Merging multiple microprocessors with high-speed optical networks has been considered a promising strategy for the improvement of overall computation power. However, the loss of the optical communication bandwidth is inevitable when interfacing between optical and electronic components. Here we present an on-chip plasmonic switching device consisting of a two-dimensional (2D) disordered array of nanoholes on a thin metal film that can provide multiple-input and multiple-output channels for transferring information from a photonic to an electronic platform. In this device, the surface plasmon polaritons (SPPs) generated at individual nanoholes become uncorrelated on their way to the detection channel due to random multiple scattering. We exploit this decorrelation effect to use individual nanoholes as independent antennas, and demonstrated that more than 40 far-field incident channels can be delivered simultaneously to the SPP channels, an order of magnitude improvement over conventional 2D patterned devices.
The clock speed of microprocessors has steadily grown over the past few decades, but it has now been saturated at around a few gigahertz. Merging multiple microprocessors has been one of the main strategies employed to increase overall computation power, but the electrical networks connecting the processors have been unable to keep up with the data streams that the individual processors produce. Optical interconnects have been considered potential solutions because optical communication is hundreds of times faster than that of electrical networks. For coupling optics to electronics, surface plasmon polaritons (SPPs) are ideal carriers because they propagate as electromagnetic waves along the dielectric/metal interface and yet induce collective charge oscillations in a metal1,2,3. For this reason, the use of SPPs for on-chip optical interconnects has gained interest in recent years4,5,6,7,8,9,10,11,12, although they have long been applied in biosensing13,14,15,16, lithography17,18,19, subwavelength imaging20,21 and nanomanipulation22,23 due to their subwavelength-scale spatial confinement and strong local field enhancement24.
In designing the SPP-based optoelectronic devices, it is important to implement multi-channel optical inputs to multi-channel plasmonic outputs for the maximized use of optical communication bandwidth. Otherwise, the devices will serve as bottlenecks in the data transfer. However, it is not straightforward to effectively convert the input channels of far-field waves propagating in three-dimensional space to the output channels of the two-dimensional (2D) surface waves. In fact, this dimensional reduction leads to the loss of most input channels upon conversion to output channels. In recent years, various multiplexing methods have been proposed to increase the deliverable channel number. For instance, structures have been designed in such a way that either the directionality25 or the beam shape of the output SPPs is controlled by the polarization23, wavelength26 and intensity patterns of incident waves22. While these studies demonstrated great potential, the number of controllable transmission channels remains small mainly due to the use of periodically ordered structures. In these cases, SPPs generated at each unit cell are replicated at the other unit cells such that they are not independent from one another. While this strategy has been necessary to increase the coupling of incident far-field waves to the SPPs by means of the constructive interference of SPPs generated among unit cells, it is ineffective in the context of transferring input channels to the SPP channels.
In this article, we propose the use of a 2D disordered array of nanoholes patterned on a thin metal film27 to increase the number of transmission channels from far-field optical inputs to plasmonic outputs. Here, the disorder enables the nanoholes distributed across 2D area to act as independent antennas by means of the random multiple scattering of SPPs generated at individual nanoholes. This is clearly distinct from the case of periodically ordered 2D patterns. We prove that the effective number of deliverable channels can be more than 40, an order of magnitude increase in comparison with existing multiplexing methods. With the increased channel number, we demonstrate simultaneous focusing of SPPs at multiple spots, which is equivalent to the implementation of multiple-input and multiple-output (MIMO) networks. In addition, we show the delivery of a 2D far-field image to the SPPs.
Channel loss from optical inputs to plasmonic outputs
In converting the input channels of far-field waves propagating in three-dimensional space to the output channels of the surface waves, there occurs inevitable dimensional reduction that leads to the loss of most input channels. To make it clear, let us take a periodic structure on a thin metal film for an example (Fig. 1a). The number of input channels is given by the number of diffraction-limit spots within the area of illumination, which is given by with L the side length of the pattern, and λ the wavelength of incident wave in free space. On the other hand, the number of output channels for the surface wave is given by the length of the output line divided by half the wavelength, that is, 2L/λSPP with λSPP the wavelength of SPPs. Therefore, the output channels are significantly smaller in number than the input channels. In the case of a periodic structure, the channel conversion efficiency is even worse. There are only one or two output channels because SPPs generated at each unit cell, instead of acting independently, are replicated at the other unit cell.
