BLACK Semiconductor The Photonics Platform for any Electronic Chip - NMWP
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2020-06-14-01 BLACK Semiconductor The Photonics Platform for any Electronic Chip Daniel Schall - NMWP Innovation 2 GO Webinar 18.06.2020
Computer performance development comes to halt amount of data explodes Data curve from IDC/EMC Digital Universe reports 2008-2017, Compute curve HPE analysis, Graphic: World Economic Forum https://www.weforum.org/agenda/2018/09/end-of-an-era-what-computing-will-look-like-after-moores-law/ © Black Semiconductor 2020 4
Chip design cost explode Source: International Business Strategies (IBS) © Black Semiconductor 2020 5
New applications - how? Datacenter 5G Infrastructure Datarate ↑ ↑ Datarate Price ↓ ↓ Price Energy consumption ↓ ↓ Energy consumption Artificial Intelligence Autonomous driving Computation speed ↑ ↑ Computation speed Energy consumption ↓ ↑ Datarate © Black Semiconductor 2020 6
Brain vs computer Brain Fastest Supercomputer: IBM Summit Instructions per second1 20 x 1015 143.5 X 1015 Elements2,3 87 billion neurons 9,216 CPUs (8 billion transistors) 100 trillion synapses 27,648 GPUs (21.1 billion transistors) 470 terabyte storage4 657 trillion transistors 250 petabyte storage Power consumption2,3 20 Watt 13 mega Watt 1) https://en.wikipedia.org/wiki/Computer_performance_by_orders_of_magnitude 2) https://en.wikipedia.org/wiki/Brain Billion = 109 3) https://en.wikipedia.org/wiki/Summit_(supercomputer) 4) 10.7554/eLife.10778 Trillion = 1012 © Black Semiconductor 2020 7 Pictures: www.artitout.com and Oak Ridge National Laboratory/IBM
Problem: chip IO and process speed Today‘s electronics needs a major upgrade! © Black Semiconductor 2020 8
Why Photonics Photonics enables data transfer and processing at speed of light Transfer speeds are a major bottleneck in computing New applications like autonomous cars require these faster data rates Traditional interconnects are too slow for modern use cases AI development is currently limited by data transfer and process speed Faster processing is required for unleashing AI applications Peng et al “Neuromorphic Photonic Integrated Circuits“, JSTQE 24, 6 (2018) © Black Semiconductor 2020 9
Solution: Universal 3D Photonic Platform #2: photonic platform, Monolithic Fabrication #1: any electronic circuit, Free choice of technology © Black Semiconductor 2020 10
State Of The Art: Planar CMOS & Si Photonics Nature 556, 349 (2018) © Black Semiconductor 2020 11
Comparison: 3D vertical vs planar New Current Photonics: waveguide, Graphene modulators, detectors VIA Planarization on CMOS BEOL CMOS Nature 556, 349 (2018) Major difference: 3D vertical vs planar architecture ► higher performance compared to Si due to integrated graphene devices ► electronics and photonics technologically seperated ► smaller footprint due to 3D integration ► integration on any CMOS electronics, no dedicated photonics & CMOS technology © Black Semiconductor 2020 12
III-V semiconductor integration Die attach Membrane transfer printing Bonded III-V dies Si Wafer 4” Si wafer 3” III-V membrane 200 or 300 mm Lou et al, Front. Mater., 07 April 2015 Yuqing, et al. "Indium phosphide membrane nanophotonic integrated circuits on silicon." physica status solidi (a) 217.3 (2020): 1900606 Alternative literature: Zhang et al. III-V-on-Si photonic integrated circuits realized using micro-transfer- printing APL Photonics 4, 110803 (2019) Hiraki et al. Heterogeneously integrated III–V/Si MOS capacitor Mach–Zehnder modulator. Nature Photon 11, 482–485 2017 © Black Semiconductor 2020 13
Solution: Universal 3D Photonic Platform #2: photonic platform, Monolithic Fabrication #1: any electronic circuit, Free choice of technology © Black Semiconductor 2020 14
Why Graphene Photonics? Material Fabrication and integration Photon • Fast carrier dynamics: ultrafast devices • Linear band structure: broadband devices • Fabrication on large sacle • Low density of states: efficient devices • BEOL integration ► Ultra fast, efficient and broadband photonic devices on wafer scale © Black Semiconductor 2020 15
Device schematic Waveguide Graphene modulator = capacitor Contact pads Optical IN detector = resistor Optical OUT Background: electron microscope picture of graphene on waveguide © Black Semiconductor 2020 16
Graphene Photonics Platform Efficient Phase Shifters Efficient Modulators Graphene Waveguide Ultrafast Photodetectors D. Schall et al., ACS Photonics 1 (9), 781-784 (2014). D. Schall, et al., J. Phys. D: Appl. Phys., (2017). S. Schuler et al., Nano Lett., 16 (11), 7107-7112 (2016). Contact D. Schall et al., Opt. Express 24, 7871-7878 (2016). M. Mohsin et al., OSA paper IM4A.1 (2015). M. Mohsin et al Scientific Reports 5, 10967 (2015). M. Mohsin et al., Opt. Express 22, 15292-15297 (2014). Mohsin, Schall et al. Opt. Express 25, 31660-31669 (2017) © Black Semiconductor 2020 17 D. Schall et al., OFC San Diego (2018).
