MODELING OF OPTOELECTRONIC PROCESSES IN SrS:Cu ACTFEL DISPLAY DEVICES V.P. Singh University of...
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Transcript of MODELING OF OPTOELECTRONIC PROCESSES IN SrS:Cu ACTFEL DISPLAY DEVICES V.P. Singh University of...
![Page 1: MODELING OF OPTOELECTRONIC PROCESSES IN SrS:Cu ACTFEL DISPLAY DEVICES V.P. Singh University of Kentucky, Lexington Ky A. Garcia The University of Texas.](https://reader036.fdocuments.net/reader036/viewer/2022081420/5697bf941a28abf838c90712/html5/thumbnails/1.jpg)
MODELING OF OPTOELECTRONIC PROCESSES IN SrS:Cu ACTFEL
DISPLAY DEVICES
V.P. Singh
University of Kentucky, Lexington KyA. Garcia
The University of Texas at El Paso, El Paso Tx
A. Aguilera
Hewlett Packard, Ft. Collins Co
D.C. Morton
U.S. Army Research Laboratory
Adelphi, Maryland
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-0.004
-0.002
0
0.002
0.004
0.006
0.008
0.01
400 480 560 640 720 800 880 960
Time in Microseconds
a.u
.
Voltage
Current
Luminance
GLASS SUBSTRATE
TRANSPARENT CONDUCTOR
DIELECTRIC STACK
PHOSPHOR
DIELECTRIC STACK
REFLECTIVE ELECTRODE
Va1µm
Typical VIL for ZnS:MnDisplay Device
Device Structure
![Page 3: MODELING OF OPTOELECTRONIC PROCESSES IN SrS:Cu ACTFEL DISPLAY DEVICES V.P. Singh University of Kentucky, Lexington Ky A. Garcia The University of Texas.](https://reader036.fdocuments.net/reader036/viewer/2022081420/5697bf941a28abf838c90712/html5/thumbnails/3.jpg)
Insulator
Insulator
Phosphor
Electrode
Electrode Mn
1
24
1) Electron ejection due to high electric field from the cathodic interface2) Electron gains velocity, becoming “hot”3) Electron impact excites activator atom (Mn or Cu)4) Impacting electron reaches anode contributing to the built-in reverse field5) Excited atom relaxes, emitting light
35
e-
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SrS:Cu
-0.02
-0.01
0
0.01
0.02
0.03
0.04
0.05
0 100 200 300 400 500 600 700
Time in Microseconds
a.u
.
Voltage
Current
Luminance
![Page 5: MODELING OF OPTOELECTRONIC PROCESSES IN SrS:Cu ACTFEL DISPLAY DEVICES V.P. Singh University of Kentucky, Lexington Ky A. Garcia The University of Texas.](https://reader036.fdocuments.net/reader036/viewer/2022081420/5697bf941a28abf838c90712/html5/thumbnails/5.jpg)
Comparisons
• Secondary Luminance Peaks
• Total Luminance is Small
• Comparable Amount of Tunnel Current
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Possible Causes for Low Luminance
• Lack of Tunnel Current (not the case)
• Excessive Impact Ionization - but this can Only Explain low Luminance but does not Explain Secondary Peaks
• “Other” Mechanism Needed to Explain Behavior
![Page 7: MODELING OF OPTOELECTRONIC PROCESSES IN SrS:Cu ACTFEL DISPLAY DEVICES V.P. Singh University of Kentucky, Lexington Ky A. Garcia The University of Texas.](https://reader036.fdocuments.net/reader036/viewer/2022081420/5697bf941a28abf838c90712/html5/thumbnails/7.jpg)
Hypothesize
-0.02
-0.01
0
0.01
0.02
0.03
0.04
0.05
0 100 200 300 400 500 600 700
Time in Microseconds
a.u
.
Voltage
Current
Luminance
We Hypothesize a Mechanism that Causes Luminance with a Field Reduction for a Given Device History
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-1.00
-0.50
0.00
0.50
1.00
1.50
2.00
2.50
3.00
3.50
4.00
4.50
350 550 750 950 1150
Time in Microseconds
a.u
.
Voltage
Current
Luminance
• Changing the Electric Field without Causing Tunnel Current
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Current Characteristics
-2
-1
0
1
2
3
4
5
6
7
8
300 500 700 900 1100
Time in Microseconds
Cu
rre
nt
(ma
)
Vapp = 105
Vapp = 120
Vapp = 130
Vapp = 140
Voltage
1
4
1
2
3
4
23
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-1
0
1
2
3
4
5
6
500 700 900 1100 1300
Time in Microseconds
a.u
.
Vapp = 140Vapp = 130
Vapp = 120Vapp = 105
Voltage
1
1
2
2
3
3
4
4
1,2,3
4
Voltage
Luminance Characteristics
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• During dent ramp iL(t) 0, however there is an increase in L(t) means that electrons are recaptured by ionized activators
a) Come from Interface State and only Recaptured by nearby Ionized Activators
b) Formed by the Activator and a Defect Produced by the Activators Presence in the Lattice electrically forming a Dipole
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Dipoles
• Are Activator-Bulk Trap pair Formed by the Introduction of the Activator in the Phosphor
• Bulk Trap is Localized in Close Vicinity of the Activator
• A Certain Minimum Field is Needed to Create/Maintain the dipole
Positively ChargedActivator
Negatively ChargedTrap
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Transient Results
-2.5
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
2.5
0 500 1000 1500 2000 2500 3000 3500 4000 4500
Time in Microseconds
a.u
.
Vapp = 130Vf = 500Hzpw = 200us10/10/99
-2.5
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
2.5
0 500 1000 1500 2000 2500 3000 3500 4000 4500
Time in Microseconds
a.u
.
Vapp = 130Vf = 500Hzpw = 200us10/10/99
Tunnel Current appears in the very first pulse
Luminance becomes noticeable in the 4th voltage pulse
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Conclusions
• A more Complete Model is required to study SrS:Cu
• Currently this Dipole Model is able to Explain the Observed Features but
• Further work is required