Spoof Plasmon Interconnects—Communications Beyond RC Limit

The inception of spoof surface plasmon polariton (SSPP) mode realized in planar, patterned conductors to manage light beyond diffraction limit at a chosen frequency garnered significant attention of late. We show that, an SSPP channel can be chosen to act in two distinct ways: first, as a regular <inline-formula> <tex-math notation="LaTeX">$RC$ </tex-math></inline-formula> limited electrical interconnect at low frequencies; and second, as an exotic, beyond <inline-formula> <tex-math notation="LaTeX">$RC$ </tex-math></inline-formula> limit communication channel near its resonant frequency by binding the electromagnetic field on its surface to the elimination of capacitance <inline-formula> <tex-math notation="LaTeX">$C$ </tex-math></inline-formula>. A dynamic transformation between these two modes can constitute an energy economic, tera-scale inter-chip hybrid communication network. We have investigated theoretical limits on the information transfer capability of SSPP interconnects. We show that, a geometry dependent tradeoff relation between cross-talk limited bandwidth density and information traveling length emerges in SSPP-based communication networks. According to our analysis, a bandwidth density of 1 Gbps/<inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula> is attainable in SSPP communication network with ~ 10-mm information transfer distance, where each channel can carry ~ 300-Gb/s information with nominal cross-talk.

[1]  Minghui Hong,et al.  Spoof Plasmon Surfaces: A Novel Platform for THz Sensing , 2013 .

[2]  Federico Capasso,et al.  Spoof surface plasmon waveguide forces. , 2014, Optics letters.

[3]  J. Michel,et al.  Electronics and photonics: convergence on a silicon platform , 2007 .

[4]  J. Valentine,et al.  Fiber-to-chip coupler designed using an optical transformation. , 2012, Optics express.

[5]  G. Keiser Optical Fiber Communications , 1983 .

[6]  P. Mazumder,et al.  Bio-Sensing by Mach–Zehnder Interferometer Comprising Doubly-Corrugated Spoofed Surface Plasmon Polariton (DC-SSPP) Waveguide , 2012, IEEE Transactions on Terahertz Science and Technology.

[7]  P. Mazumder,et al.  Active Terahertz Spoof Surface Plasmon Polariton Switch Comprising the Perfect Conductor Metamaterial , 2009, IEEE Transactions on Electron Devices.

[8]  Federico Capasso,et al.  Spoof plasmon analogue of metal-insulator-metal waveguides. , 2011, Optics express.

[9]  Ehsan Afshari,et al.  25.5 A 320GHz phase-locked transmitter with 3.3mW radiated power and 22.5dBm EIRP for heterodyne THz imaging systems , 2015, 2015 IEEE International Solid-State Circuits Conference - (ISSCC) Digest of Technical Papers.

[10]  Y. Urino,et al.  High density optical interconnects integrated with lasers, optical modulators and photodetectors on a single silicon chip , 2013, 2013 Optical Fiber Communication Conference and Exposition and the National Fiber Optic Engineers Conference (OFC/NFOEC).

[11]  Wei-Ping Huang Coupled-mode theory for optical waveguides: an overview , 1994 .

[12]  P. Mazumder,et al.  Analysis of Doubly Corrugated Spoof Surface Plasmon Polariton (DC-SSPP) Structure With Sub-Wavelength Transmission at THz Frequencies , 2012, IEEE Transactions on Terahertz Science and Technology.

[13]  Qiang Cheng,et al.  Broadband and high‐efficiency conversion from guided waves to spoof surface plasmon polaritons , 2014 .

[14]  Gunther Roelkens,et al.  Silicon-Based Photonic Integration Beyond the Telecommunication Wavelength Range , 2014, IEEE Journal of Selected Topics in Quantum Electronics.

[15]  Chao Li,et al.  Review of Silicon Photonics Foundry Efforts , 2014, IEEE Journal of Selected Topics in Quantum Electronics.

