nonlinearity in terahertz photon physics masaya nagai dep. physics, kyoto univ. janan presto, jst,...
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Nonlinearity in terahertz photon physics
Masaya NAGAI
Dep. Physics, Kyoto Univ. Janan
PRESTO, JST, Japan
June 15, 2010APSE2010Osaka, Japan
Colleague
M. Jewariya, H. Hirori, K. Tanaka (Kyoto Univ.)
I. Ichikawa, H. Ohtake, T. Sugiura, Y. Uehara (Aishin seiki)
I. Katayama, H. Aoki, J. Takeda (Yokohama National Univ.)
H. Shimosato, M. Ashida, R. Kinjo, I. Kawayama, M. Tonouchi (Osaka Univ.)
Outlines
• Intense THz field governs material properties non-collinear optical rectification with LiNbO3
• nonlinear spectroscopy in THz frequency regionVibrational mode in amino-acid microcrystal and SrTiO3
e-h system in semiconductorsOrientational motions in water
• Summary
Material Science in THz region
Plasma motion
0.1nm1nm1m1mm1m 10nm100nm10m100m10mm100mm
visble
X 線
Intramolecularvibration
Electric transition
MIR
1
2
X-raydifraction
microwave NIR UV X-ray 線
Orientationalmotion
FIR
1
2
Intermolecular vibration
Soft mode in dielectric materialSuperconductor gap …..
rot H = Jcond +4D ct
Electronics(LCR, diode, etc)
Photonics(transition between
quantum levels)
Typical timescale of damping in solids is ps.
Intense monocycle THz pulse can be assume as
i
ine2/m
Impulsive force with lowest center frequency
as intense quasi-DC field
ps timescale of damping in materials
Intense THz pulse generation with tilted pulsefront excitation
Tilted pulsefrontExcitation pulse
THz pulse
EO crystal(Mg: LiNbO3)
Review: Hebling et al. J. Opt. Soc. Am. B 25, B6 (2008)
10J
vgr cos = vTHz
Intense THz pulse in Kyoto Univ.
Output power 0.6 J Maximum filed 249 kV/cmJewariya, MN, et al., JOSAB 26, A101 (2009).
109
1010
1011
1012
1013
1014
1015
1016
Pow
er (log scale)
76543210Frequency (THz)
300
200
100
0
-100
Ele
ctric
fiel
d (k
V/c
m)
1050Time (ps)
600 J ex.
Cascaded (2) process enhances generation efficiency
MN et al. Opt. Express, 17 11543 (2009).
IMRA AMERICA FCPA Jewel D1000
Wavelength: 1045nmOutput power: 1W 10JRepetition: 100kHz Duration: 600fs
10-1
100
101
102
103
104
105
106
Pow
er (log)
3.02.01.00.0Frequency (THz)
8
4
0
-4
Ele
ctric
fiel
d (k
V/c
m)
12840Time (ps)
8.5J
3.7J
.95J
X12
X70
aExcitation pulse
Phase modulationOptical
rectification
THz pulse
EO crystal
Large amplitude vibration driven with intense THz pulse
Vibrational potential has anharmonicity, and large-amplitude vibrational motions (climbing higher excited levels) brings in dissociation, which is decisive for chemical reaction and phase transition.
Using intense THz pulse resonant for vibrational modes, we can coherently drive large amplitude vibrational motions
Nonlinear medium: L-Arginine
L-Arginine: amino-acid molecules
L-Arginine microcrystal has the intermolecular vibration mode at 1 THz.
60
50
40
30
20
10
0
Ab
sorp
tion
(cm
-1)
1.51.00.50.0Frequency (THz)
13K100K300K
Population
kBT
Jewariya, MN, Tanaka , submitted
Time profile of Electric pulse passed through the arginine pellet
Ele
ctri
c fie
ld (
nor
m.)
151050Time (ps)
Ref.
Arginine 300K 100kV/cm 3 kV/cm
X1/2
Jewariya, MN, Tanaka , submitted
Inte
nsi
ty
1.51.00.50.0Frequency (THz)
1.0
0.5
0.0
Op
tica
l De
nsi
ty
100 25 3 kV/cm
arginineref
sample
0.8
0.7
OD
1 10 100kV/cm
1.0THz
Ladder climbing in anharmonic potential
Above 10 stepsLadder climbing
Large E()
small E()
Jewariya, MN, Tanaka , submitted
Coherent processes in several levels system
86420Time (ps)
(a)
(b)
E (n
orm
.)P (no
rm.)
