橋本佑介 a,b 三野弘文 a 、山室智文 a 、蒲原俊樹 a 、神原大蔵 a...
DESCRIPTION
13aXD-14. 希薄磁性半導体 CdMnTe における強励起効果. High excitation effects in dilute magnetic semiconductor CdMnTe. 橋本佑介 A,B 三野弘文 A 、山室智文 A 、蒲原俊樹 A 、神原大蔵 A 、松末俊夫 B Jigang Wang C 、 Chanjuan Sun C 、河野淳一郎 C 、嶽山正二郎 D 千葉大院自然 A 、千葉大工 B 、ライス大 ECE C 、東大物研 D Y. Hashimoto A,B - PowerPoint PPT PresentationTRANSCRIPT
橋本佑介 A,B
三野弘文 A 、山室智文 A 、蒲原俊樹 A 、神原大蔵 A 、松末俊夫 B
Jigang WangC 、 Chanjuan SunC 、河野淳一郎 C 、嶽山正二郎 D
千葉大院自然 A 、千葉大工 B 、ライス大 ECEC 、東大物研 D
Y. HashimotoA,B
H. MinoA, T. YamamuroA, T. KamoharaA, D. KanbaraA, T. MatsusueB, J. WangC, C. SunC, J. KonoC, S. TakeyamaD
Graduate School of Science and Technology, Chiba Univ.A 、Department of Engineering, Chiba Univ.B, ECE Dept., Rice Univ.C 、 ISS
P, Univ. of TokyoD
13aXD-14
High excitation effects in dilute magnetic semiconductor CdMnTe
希薄磁性半導体 CdMnTe における強励起効果
Magnetic Polarons
Mn spin
Exciton spine
h
Free Exciton Magnetic Polaron (FEMP)
Localization only by sp-d exchange interaction
A Golnic, et. al. J. Phys. C16, 6073 (1983)M. Umehara, Phys. Rev. B 68, 193202 (2003)
Photo-induced ferromagnetismvia the FEMP
Free exciton magnetic polaron (FEMP) in CdMnTe
High quality CdMnTe sample
with low Mn concentration
He-Ne laser76 MHz Ti:Sapphire laser
250 kHz OPA laser1 kHz OPA laser
Exciton density 1012 – 1020
[cm-3]
CW and Time-resolved Photoluminescence
Current work :
Alloy potential fluctuation : Small
x = 5 ~ 10% → FEMP energy : Large
S. Takeyama, J. of Crys. Growth, 184-185 (1998) 917-920
Mn Concentration [%]
Localiza
tion
en
erg
y
105
Alloy Potential fluctuation
Localization energy of Magnetic Polaron
Free Exciton Magnetic Polarons
FEMP Bipolaron
Ferromagnetic Phase Transition via Free Exciton Magnetic Polarons ?
Experimental Setup for PL measurements
Laser
CCDor
Streak camera
Spectro-meter
Sample 1.4 K
Bulk Cd1-xMnxTex = 5%
Cd1-yMgyTe
Cd0.95Mn0.05Te
GaAs
Lasers
Laser Exciton density [/cm3] rs Wavelength
He-Ne 2.2 x 1013 33 634 nm
Ti: Sapphire 2.8 x 1015 6.6 400 nm
250KHz OPA 8.6 x 1017 1 700 nm
1KHz OPA 2.2 x 1020 0.15 634 nm
1 kHz OPA250 kHz OPATi: SapphireHe-Ne
1013 1014 1015 1016 1017 1018 1019 10201012
1210 0.1100
nrs
Excitation intensity: 1mW, Focus size: 200m, O.D. 1
aB = 6.7 nm nMott = 7.9 x 1017 [cm-3]
Low Excitation Limit Exciton Density 1012 - 1014 [cm-3]
Absorption: 4.2 K, PL: 1.4KPL Light source: He-Ne 633nm
Absorption
PL
1.6801.6701.6601.650
FEMP
FX
BMP
BMP'
Pho
tolu
min
esce
nce
Absorption
Photon energy [eV]
Distinct PL line of the FEMP appear !! FEMP binding energy 1.8 meV
Ti: S
1
kHz O
PA
25
0 kH
z OPA
He-N
e
1013
1014
1015
1016
1017
1018
1019
1020
1012
BX
Photoluminescence Exciton Density 1015 – 1016 [cm-3]
Ti:S
1 kH
z OPA
25
0 kH
z OPA
He-N
e
1013
1014
1015
1016
1017
1018
1019
1020
1012
Excitation intensity normalized PLExciton density 1015, 1016[cm-3]
FEMP PL intensity: SaturateFX PL intensity: Increase
PL
inte
nsi
ty
1.6761.6721.668Photon energy [eV]
FX
FEMP
1015
1016
BX
1.681.671.66
Photon energy [eV]
400
300
200
100
0T
ime
[ps]
Time Resolved Photoluminescence Exciton Density 8.6 x 1017 cm-3
1020
Ti: S
1
kHz O
PA
25
0 kH
z OPA
He-N
e
1013
1014
1015
1016
1017
1018
1019
1012
AB1.674eV1.667eV
BXEHP
PL
inte
nsi
ty
1.701.681.661.64Photon energy [eV]
t = 40 - 140 ps
Time Resolved Photoluminescence
Exciton Density 8.6 x 1017 cm-3
A: 1.674 eV ~ 150 ps BiexcitonB: 1.667 eV < 30 ps ?