[16]  Alyssa B. Apsel,et al.  Analysis of challenges for on-chip optical interconnects , 2009, GLSVLSI '09.

[17]  Mark I. Stockman,et al.  Theory of spoof plasmons in real metals , 2010, NanoScience + Engineering.

[18]  Eby G. Friedman,et al.  On-chip optical interconnect roadmap: challenges and critical directions , 2005 .

[19]  E. Afshari,et al.  Filling the terahertz gap with sand: High-power terahertz radiators in silicon , 2015, 2015 IEEE Bipolar/BiCMOS Circuits and Technology Meeting - BCTM.

[20]  Lingling Sun,et al.  On-chip sub-terahertz surface plasmon polariton transmission lines with mode converter in CMOS , 2016, Scientific Reports.

[21]  Qi Jie Wang,et al.  Designer spoof surface plasmon structures collimate terahertz laser beams. , 2010, Nature materials.

[22]  Shun Lien Chuang,et al.  A coupled mode formulation by reciprocity and a variational principle , 1987 .

[23]  Barry B. Brey The Intel Microprocessors , 2008 .

[24]  Tie Jun Cui,et al.  On-chip sub-terahertz surface plasmon polariton transmission lines in CMOS , 2015, Scientific Reports.

[25]  Qun Jane Gu,et al.  THz interconnect: the last centimeter communication , 2015, IEEE Communications Magazine.

[26]  Hao Yu,et al.  An energy efficient and low cross-talk CMOS sub-THz I/O with surface-wave modulator and interconnect , 2015, 2015 IEEE/ACM International Symposium on Low Power Electronics and Design (ISLPED).

[27]  P. Kapur,et al.  Power comparison between high-speed electrical and optical interconnects for interchip communication , 2004, Journal of Lightwave Technology.

[28]  P. Winzer,et al.  Capacity Limits of Optical Fiber Networks , 2010, Journal of Lightwave Technology.

[29]  P. Dumon,et al.  Efficient fiber to SOI photonic wire coupler fabricated using standard CMOS technology , 2005, 2005 IEEE LEOS Annual Meeting Conference Proceedings.

[30]  Soumitra Roy Joy,et al.  Spoof surface plasmon resonant tunneling mode with high quality and Purcell factors , 2017 .

[31]  David A. B. Miller Attojoule Optoelectronics for Low-Energy Information Processing and Communications , 2017, Journal of Lightwave Technology.

[32]  Y. Arakawa,et al.  First demonstration of high density optical interconnects integrated with lasers, optical modulators and photodetectors on a single silicon substrate , 2011, 2011 37th European Conference and Exhibition on Optical Communication.

[33]  Stefan A Maier,et al.  Terahertz surface plasmon-polariton propagation and focusing on periodically corrugated metal wires. , 2006, Physical review letters.

[34]  Electrodynamics of spoof plasmons in periodically corrugated waveguides , 2016, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[35]  J. Pendry,et al.  Mimicking Surface Plasmons with Structured Surfaces , 2004, Science.

[36]  S. G. Kim,et al.  Integration of silicon photonics into DRAM process , 2013, 2013 Optical Fiber Communication Conference and Exposition and the National Fiber Optic Engineers Conference (OFC/NFOEC).

[37]  Thomas Szkopek,et al.  Plasmonic interconnects versus conventional interconnects: a comparison of latency, crosstalk and energy costs. , 2007, Optics express.

[38]  R. Montoye,et al.  Beyond Moore's Law: the interconnect era , 2004, Computing in Science & Engineering.

[39]  J. Pendry,et al.  Surfaces with holes in them: new plasmonic metamaterials , 2005 .

[40]  D. Miller,et al.  Optical interconnects to electronic chips. , 2010, Applied optics.

[41]  Tie Jun Cui,et al.  Conformal surface plasmons propagating on ultrathin and flexible films , 2012, Proceedings of the National Academy of Sciences.

[42]  Tie Jun Cui,et al.  Planar plasmonic metamaterial on a thin film with nearly zero thickness , 2013 .