A simple way to avoid the problem associated with the periodically patterned devices is to use a one-dimensional (1D) array of nanoholes in the metal film (Fig. 1b). Individual nanoholes are scatterers that convert the incoming far-field wave to the SPPs. Therefore, they can act as antennas sending far-field information to the detection channel. One can either choose the phase map of incident wave to individual holes (Fig. 1b)28,29 or design the arrangement of nanoholes30 to focus SPPs at an arbitrary spot where an electronic circuit is to be connected. In this case, however, the maximum number of transmission channels is given by N1D=2L/λ, which is the same in dimension as the SPP channels. Therefore, the dimensional reduction problem remains unsolved.
Deliverable channel number via disordered nanohole array
To increase the number of transmission channels from far-field optical inputs to plasmonic outputs, we propose the use of a 2D disordered array of nanoholes patterned on a thin metal film (Fig. 1c,d) (see Supplementary Note 3 for the possible layout of the optoelectronic networks). The nanoholes distributed across 2D area can act as independent antennas due to the random multiple scattering of SPPs generated at individual nanoholes. This is clearly distinct from the case of periodically ordered 2D patterns. However, the multiple scattering process is problematic because it makes the SPP fields unpredictable at the detection channels (Fig. 1c). However, there is a way to deterministically control these randomly scattered SPPs. We can measure a transfer matrix31,32,33 connecting far-field input to SPP output. From this matrix, the wavefront of an incident wave that would maximize the SPPs at arbitrary target points can be identified. By shaping this wavefront using a spatial light modulator (SLM), it is possible to focus the SPPs at target spots (Fig. 1d). In our study, we defined as the signal-to-noise ratio of intensity at the target spot with respect to the average intensity in the background because this signal-to-noise ratio is determined by the number of independent channels transferred to the detection.
We performed theoretical analysis for the effective number of transmission channels for the 2D disordered array of nanoholes. The SPPs generated at the holes illuminated by a far-field wave experience multiple scattering events on their way to the sampling line (Fig. 1c). The scattering occurs in two different pathways—in-plane scattering which alters the propagation direction of the SPPs and out-of-plane scattering to the far-field waves. In-plane scattering gives rise to the decorrelation of SPPs generated at particular nanoholes with those at the other nanoholes and makes the contribution of individual nanoholes to the detection channels to be independent. Therefore, it plays an important role in increasing the number of effective transmission channels. Out-of-plane scattering works the same way as absorption loss in the sense that the photons disappear from the medium, thereby attenuating the intensity of the SPPs. In fact, we could determine the scattering (ls) and transport (lt) mean free paths of the SPPs propagating through the disordered metal film depending on the size and fill factor of the nanoholes (see Supplementary Note 4), and use these parameters to quantitatively describe the effect of multiple scattering events on the effective number of transmission channels.
As shown in Fig. 1c, the SPPs generated at one slab of illumination gradually become uncorrelated with those at the other slabs as the separation between the slabs increases. Complete decorrelation occurs at the characteristic length lc, which is mainly determined by the diffraction-limit width of the far-field illumination at a high fill factor of the nanoholes. The lc was measured to be 1.0 μm in the experiment and 0.8 μm in the numerical analysis (Supplementary Note 4), close to the width of illumination set by the numerical aperture of 0.6 used in the experiment. Therefore, slabs of width lc can be treated as independent sources, and the 2D disordered array of nanoholes in the area L × L can be considered the combination of individual slabs of width lc. The blue, green and red rectangular areas in Fig. 1c represent these slabs. Effectively, there are m=[L/lc] slabs, where  stands for the floor function which independently contributes to the SPPs at the output channels. Since there are N1D=2L/λSPP independent antennas per slab along the x-direction, the total number of antennas for the entire pattern is given by m × N1D.
