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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
BENEQ –
HOME OF
ALD
6/22/2022
BENEQ – HOME OF ALD
 World’s leading ALD-dedicated company
 40+ years of ALD expertise
 40+ dedicated ALD systems in operation 24/7
 200+ personnel
 Divided into two business lines
 Advanced ALD
• Optics & Photonics
• Battery Technology
• Part Coating
 Semiconductor ALD
• Micro- & optoelectronics
• Power & RF Devices
• MEMS
6/22/2022
BENEQ – HOME OF ALD
Research Equipment
Beneq R2 Beneq TFS200 Beneq TFS500
Wafer Fabrication
Beneq Transform™
3D & Batch
Beneq P400A Beneq P800 Beneq P1500
Spatial ALD
Beneq C2R Genesis ALD
6/22/2022
BENEQ – HOME OF ALD
 Why ALD?
6/22/2022
BENEQ – HOME OF ALD
 Application areas: Microstructures
 Integrated waveguides
 Cylindrical lenses, Fibers
 Structured wafers
6/22/2022
BENEQ – HOME OF ALD
 Application areas: Macrostructures
 Highly-curved lenses
 3D-Structures
 Freeform optics
ALD FOR
SILICON
PHOTONICS
6/22/2022
ALD FOR SILICON PHOTONICS
 On-chip active functionalities have been extensively studied over the past decades
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
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
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
6/22/2022
ALD FOR SILICON PHOTONICS
 Er-doped Al2O3 with ALD
Beneq TFS500
Al C
H Er
O
6/22/2022
ALD FOR SILICON PHOTONICS
 Er-doped Al2O3 with ALD
Beneq TFS500
Al C
H Er
O
6/22/2022
ALD FOR SILICON PHOTONICS
 Er-doped Al2O3 with ALD
Beneq TFS500
6/22/2022
ALD FOR SILICON PHOTONICS
 Er:Al2O3-Si3N4 hybrid slot waveguides
6/22/2022
ALD FOR SILICON PHOTONICS
 Er:Al2O3-Si3N4 hybrid slot waveguides
• Up to 20 dB/cm modal gain
6/22/2022
ALD FOR SILICON PHOTONICS
 Er:Al2O3-Si3N4 hybrid strip waveguides
Er-doped hybrid
waveguide
amplifiers with
multiple spatially
engineered active
layers
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
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
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
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
6/22/2022
Er-doped hybrid waveguides with multiple spatially
engineered active layers
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
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
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
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
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
6/22/2022
BENEQ AT PHOTONICS EUROPE 2022
Beneq® is a leading supplier of
production and research equipment for
atomic layer deposition (ALD) and a
provider of thin film coating services.
www.beneq.com |
info@beneq.com | +358 9 7599 530
firstname.lastname@beneq.com
SCALING-UP
6/22/2022
SCALING-UP
 Myth: ALD is a very slow deposition technique
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
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
BACKUP
6/22/2022
Theoretical modeling
6/22/2022
Theoretical modeling

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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 BENEQ – HOME OF ALD  World’s leading ALD-dedicated company  40+ years of ALD expertise  40+ dedicated ALD systems in operation 24/7  200+ personnel  Divided into two business lines  Advanced ALD • Optics & Photonics • Battery Technology • Part Coating  Semiconductor ALD • Micro- & optoelectronics • Power & RF Devices • MEMS
  • 4. 6/22/2022 BENEQ – HOME OF ALD Research Equipment Beneq R2 Beneq TFS200 Beneq TFS500 Wafer Fabrication Beneq Transform™ 3D & Batch Beneq P400A Beneq P800 Beneq P1500 Spatial ALD Beneq C2R Genesis ALD
  • 5. 6/22/2022 BENEQ – HOME OF ALD  Why ALD?
  • 6. 6/22/2022 BENEQ – HOME OF ALD  Application areas: Microstructures  Integrated waveguides  Cylindrical lenses, Fibers  Structured wafers
  • 7. 6/22/2022 BENEQ – HOME OF ALD  Application areas: Macrostructures  Highly-curved lenses  3D-Structures  Freeform optics
  • 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
  • 13. 6/22/2022 ALD FOR SILICON PHOTONICS  Er-doped Al2O3 with ALD Beneq TFS500 Al C H Er O
  • 14. 6/22/2022 ALD FOR SILICON PHOTONICS  Er-doped Al2O3 with ALD Beneq TFS500 Al C H Er O
  • 15. 6/22/2022 ALD FOR SILICON PHOTONICS  Er-doped Al2O3 with ALD Beneq TFS500
  • 16. 6/22/2022 ALD FOR SILICON PHOTONICS  Er:Al2O3-Si3N4 hybrid slot waveguides
  • 17. 6/22/2022 ALD FOR SILICON PHOTONICS  Er:Al2O3-Si3N4 hybrid slot waveguides • Up to 20 dB/cm modal gain
  • 18. 6/22/2022 ALD FOR SILICON PHOTONICS  Er:Al2O3-Si3N4 hybrid strip waveguides
  • 19. Er-doped hybrid waveguide amplifiers with multiple spatially engineered active layers
  • 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
  • 24. 6/22/2022 Er-doped hybrid waveguides with multiple spatially engineered active layers
  • 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 production and research equipment for atomic layer deposition (ALD) and a provider of thin film coating services. www.beneq.com | info@beneq.com | +358 9 7599 530 firstname.lastname@beneq.com
  • 33. 6/22/2022 SCALING-UP  Myth: ALD is a very slow deposition technique
  • 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