140.120.11.120 1 high-frequency transport properties of two- dimensional electronic systems at low...
TRANSCRIPT
1140.120.11.120
High-frequency transport properties of two-dimensional electronic systems at low temperatures
Y. W. Suena(孫允武 ), W. H. Hsiehb(謝文興 ), L. C. Lia(李良箴 ), H. M. Chenga (鄭憲明 ), T. C. Wana (萬德昌 ), J. Y. Oua (歐俊裕 ), Y. J. Huanga (黃盈傑 ), C. Y. Chena (陳紫瑜 )
a Department of Physics, National Chung Hsing University, Taichung, Taiwan, R.O.C.b.Department of Electrical Engineering, National Taiwan University, Taipei, Taiwan, R.O.C.
Our home:140.120.11.120
2140.120.11.120
Samples:
GaAs/AlGaAs: (1) 交大電子 李建平
(2) 以色列 / 彰師物理 吳仲卿
Si/SiGe: 台大凝態中心 鄭鴻祥
Instrumentaions:
Pulsed RF/microwave PLL: 張冠英,陳家怜,王文凱,黃盈傑,李良箴
Cryogenic Systems, Wiring & Programming: 謝文興,李良箴,歐俊裕
Samples & Measurement: 萬德昌,鄭憲明,謝文興,李良箴
Cheap Labor: 陳紫瑜,歐俊裕
Money:NSC
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Outline
1. Detection by a Phase Lock Loop
2. Surface Acoustic Wave Detector
3. Coplanar Wave Guide Detector
4. Pulsed Microwave PLL system
5. Some Preliminary Results
6. Kind of Conclusions
7. Future Works
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Detection by Phase Lock Loop (PLL)
Type-II PLL
Sample under detection
phase=1=11PLL system
s=ss
0 =1+ s =11
+s(B)s
0 =0=1+ s(B) =11+s(B)s
111
B:the parameter (magnetic field) changed in the experiment:velocity of the wave
can be measured very accurately.
sample
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Reference
From sample
Keep at a constant phase difference
Reference
From sample
Due to the change of sample conditions
Reference Tuning the frequency to match the phase
From sample
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SAW Delay-Line Sensor
2
2
00 )/(1
1
2 Mxx
effK
Lf
f
σ
2
2
SAW )/(1
/
2 Mxx
MxxeffKk
σσσσ
L
)( 210 M
GaAs:3.6×10-7 -1
GaAs/LiNO3(Y-Z):1.8×10-6 -1
2
,2, 00 fq xxxx
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Anything GOOD to use SAW detectors?!
1. No contact!
2. Short wavelength compared to EM signals at the same frequency.
3. Low energy compared to EM signals at the same wavelength.
4. We can use SAWs to detect the special length scale in the sample via the size-resonance of SAWs and the sample.
11140.120.11.120
Coplanar Waveguide (CPW) Sensor
Electric field
50 meandering CPWtotal length s
xx
0,0 qxx
m2
12
eff
D
dG
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Coplanar Waveguide (CPW) Sensor
Some formulae: 1m)()( CjGLjjj
m
F0 eff
LC ,
eff
r
C
LZ
0
00
11
m
12
12
eff
D
d
G
m
Np
2
m
rad
8
11
2
1
0
2 ln
Z
deffD
xx or 1
2/1
20
222 8
L
eff
s
Dxx Z
dfLf
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Pulsed RF/Microwave PLL and Gated Averaging System
Gated Average
Time Delay
RF or Microwave Generator
DC-Coupled Frequency Modulation (FM)
Directional Couplers
HighSpeed Diode Switch
Step Attenuator
Double-Balance Mixer
Pulse Generator
Amplifier
Power Splitter
Intensity Output
Power Detector
PLL
Integrator積分器
Precision Counter
(b1)
(I)
(C)
(M)
(D)
(E)
(P)
(G)
(H)
(s1)
(A)
(b2)
(s2)
(b3)
Stainless-StealSemirigid Coax
Stainless-StealSemirigid Coax
黑色 : 低頻訊號橙色 : 高頻訊號
(B)
Z Z
Cryogenic Environment
Impedance Match Network
Impedance Match Network
Active LDES Region
SAW Emitter IDT
SAW Receiver IDT
Sample
(F) (F)
(S)
(J)
Why pulsed?