The out-of-plane scattering and the metallic loss of SPPs attenuate SPP intensity depending on the distance between the holes to the sampling line, thereby reducing the effective channel number. The decay of intensity takes the form (ref. 34), where la and lt are absorption length due to metallic loss and transport mean free path, respectively, and c is extrapolation length (see the Supplementary Note 4 for experimental and numerical measurements of T(y)). In general, la plays a major role at small y, and lt becomes more important at large y (see the Supplementary Note 4). We defined the effective channel number by the ratio of signal intensity at the target point to the average intensity in the background (signal-to-noise ratio) for SPP focusing:
Here the numerator accounts for the constructive addition of SPP fields at the target point, and the denominator for the incoherent addition of SPPs at points other than the target point. The , the enhancement factor of channel number due to the dimensional increase, is plotted as the blue dots in Fig. 1e as a function of m=[L/lc]. Under the experimental conditions introduced below, the theoretical model predicts αth to be around 9 for L=10 μm and lc=1 μm.
We constructed an experimental setup to measure the transfer matrix from far-field input to SPP output (Fig. 2). The setup is based on a leakage radiation microscope35,36,37, to which we added a reference wave for the recording of the phase and amplitude of the SPPs generated at the air/metal interface. In addition, we installed an SLM in the sample beam path to control the angle of the incident waves to the sample for the measurement of the transfer matrix. The device was also used to shape the wavefront of the incident waves to focus SPPs at target spots. The pixel size of the SLM was 20 × 20 μm2, and the magnification from SLM to the sample plane was 1/444. The number of SLM pixels used for illumination was 230 × 230 to match the 10 × 10 μm2 area where nanoholes were patterned. A quarter-wave plate was installed at the upstream of the SLM to set the polarization of the illumination to be circular to ensure that the scattering angles of SPPs at the holes were isotropic. As a sample, we coated 100 nm-thick Au film on a glass substrate and fabricated a 2D disordered array of nanoholes using a focused ion beam (Fig. 3a). Individual holes measuring 100 nm in diameter filled an L × L=10 × 10 μm2 area with a fill factor ranging from 3 to 15%. Since the channel conversion efficiency was the best at 12% fill factor in our experiment (see Supplementary Note 5), all the data shown in the main text used the 12% samples. The coated layer of the sample faced the condenser lens, and no immersion medium was inserted between the sample and the lens. This set the magnitude of the wavevector of the SPPs generated on the air/metal interface at kSPP=nSPP × k0, where k0=2π/λ with λ the wavelength of the light source in a vacuum (helium–neon laser, λ=633 nm) and nSPP=1.051.
The SPPs generated at the air/metal interface were leaked toward the metal/glass interface and propagated down to the bottom of the glass substrate (nglass=1.515). These leaked SPPs could be picked up by an oil-immersion objective lens because the refractive index of oil (noil=1.515) is larger than nSPP. Due to the boundary conditions, the transverse wavevectors, the component of wavevectors projected to the x–y plane of the leaked SPPs in the glass is equal to the kSPP. Therefore, the azimuthal angle ϕ of the SPP waves at the glass is given by . As a consequence, the SPPs appeared as a circular ring at the conjugate plane of the back focal plane of the objective lens in which the map of the Fourier transform of the transmitted electric field is displayed (inset in Fig. 2). In addition to the SPPs, far-field waves scattered by the nanostructures at the air/metal and metal/glass interfaces were also present. The transverse wavevectors of these waves can range from 0 to nglassk0. Therefore, the far-field waves covered the circular area with a radius corresponding to nglassk0, which is larger than kSPP. However, the high spatial frequency components generated at the metal/glass interface were weak as the incident waves were significantly attenuated there. As such, far-field waves were mostly confined to a circle of radius k0, mostly due to the leakage of scattered waves generated at the holes on the air/metal interface. We placed a circular beam block plate at the conjugate plane of the back aperture of the objective lens to block far-field waves whose transverse wavevector is smaller than kSPP. According to our analysis, the total intensity of the residual far-field waves was ∼10% of the total SPP intensity (Supplementary Note 5). The surface roughness of the metal layer also generated unwanted SPPs and far-field waves, but their contribution was measured to be ∼1% of the total detected wave. An additional lens was positioned at the downstream to relay the SPP map for the sample to the camera (RedLake M3). The view field was 26 × 26 μm2 at the sample plane. A reference wave was linearly polarized along the y-direction and introduced to the camera via a beam splitter to form interference fringes with a sample wave, from which we obtained the phase and amplitude maps of the generated SPPs38.