0.1 6
1.5
1.0
0.5
0.0
Im[P
/E ] (arb. units)
1.51.00.50.0Frequency (THz)
(c)
0.1 3 6
E0/h=1
iiiiiiiiiiiiii
iiii
iiiiiiiiiiiiiiiiiiiiii
tEi
tEi
dt
td
dt
td
tEi
tEi
dt
td
,1,1*
1,1,2,1,11,
*,11,
*1,
*1,,11,
*,1
*,1,1,11,11,1
,
2
P=Tr[]
nn
n-1 n-1
n+1 n+1
n+2 n+2 3 kV/cm25 kV/cm100 kV/cm
n-1,n
n,n+1
n+1,n+2
Two level system: Casperson, PRA 57, 609 (1998).
Hardening of softmodein SrTiO3 thin film
kBT
Katayama MN et al. CLEO/QELS 2010
THz pump-vis probe spectroscopy in ZnSe MQW system
Hirori, MN, Tanaka, PRB 81, 081305(R) (2010).
1.5
1.0
0.5
0.0
OD
2.962.922.882.84
Energy (eV)
THz off
THz onhhlh
(b)MQWs
THz pump pulse
probe optical pulseat 10 K
nB=1
V reh
Exciton resonance disappears with blue shiftEex/eaB = 70 kV/cm
THz motions of WATER
Fukasawa et al. PRL 95, 197802 (2005)
Huge orientational relaxation mode, related to hydrogen bonding network, lies in THz frequency region.
Raman tensor at low frequency is little, so it is difficult to drive water molecules via Raman induced Kerr effect.
Dielectric tensor
Raman tensor
Response of water in 100m silica cell
EO s
igna
l
15105Time (ps)
ref(x1/ 5)
ref(x1/ 5)
E0
E0/ 32
Water (296K)(a)
4
3
2
1
0
-Log
(T)
1.51.00.50.0Frequency (THz)
2
1
0
Phase (rad) -20ps off
set
E0 E0/ 2 E0/ 4 E0/ 8 E0/ 16 E0/ 32
(b)
Single THz pulse responses of water
MN and Tanaka CLEO/QELS 2010
Temporal evolution of dielectric constant of water
(c)
100
50
0
-50Ele
ctri
c fie
ld (
kV/c
m)
2015105Time (ps)
pump
probe (2.5ps)
10
8
6
4
2
0D
iele
ctric
con
sta
nt
1.51.00.50.0
Frequency (THz)
-3.0 1.0 6.5 ps
ri
76543
i
50-5t (ps)
0.3
0.6THz
MN and Tanaka CLEO/QELS 2010
Even with sub-mW injection, temperature of orientational motion increase a few tens K.
Rotational motion is driven without thermal relaxation (or before heating other modes)8
6
4
2
0
Im[
]
43210
Frequency [THz]
i
362 K (89°C)335 K (62°C)313 K (40°C)295 K (22°C)278 K (5°C) 267 K (-6°C)
8
6
4
2
0
Im[
]
43210
Frequency [THz]
i295 K (22 ºC)
10
8
6
4
2
0
Re
[] r
Water10
8
6
4
2
0
Re
[]
r
H2O(a)
Yada, MN, Tanaka, CPL (2008).
Driving orientational motion of water
Hydrogen bonding network controlled with THz pulse
We can control water properties as SOLVENT in ps timescale, which influence chemical reactions of solute molecules.
MN and Tanaka CLEO/QELS 2010
Summary
• We succeed intense THz pulse generation with >200 kV/cm field amplitude.
• We demonstrate THz nonlinearity of vibration modes in amino acide microcrystal and dielectric materials. Experimental results is interpreted with ladder climbing in anharmonic potential.
• We demonstrate huge spectrum modulation near the bandgap of semiconductors with intense THz pulse, which shows non-perturbed nonlinear regime.
• We observe water molecules driven by intense THz pulses. This motions is different from thermal effects. Results show the reorientational motion of water molecules with breaking hydrogen bonding in several picosecond timescale.