dispersion.
• To detect the THz wave generated by a
DAST crystal using monochromator and
THz-TDS.
Experimental setup
(Spectral Phase Interferometry for
Direct Electric-field Reconstruction)
BaF2 (a positive dispersion medium)
pulse
image
Positive chirping
Short
wavelength
Long
wavelength
Positive dispersion
medium
Time lag
Group velocity dispersion (郡速度分散)
Results & discussion
The data of laser phase spectra observed using SPIDER.
BaF2 thickness
― 0mm
― 2mm
― 4mm
0mm-thick BaF2
Long
wavelength
2mm-thick BaF2
0mm-thick BaF2
Short
wavelength
Negative chirping
Positive chirping
Results & discussion
BaF2 thickness
― 0mm
― 2mm
― 4mm
The best of these data is the one of negative chirping.
Experimental setup
Chirp mirror
Ti:Sapphire laser
BS
Pump pulse
Chopper
BaF2 plate
DAST
400mm
Delay stage
Band-pass filter
PC antenna
Probe pulse
I/V amp
lock-in amp
PC
Results & discussion
In this graph, very high frequency part is present.
Results & discussion
BaF2 thickness
― 0mm
― 2mm
― 4mm
The Fourier transform of the electric waveform. (dotted line)
Results & discussion
0mm-thick BaF2
2mm-thick BaF2
DAST
(Large positive dispersion)
Short
wavelength
Long
wavelength
The region of
generating
High-frequency
THz wave
Short
wavelength
Long
wavelength
The energy is
absorbed a lot.
Summary
• In the DAST crystal, the group velocity
dispersion is important for the generation
of the ultrahigh-frequency terahertz wave.
• A waveform is detected by using
photoconductive antenna.
My work
I try to measure a wave form by using this
optical system when there is a sample in
front of PC antenna.
Monochromator
Concave mirror
Slit
Diffraction
grating
HgCdTe and
InAs Detector
Slit
THz
pulse
SPIDER法 (Spectral Phase Interferometry for
Direct Electric-field Reconstruction)
Sum frequency

I (t)

I ()
 (t)

Intense strongly-chirped pulse from Ti: sapphire amplifier
Nonlinear Crystal

Replica2
I (t)
Interferogram
Replica1
I ()
Pulse to be measured and its duplication

SPIDER interferogram
S ()  E()  E(  )  2 E()E(  ) cos ()   (  )   
2
2
2
21