Data transmission in long-range dielectric-loaded surface plasmon polariton waveguides

Kharitonov, Svyatoslav; Kiselev, Roman; Kumar, Ashwani; Ruiz, Ivan Fernández de Jáuregui; Shi, Xueliang; Leósson, Kristján; Pertsch, Thomas; Nolte, Stefan; Bozhevolnyi, Sergey I.; Chipouline, A.

doi:10.1364/oe.22.026742

Cited by 6 publications

(4 citation statements)

References 22 publications

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“…Usually, BERs of 10 −12 to 10 −15 are achieved for telecommunication links after forward-error correction ( 45 ). To characterize the components used in a transmission link, the BER penalty is used, describing the change in the BER introduced by the component under test, when compared to an element that introduces a similar amount of optical loss without distorting the signal ( 46 ). …”

Section: Resultsmentioning

confidence: 99%

“…6B) for several input powers. The evaluation of the latter finally gives us the decision threshold x 0 and the BER of the system under the current conditions ( 46 ), plotted with the red dots in Fig. 6A as a function of the received power.…”

Section: Resultsmentioning

confidence: 99%

“…( 46 ), was used. The optical signal was generated from the transmitter part, and the signal was guided by an optical setup to the sample.…”

Section: Methodsmentioning

confidence: 99%

“…In the optical modulation tests, a typical prototype of a fiber optic telecommunication line, as described by Kharitonov et al (46), was used. The optical signal was generated from the transmitter part, and the signal was guided by an optical setup to the sample.…”

Section: High-frequency Measurement Setupmentioning

confidence: 99%

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High–bit rate ultra-compact light routing with mode-selective on-chip nanoantennas

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Section: Resultsmentioning

confidence: 99%

Section: Resultsmentioning

confidence: 99%

“…( 46 ), was used. The optical signal was generated from the transmitter part, and the signal was guided by an optical setup to the sample.…”

Section: Methodsmentioning

confidence: 99%

Section: High-frequency Measurement Setupmentioning

confidence: 99%

See 2 more Smart Citations

High–bit rate ultra-compact light routing with mode-selective on-chip nanoantennas

et al. 2017

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Aluminum plasmonic waveguides co-integrated with Si3N4 photonics using CMOS processes

Dabos

Manolis

Tsiokos

et al. 2018

Sci Rep

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Co-integrating CMOS plasmonics and photonics became the “sweet spot” to hit in order to combine their benefits and allow for volume manufacturing of plasmo-photonic integrated circuits. Plasmonics can naturally interface photonics with electronics while offering strong mode confinement, enabling in this way on-chip data interconnects when tailored to single-mode waveguides, as well as high-sensitivity biosensors when exposing Surface-Plasmon-Polariton (SPP) modes in aqueous environment. Their synergy with low-loss photonics can tolerate the high plasmonic propagation losses in interconnect applications, offering at the same time a powerful portfolio of passive photonic functions towards avoiding the use of bulk optics for SPP excitation and facilitating compact biosensor setups. The co-integration roadmap has to proceed, however, over the utilization of fully CMOS compatible material platforms and manufacturing processes in order to allow for a practical deployment route. Herein, we demonstrate for the first time Aluminum plasmonic waveguides co-integrated with Si3N4 photonics using CMOS manufacturing processes. We validate the data carrying credentials of CMOS plasmonics with 25 Gb/s data traffic and we confirm successful plasmonic propagation in both air and water-cladded waveguide configurations. This platform can potentially fuel the deployment of co-integrated plasmonic and photonic structures using CMOS processes for biosensing and on-chip interconnect applications.

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Interference and wave propagation in a plasmonic Al2O3-Au-Al2O3 ridge waveguide

Yankovskii

Kornienko

Shaimanov

et al. 2020

J. Phys.: Conf. Ser.

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Performance of plasmonic ridge waveguides of different length formed on fused silica substrates has been studied experimentally and theoretically. All the waveguides were single-mode ones, had a width of 70 μm, and their cross-section had a structure of Al2O3-Au-Al2O3 sandwich–10 nm-thick Au film deposited between 240 nm- and 70 nm-thick Al2O3 top layer and bottom layers. To shape sidewalls, the wave guiding sandwich was etched through its depth. The waveguides were terminated by 1D gratings etched in the sandwich for light coupling/decoupling. The optimized input grating had an elliptical shape for focusing plasmon waves upon excitation, and the output grating was a conventional one. It was found that the traveled plasmonic waves decoupled and visualized themselves as interference patterns in the output grating area. We study propagation of these waves for a set of waveguides with lengths of 0.5-1 mm and demonstrate their main characteristics–the propagation length and attenuation factor.

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Data transmission in long-range dielectric-loaded surface plasmon polariton waveguides

Cited by 6 publications

References 22 publications

High–bit rate ultra-compact light routing with mode-selective on-chip nanoantennas

High–bit rate ultra-compact light routing with mode-selective on-chip nanoantennas

Aluminum plasmonic waveguides co-integrated with Si3N4 photonics using CMOS processes

Interference and wave propagation in a plasmonic Al2O3-Au-Al2O3 ridge waveguide

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