Experimental demonstration of the increased channel number
We experimentally constructed the transfer matrix by measuring the amplitude and phase maps of SPPs for the illumination of far-field plane waves over a wide angular range. Various angles of illumination (a total of 400) were chosen in such a way that the transverse wavevectors of the plane waves formed a complete basis for the illumination area of 10 × 10 μm2 and a numerical aperture of 0.6. The angle of illumination was set by writing a phase ramp of an appropriate slope and direction on the SLM. From a set of these measurements, we constructed transfer matrix t(η; x, y) which is the complex-field amplitude of SPPs at point η along the sampling line indicated in Fig. 3a for the illumination of a far-field wave at point (x, y) located within the square area of the pattern33,39. (see the Supplementary Note 5 for the representative images and construction of the matrix.)
To confirm that the nanoholes far away from the sampling line can make a significant yet independent contribution to the control of the SPPs, we gradually increased the width of illumination W and investigated the focusing of the SPPs on a target point. For the finite width of illumination W≤L, a submatrix was chosen from the original matrix. A complex field map of illumination E1 was identified that would maximize SPP intensity at a particular target point η=η1 following the equation . Here, η1 is a vector whose element is unity at η=η1 and zero otherwise. Setting an incident wave as E1 would lead to the constructive interference of SPPs originating from the nanoholes at the target point. At points , SPPs would be added incoherently such that the net intensity would be much smaller than at the target point. The ratio of intensity between the focus point and the background will correspond to the effective channel number.
We experimentally demonstrated the focusing of SPPs by writing the phase map of E1 on the SLM and recording the complex field map of the SPPs at the camera. Experiments were performed by increasing W at intervals of 1 μm. Representative images are shown in Fig. 3b–e for W=2, 5, 8 and 10 μm, respectively. The boundary of the 2D pattern is indicated by a white dashed box, and the area of far-field illumination as a red rectangular box. The SPPs were clearly focused at the target point, and the focus became progressively more distinct as the width of illumination increased. From the line profiles along the sampling line (Fig. 4a), we observed that the intensity at the target point significantly increased. The intensity of the SPPs at the target point was plotted as a function of W in Fig. 4b, from which we observed that the intensity increased by almost 100 times at the full width of illumination in comparison with W=1 μm. This confirms that the SPPs arising from nanoholes far away from the sampling line made a significant contribution to the control.
To prove that the effective channel number had increased, we assessed by measuring the signal-to-noise ratio of SPP focusing. As shown in Fig. 4c, the signal-to-noise ratio increased from for W=1 μm to for W=10 μm. Considering that W=1 μm is asymptotically 1D slab, this corresponds to a fold increase in the channel number, confirming the effectiveness of disordered nanoholes in enhancing information transfer capacity. On the other hand, the enhancement factor α was larger than the theoretical expectation. From the analysis of the measured transfer matrix, the characteristic length lc was measured to be ∼1 μm (Fig. 4d). Since the width of the 2D disordered pattern used in the experiment was L=10 μm, the theoretically expected enhancement factor is αth≈9 (Fig. 1e). The discrepancy is mainly due to the relatively imperfect control of incident waves at small W. The shaping of incident waves at a narrow width causes diffraction which interacts with neighbouring holes and generates unwanted SPPs. As a relevant control experiment, we prepared a 1D array of nanoholes and performed the same focusing experiment (see the Supplementary Note 5). Because there were no neighbouring holes along the y-direction for the 1D pattern, the diffraction from the illumination does not generate SPP noise. The experimentally measured signal-to-noise ratio for the 1D pattern was ∼7.6 (the dashed line in Fig. 4c). Therefore, the experimentally observed channel enhancement factor from 1D to 2D patterns was about αexp≈6. The discrepancy between αexp and αth arises mainly due to an approximate residual correlation of 20% (Fig. 4d). When this residual correlation was accounted for (see the Supplementary Note 2 for more details), the theoretically expected enhancement factor was ∼6 (the red dots in Fig. 1e) which was in excellent agreement with the experimental observation.