1. Use low average power to prevent from heating
2. Use gated averaging technique to avoid direct EM interruption
3. Avoid the reflection and multiple reflection signals
What’s different from others:
We use type II PLL, home-brew sample-&-hold circuits, and cheap lock-in amplifiers.
14140.120.11.120
An improved homodyne amplitude detection scheme.
0º 90º
Ref. Signal
Signal from the sample
90º hybrid
Power splitter
mixerTo PLL
To amplitude detection
~0
A home-made vector meter??
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Signal Gating & Averaging:
RF/Microwave pulse train
3~4 ms set by lock-in amp
~200 s set by lock-in amp
0.2~2 s set by pulse shaping circuit
s1(t)
s1(t)
time delays2(t) signal of mixer or power detector
sampling delay set by pulse generator
sampling gate set by a pulse generatorfed into the controlling node of a sample-and-hold circuit
s3(t)
Direct coupled EMReflected signals
s4(t) signal after SH
Peak power about –30dBm
fed into lock-in
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A semiconductor chip attached on the SAW delay line
BeCu SR coax
IDT SAW transducer
Chip tied on the SAW delay line
He3 sample holder
5mm
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90M 100M 110M 120M 130M 140M 150M
10dB
Tra
nsm
issi
on
Frequency
LiNbO3 120M 022
Transmission of the SAW transducers
=29m
500m
30 pairs
Y-cut
Z-propagation
Room temperature
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Data read from SAW delay line (sample #1):
0 2 4 6 8 10
0
1x10-4
2x10-4
3x10-4
0.2dBm
f/f 0
B (Tesla)
f/f0
SAW Intensity
=1
=2
ns=1.9×1011 cm-2
f0=120MHzT=0.3KGaAs/AlGaAs 2DES
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Data read from SAW delay line (sample #2):
0 2 4 6 8 10 12
SAW
Int
ensi
ty
0.001%
f
/f 0
B (Tesla)
=2
=1
ns=2.5×1011 cm-2f0=120MHzT=0.3KGaAs/AlGaAs 2DES
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Compared with :(SAW Data #1)
0 2 4 6 8 10 121x10-8
1x10-7
1x10-6
1x10-5
1x10-4
xx
B (Tesla)
xx of sample #1
T=0.3 K
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Compared with :(SAW Data #1)
0 2 4 6 8 10
measured calculated
f/f 0
B(Tesla)
-0.001
0.000
0.001
0.002
0.003
0.004
0.005
0.006
0.007
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Compared with :(SAW Data #1)
0 2 4 6 8 10
Inte
nsity
B (Tesla)
measured calculated
0.2dBm
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Transmission of the CPW transducer on Si/SiGe
Width = 25μmGap(deff) = 43μmTransmission lenth = 13mm
108 109
CPW at 0.3K
6dB
Tra
nsm
issi
on
Frequency(Hz) 5k-Si substrate
500Å Si
3000 Å Si
1.6×1012 cm-2(B doping)
100 Å_Sispacer_layer
300Å SiGe
3000Å Si buffer
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Data read from CPW:
0 2 4 6 8 10 12
0
5x10-4
1x10-3
N383 CPWT=0.3K
f/f 0
B (Tesla)
200MHz 800MHz
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Compared with :
0 2 4 6 8 10 12
1x10-5
2x10-5
3x10-5
N383T=0.3 K
xx
(f 0)
B (Tesla)
200MHz 800MHZ
0
1x10-5
2x10-5
3x10-5
4x10-5
DC
xx (-1
)