Fabrication flow Start: Simulation Photonic layer Graphene integration waveguide Si waveguide On-wafer EO Fabricated devices Graphene on Si characterization waveguides Graphene devices © Black Semiconductor 2020 18
6“ Graphene Line 100 Ω 1Ω 2048 Photodetectors on one wafer 50 Ω +/-20%: 60% OK 100 Ω threshold: 80 % OK 200 Ω threshold: 88% OK 500 Ω threshold: 90 % OK © Black Semiconductor 2020 19
Proof of Concept Photodetector Data transmission at 56 Gb/s More than 130 GHz bandwidth 5 ps AMO and CNIT unpublished (2018) Schall et al. OFC (2018) Data rate limited by equipment. © Black Semiconductor 2020 20
First demonstration: Graphene link @ 25 Gb/s MZI graphene modulator EDFA graphene detector AMO, CNIT, Ericsson, Nokia (Mobile World Congress 2018) © Black Semiconductor 2020 21
Photonic Platform b) a) Light coupling section grating coupler c) BEOL devices waveguide device 6” wafer with BEOL photonic devices; mockup, no electronics d) © Black Semiconductor 2020 22
Our Customer‘s Markets Datacenter Chips 2025 €15 B (Allied Market Research Jan 2019) 5G Infrastructure 2027 €45 B (Research and Markets 2019) AI Chip Market 2024 €27 B (Forecast Intel 2019) Automotive Chip Market 2025 €52 B (Research and Markets 2018) © Black Semiconductor 2020 23
Commercial Graphene Photodetectors Long term testing Data transmission at 14 Gb/s Limited by pattern generator Graphene Photodetector © Black Semiconductor 2020 24
Graphene Photodetector to be released soon
Technology Partner Applied Micro and Opto-Electronics, AMO GmbH Managing Directors: Prof. Dr.-Ing. Max Christian Lemme Key Facts Dr. Michael Hornung • High-Tech Research Foundry (non-profit) Key Technologies • Close ties to RWTH Aachen University • Silicon technology • 500 m2 clean room • Nanofabrication (Stepper, NIL, E-Beam, IL) • ~60 staff members • New materials integration (high-k/metal gate, graphene, 2D Key Applications materials, perovskites) • Nanoelectronics • Nanophotonics • Integrated sensors © Black Semiconductor 2020 26
AMO‘s Graphene Research Milestones First commercial First Top-Gate Photodetector Photodetector Graphene- Monolithic 3D Transistor WR: 43 GHz WR: 130 GHz Photodetector Integration Start 6“ Graphene Graphene Photonic Pilotlinie Start Photonics Graphene First reseach waveguide photodetector 2006 2007 2009 2011 2014 2015 2017 2018 2019 2020 + © Black Semiconductor 2020 27
Acknowledgements to contributors in the last 10 years ALL AMO EMPLOYEES contributed at least indirectly with their knowledge and work. Everyone contributes to keeping the cleanroom running and developing IP. Thank YOU. Directly contributed: We would like to say thank you for giving us the opportunity to draw on 20 years of experience in CMOS, Abbas Madani photonics, and graphene research projects at AMO in Aachen, Germany. Abhay Sagade Andreas Umbach Anna Lena Giesecke Bart Szafranek Bartos Chmielak Bernhard Junginger Bernhard Wasmayr Burkhard Grudnik Caroline Porschatis Christopher Matheisen Daniel Neumaier Galip Hepgüler Heinrich Kurz Holger Lerch Martin Otto Max Lemme Mehrdad Shaygan Muhammad Mohsin Jens Bolten Sebastian Schall Stefan Wagner Stephan Suckow Thorsten Wahlbrink Tobias Plötzing Vimoh Shah Wolfgang Kuebart © Black Semiconductor 2020 28