A
Inverse Boltzman
1020
Ti: S
1
kHz O
PA
25
0 kH
z OPA
He-N
e
1013
1014
1015
1016
1017
1018
1019
1012
4
6
1
2
4
6
10
2
4
6
100
PL
inte
nsi
ty
10008006004002000
Time Delay [ps]
A (1.6768 ~ 1.6723 eV) B (1.6611 ~ 1.6656 eV)
Many Body Effect of FEMPs
Coupled two FEMPs has been expected to be more stable than single FEMP
Bi-polaron Bi-exciton
PhotoluminescenceExciton Density > Mott Density
Ti: S
1
kHz O
PA
25
0 kH
z OPA
He-N
e
1013
1014
1015
1016
1017
1018
1019
1020
1012
Electron hole plasma I4.2
Biexciton I1.6
Ph
otol
um
ines
cen
ce
1.681.661.641.62
Photon energy [eV]
Biexciton
12 K
I2I
3.3I
EHP I = 5.6 × 1018 [cm-3]
Exciton Density Dependence of Origin of Photoluminescence
FEMPElectron hole
PlasmaBiexciton
Ti: S
1
kHz O
PA
25
0 kH
z OPA
He-N
e
1013
1014
1015
1016
1017
1018
1019
1020
1012
Summary
PL measurements Exciton density: 1012 – 1020 [cm-3]
FEMP Biexciton
Electron hole plasma
Future work
Spin Dynamics Under Strong Excitation
Free Exciton Magnetic Polaron
Hole mass:
0960
810
.m
m
.m
m
e
e
e
h
Electron mass:
meVN
meVN
880
220
0
0
Hole14.4Å
Electron
64Å
The number of Mn ionelectron: 481hole: ~5.5
Mn spin
Exciton Density Dependence
When the exciton density is above 1018 cm-3 FEMP may disappear
1.5
1.0
0.5
0.0
FE
MP
bin
din
g en
ergy
[m
eV]
0.1 1 10 100 1000Exciton density (× 10
16) [cm-3]
Ti: S
1
kHz O
PA
25
0 kH
z OPA
He-N
e
1013
1014
1015
1016
1017
1018
1019
1020
1012
Excitation intensity normalized FEMP PL int.FEMP binding energy
Nor
mar
ized
FE
MP
PL
In
t.
0.1 1 10 100Exciton density (× 10
16) [cm-3]
0
Spin Relaxation Dynamics
]cm[~n 316104
][104~ 317 cmn ]cm[~n 318101
1013
1014
1015
1016
1017
1018
1019
1020
1012
-4x10-3
0
4
T
/T
20100Time delay [ps]
10x10-3
86420
T
/T
20100Time delay [ps]
-8x10-3
-4
0
T
/T
20100Time delay [ps]
5K
Time Resolved Photoluminescence
1.6901.6851.6801.6751.6701.665
300
200
100
0
1.4K
Ti: S
1
kHz O
PA
25
0 kH
z OPA
He-N
e
1013
1014
1015
1016
1017
1018
1019
1020
1012
1.681.671.66Photon energy [eV]
400
300
200
100
0
Tim
e [p
s]
250 kHz OPA laser 76 MHz OPA laser
1.4K
Experimental Setup for PL measurements
chopper
Movablemirror
Sample 13 K1kHz OPA&CPA
He-Ne
PhotodiodeSpectro-meter
Lock-in Amplifier
Discussions
1.665
1.660
1.655
1.650
1.645
PL
pea
k p
osit
ion
[eV
]
151050
Exciton density ( x 1018
) [cm-3
]
100x10-15
80
60
40
20
0
PL
inte
nsi
ty
151050Exciton density ( x 10
18) [cm
-3]
0
Mott transition
EHP Exciton
Excitation Dependence of the PL Intensity
Excited with Ti:Sapphire Laser
2
4
1
2
4
10
2N
orm
ariz
ed P
L in
tens
ity
60.1
2 3 4 5 61
Exciton density (× 1016
) [cm-3]
FEMP FX
I1.28
I1.04
I1.0
meVEE FEMPBX 1G
X
X2BX
FEMP
meV.EFEMP 82
Peak position [eV]
Binding Energy[meV]
Absorption 1.6748
Biexciton 1.6741 0.7
FEMP 1.6722 2.6
meV.meV.EBX 3383 Estimate by the EBX (4.1 meV) on CdSe
Purpose
G
X
FEMP
BXX2
21 n/BX
ps~FEMP 10