Min Hyeong KIM High-Speed Circuits and Systems Laboratory E.E. Engineering at YONSEI UNIVERITY
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Transcript of Min Hyeong KIM High-Speed Circuits and Systems Laboratory E.E. Engineering at YONSEI UNIVERITY
A hybrid silicon evanescent laser fabricated with a silicon
waveguide and Ⅲ-Ⅴ offset quantum wells
Hyundai Park, Alexander W. Fang, Satoshi Kodama, and John E. Bowers
Min Hyeong KIMHigh-Speed Circuits and Systems Laboratory
E.E. Engineering at YONSEI UNIVERITY2011. 4. 13.
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[ Contents ]
1. Abstract2. Introduction
- Several laser structures3. Device structure
I. Lasing gain material II. Waveguides III. Bonding technologyIV. Additional layer
4. Fabrication process5. Experimental results6. Conclusion & Summary
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1. Abstract
A laser can be utilized on a silicon waveguide bonded to a multiple quantum wells(MQW).
This structure allows the optical waveguide defined by CMOS technology to get an optical gain provided by Ⅲ-Ⅴ materials.
It has a 1538nm laser, pulsed threshold of 30mW, and an output power of 1.4mW.
How to implement this structure?How to operate??Which principles???
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2. IntroductionIt is challenge to build light-emitting devices on VLSI CMOS technology. Because Si has an indirect bandgap(E_g).How to overcome this challenges?1. Raman laser2. Using porous silicon or nanocrystalline-Si3. SiGe quantum cascade structures4. Er doped silica5. Etc….In this paper, we report the first demonstration of silicon evanescently** coupled laser structure.
** Evanescent waveAn evanescent wave is a nearfield standing wave with an intensity that exhibits exponential decay with distance from the boundary at which the wave was formed.
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3. Device structure
Silica
Si substrate
InP Cladding
MQW gain material
Si
MQW laser+
SL barrier+
Bonding technology+
SOI waveguide
Light-emitting Process :Current or Laser Pumping >> MQW lasing >> wave evanescent to SOI waveguide >> output guiding
3.6%
42.8%QW
Si
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3. Device structureⅠ. Lasing gain material – MQW(mutiple quantum wells)
Ⅱ. Waveguides – SOI structure(last topic)
• A quantum well laser is a laser diode in which the active region of the device is so narrow that quantum confinement occurs.
• The wavelength of the light is determined by the width of the active region.
• Much shorter wavelengths can be obtained.
• Low threshold current.• The greater efficiency.
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out C I
I
E E E
hEm d
Ⅰ
Ⅱ
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3. Device structureⅢ. Bonding technology – Plasma-Assisted Low Temperature Wafer Bonding
Ⅲ
• Two samples are bonded together via oxygen plasma assisted wafer bonding
• Low temperature annealing(~250℃) preserves the optical gain of MQW.
• High temperature annealing makes (1) a surface non-uniformities and (2) gain reduction.
Hydrophilic surface bonding : 125℃Hydrophobic surface bonding : 400℃Are better choices.
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3. Device structure Ⅳ
Ⅳ. Additional layer – SL(Superlattice) barrier
SL interpositio
n
Doped SL
Non-intentionally doped SL
• Defect-blocking layer : It prevents the deep propagation of defects by fusing process.
• Luminescent properties are improved.
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3. Device structure _ detailed design
• InP cladding layer• MQW absorber (500nm)• MQW laser structure• MQW absorber (50nm)• InP cladding layer (110nm spacer)• SL barrier (7.5nm)• Si waveguide (W=1.3u, H=0.97u,
L=0.78u)• Silica layer (500nm)• Si substrate
For operating 1538nm wavelength
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4. Fabrication process1. Form SiO2 layer on Si substrate _ thermal oxidation for 2
hours at 1050℃2. Form Si rib waveguides _ using inductively coupled
plasma etching3. Hetero-bond InP(already completed)/Si _ Plasma-Assisted
Low Temperature Wafer Bonding4. Dice the device for mirroring 5. Polish and HR coat**(High-reflection coatings) for
mirroring
** HR coating
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5. Experimental results[Experimental Conditions]
• 980nm laser diode pumping• Through the top InP cladding
layer• Recorded on an IR camera
through a polarizing beam splitter
Laser diode Pumping
[Results Pictures]
Calculated TE mode profile TE near field image
3.6%
42.8%QW
Si
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5. Experimental results
• A laser output almost occurs in the optical mode(Si waveguide)
• Slab mode(MQW) do not support lasing output
• The pumping threshold increase from 30mW to 50mW between 12℃~20 ℃.
• Quantum efficiency at 12℃ : about 3.2%
Cavity length 600umTemperature 12℃Pump power=1.4* thresholdGroup index=C/Vg=3.85
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6. Conclusion & Summary
• We can make the optically pumped Si evanescent laser consisting of MQW as active region bonded to Si waveguide as a passive device. (conclusion!)
• For operating at 1538nm, pump threshold is 30mW and slope efficiency is 3.2%. (conclusion!)
• On bonding process, use Plasma-Assisted Low Temperature Wafer Bonding to maintain the optical gain of gain material.
• By using SL(Superlattice) barrier, we can block the defects propagation from fusing(bonding) process.