Excited? Get in touch for further information: CEO: Daniel Schall - daniel.schall@blacksemicon.de +49 241 916 074 20 CFO: Sebastian Schall - sebastian.schall@blacksemicon.de +49 241 916 074 21 © Black Semiconductor 2020 29
BLACK Semiconductor The Photonics Platform for any Electronic Chip
Additional information © Black Semiconductor 2020 31
Waferscale Photodetector on Si SOTA Responsivity Bandwidth Data rate Wavelength Type (A/W) (GHz) Gb/s nm 0.2 1480 to 1620 Graphene [1] >130 56 (gated 2 A/W) and 1980 Graphene/plasmonic 0.5 >110 100 [2] Graphene [3] 0.36 >110 40 Ge on Si [4] 0.8 – 0.9 120 56 1) Schall et al. OFC (2018) 2) Ma et al. ACS Photonics 6, 154 (2019) 3) Ding et al. arXiv:1808.04815v3 (2018) 4) Vivien et al. Optics Express 20, 1096 (2012) © Black Semiconductor 2020 32
Absorption Modulator on Si SOTA Modulation Attenuation Modulation/ Length Bandwidth Data rate Type (dB) (dB) Attenuation (µm) (GHz) Gb/s Graphene [1] 16 3 5 300 0.7 - (DC device) Graphene [2] 1.3 20 0.07 120 29 50 Graphene 16 15 50 - Simulation Ge on Si [3] 4.6 4.1 1.1 40 >50 28 1) M. Mohsin et al. Optics Express 22, 15292 (2014) 2) Giambra et al., Optics Express 27, 20146 (2019) 3) S. Gupta et al. OFC (2015) © Black Semiconductor 2020 33
MZI Modulator SOTA α loss VπLα BW Data rate Modulator Type VπL (Vmm) length (µm) (dB/mm) (dBV) (GHz) (Gb/s) Si depletion vertical pn [1] 26.7 1.04 27.8 4000 25.6 50.1 Si depletion vertical pn [2] 7.5 2.25 16.9 2000 30.5 40 Si depletion vertical pn [3] 20 4.6 92 750 27.7 60 SISCAP [4] 2 6.5 13 400 40 III/V on Si [5] 0.9 2.6 2.3 250 2.6 32 Graphene [6] 2.8 23.6 62 300 5 10 Graphene [7] 2.7 8.7 24 RR (17µm) - Graphene simulation [7,8] 0.8
Graphene: tunable absorption cross section 3D view Absorption in dB/µm Absorption in dB/µm 500 nm 0.5 * Ephot Chemical potential µc EF 0.5*Ephot X § λ = 1550 nm → Ephot = 0.8 eV 0.5*Ephot EF § For |µc| ≥ 0.5 * Ephot states are blocked Ephot → graphene is transparent Absorbing Transparent © Black Semiconductor 2020 35 M. Mohsin et al. Scientific Reports 5,10967 (2015)
Tunable refractive index cross section 3D view Effective refractive index Effective refractive index 500 nm 0.5 * Ephot Chemical potential § λ = 1550 nm → Ephot = 0.8 eV § Kramers-Kronig relates the absorption to the refractive index → refractive index is a function of the electro chemical potential © Black Semiconductor 2020 36 M. Mohsin et al. Scientific Reports 5,10967 (2015)
Absorption and Phase Modulator cross section 3D view Effective refractive index and absorption Effective refractive index Absorption in dB/µm 500 nm Phase mod Amplitude mod § Refractive index and absorption depend on the chemical potential § high mobility gives low absorption for µ < -0.4 eV preferred for phase modulators. Phase and absorption modulator realizable © Black Semiconductor 2020 37 M. Mohsin et al. Scientific Reports 5,10967 (2015)
Ultrafast Carrier Dynamics in Graphene Cooling: 1.3 ps EF Excitation Ephot Heating: 50 fs photon Tielrooij et al Nature nanotech 10 (2015) © Black Semiconductor 2020 38
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