Er-doped hybrid waveguide amplifiers with multiple spatially engineered active layers can enhance optical gain on a chip. Modeling shows that using three thin Er-doped layers instead of a single thick layer in a 1 cm long waveguide can increase the net gain by up to 30%. Spatially engineering the active layers takes advantage of rare-earth ion interactions to optimize doping and minimize quenching effects, improving efficiency.
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Er-doped hybrid waveguide amplifiers with multiple spatially engineered active layers for on-chip optical gain enhancement
1. Er-doped hybrid waveguide
amplifiers with multiple
spatially engineered active
layers for on-chip optical
gain enhancement
D.Sc. John Rönn
SPIE Photonics Europe 2022
Paper 12148-3
john.ronn@beneq.com
3. 6/22/2022
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4. 6/22/2022
BENEQ – HOME OF ALD
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9. 6/22/2022
ALD FOR SILICON PHOTONICS
On-chip active functionalities have been extensively studied over the past decades
10. 6/22/2022
ALD FOR SILICON PHOTONICS
On-chip active functionalities have been extensively studied over the past decades
Semiconductors undisputed in many applications
• Integration with Si difficult
• Temperature sensitive
• Short lifetime
11. 6/22/2022
ALD FOR SILICON PHOTONICS
On-chip active functionalities have been extensively studied over the past decades
Semiconductors undisputed in many applications
• Integration with Si difficult
• Temperature sensitive
• Short lifetime
Rare-earth-ion-doped materials an alternative solution
Monolithic integration with Si
Cheap and easy to fabricate
Long excited state lifetime → High output power
Temperature insensitive → Narrow laser linewidths
Low noise
12. 6/22/2022
ALD FOR SILICON PHOTONICS
In rare-earth materials, transitions are parity-forbidden
• Weak oscillator strengths for transitions
• High doping required to provide reasonable gain
High doping causes quenching and up-conversion
• ∝ 𝑅−6
, 𝑅 = Distance between ions
• Can be optimized by tailoring the doping profile
20. 6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
𝐿 = 1 cm
𝛼0 = 1 dB/cm
𝑡 = 10 − 500 nm
𝜆p = 1480 nm
𝜆s = 1533 nm
𝑃in = 50 mW, Sin = 1μ𝑊
21. 6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
𝐿 = 1 cm
𝛼0 = 1 dB/cm
𝑡 = 10 − 500 nm
Net Gain for a single active layer
𝜆p = 1480 nm
𝜆s = 1533 nm
𝑃in = 50 mW, Sin = 1μ𝑊
22. 6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
𝐿 = 1 cm
𝛼0 = 1 dB/cm
𝑡 = 10 − 500 nm
Net Gain for a single active layer
𝜆p = 1480 nm
𝜆s = 1533 nm
𝑃in = 50 mW, Sin = 1μ𝑊
23. 6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
𝐿 = 1 cm
𝛼0 = 1 dB/cm
𝑡 = 10 − 500 nm
Net Gain for a single active layer
𝜆p = 1480 nm
𝜆s = 1533 nm
𝑃in = 50 mW, Sin = 1μ𝑊
25. 6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
Net Gain for three active layer
𝐿 = 1 cm
𝛼0 = 1 dB/cm
𝑡 = 10 − 500 nm
𝜆p = 1480 nm
𝜆s = 1533 nm
𝑃in = 50 mW, Sin = 1μ𝑊
26. 6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
Net Gain for three active layer
𝐿 = 1 cm
𝛼0 = 1 dB/cm
𝑡 = 10 − 500 nm
𝜆p = 1480 nm
𝜆s = 1533 nm
𝑃in = 50 mW, Sin = 1μ𝑊
27. 6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
Net Gain for three active layer
𝐿 = 1 cm
𝛼0 = 1 dB/cm
𝑡 = 10 − 500 nm
𝜆p = 1480 nm
𝜆s = 1533 nm
𝑃in = 50 mW, Sin = 1μ𝑊
28. 6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
Net Gain for three active layer
Up to 30% gain enhancement!
𝐿 = 1 cm
𝛼0 = 1 dB/cm
𝑡 = 10 − 500 nm
𝜆p = 1480 nm
𝜆s = 1533 nm
𝑃in = 50 mW, Sin = 1μ𝑊
29. 6/22/2022
Summary
ALD performs extremely well in devices that require conformal
coating
Material properties can be tailored by engineering the ALD-
precursors
ALD shows excellent potential in Silicon Photonics where active
devices are in high demand
Further optimization of the active layer properties enables higher
efficiencies and opens up a completely new way of designing
active devices
31. Beneq® is a leading supplier of
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34. 6/22/2022
SCALING-UP
Myth: ALD is a very slow deposition technique
Batch ALD:
Beneq P400A Beneq P800 Beneq P1500
Batch size: up to 8 m2 Batch size: up to 40 m2 Batch size: a medium-sized car
35. 6/22/2022
SCALING-UP
Myth: ALD is a very slow deposition technique
Spatial ALD:
Beneq C2R
Process Temperature Deposition rate
Al2O3 120 °C > 1500 nm/h
TiO2 120 °C > 1100 nm/h
SiO2 120 °C > 650 nm/h
Ta2O5 150 °C > 800 nm/h