Experimental demonstration of a MIMO network
With the increased channel number, we can not only switch incoming far-field waves to individual output points at an improved signal-to-noise ratio, but also send them to multiple different spots at the same time. The signal-to-noise ratio of the individual spots in multiple-spot focusing is approximated by the signal-to-noise ratio of single-spot focusing divided by the number of target spots. In effect, the signal-to-noise ratio is shared by multiple spots. Therefore, the transmission channel number to is a critical factor to determine the number of output channels to which information can be transferred with enough signal-to-noise ratio. From the measured transfer matrix, we identified proper incident wave E2 using , where η2 is a unit-amplitude vector whose elements are zero except for the target spots. By writing the phase map of E2 on SLM, we experimentally demonstrated the focusing of SPPs at multiple different spots. The SPP maps are shown in Fig. 5a–c for two, four and six spots, respectively. The square maps displayed at the centre of the images indicate the phase maps of the far-field illumination written on the SLM. Clean focusing was observed even for six spots due to the enhanced effective channel number. To quantitatively assess the signal-to-noise ratio of the focusing, we plotted the intensity of the SPPs along the circle indicated with respect to θ in Fig. 5a. As shown in Fig. 5d–f, the intensity of the individual spots decreased when the number of target spots increased. Because the background noise remained approximately the same, signal-to-noise ratio progressively decreased. The measured signal-to-noise ratio was 20.8, 12.8 and 7.3 for the two-, four- and six-spot focusing, respectively.
Experimental demonstration of image delivery
Finally, we demonstrated the delivery of far-field 2D image information to 1D SPP output channels. As shown in Fig. 6a, a far-field wave Et containing an amplitude pattern resembling a flower was projected onto the disordered array of nanoholes. The SPPs generated by this illumination were sampled along the solid white line forming a square (Fig. 6b). The measured SPPs formed vector ηt, from which we identified Et using . To reduce the noise of reconstruction, we averaged 400 far-field waves with the same amplitude pattern of the flower, but with different phase patterns. Figure 6c shows the reconstructed image which faithfully reproduced the original flower pattern. This confirms that the decorrelation effect of the disordered array of nanoholes enabled the delivery of 2D image information projected to each and every point within the disordered pattern to the 1D SPP sampling line.
We have presented a 2D disordered array of nanoholes on a thin metal film as a MIMO plasmonic switching device. By exploiting the decorrelation of plasmonic waves due to their random multiple scattering, we could convert nanoholes encompassing a 2D area as independent antennas. We demonstrated the transfer of more than 40 far-field input channels to the SPPs which is about an order of magnitude increase in the number of transmission channels with respect to periodically ordered 2D devices. The use of lower loss material than gold such as silver is expected to increase channel capacity even further (see Supplementary Note 6). With the increased transmission channel number, we implemented the simultaneous control of 6 SPP channels at high signal-to-noise ratios. The additional experiments of delivering a 2D image embedded in far-field waves to the SPPs sampled along a 1D line confirmed that the nanoholes distributed across the 2D area indeed acted as independent transmission antennas.
Our method of exploiting the disorder to minimize the effect of the dimensional reduction from far-field waves to surface waves and therefore maximizing the deliverable far-field input channels to the plasmonic output channels will expedite the use of plasmonics in optoelectronic devices5,6,7,8,9,10,11. In particular, we expect that the successful integration of the proposed switching device with multiple electrical circuits will lead to a dramatic increase in the processing speed of complex computational tasks. For the real practices, additional steps may be necessary such as increasing the speed of channel control which can be done by replacing a spatial light modulator with the combination of a high-speed beam scanning device and multiple static phase masks. In the long run, high-end microprocessors can take the advantage of the proposed type of a high-throughput switching device and help a wide range of scientific activities relying on heavy computation.
All relevant data are available from the authors.
How to cite this article: Choi, W. et al. Control of randomly scattered surface plasmon polaritons for multiple-input and multiple-output plasmonic switching devices. Nat. Commun. 8, 14636 doi: 10.1038/ncomms14636 (2017).
Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Engheta, N. Circuits with light at nanoscales: optical nanocircuits inspired by metamaterials. Science 317, 1698–1702 (2007).
Brongersma, M. L. & Shalaev, V. M. Applied physics. The case for plasmonics. Science 328, 440–441 (2010).
Fang, Y. R. & Sun, M. T. Nanoplasmonic waveguides: towards applications in integrated nanophotonic circuits. Light Sci. Appl. 4, e294 (2015).
Ozbay, E. Plasmonics: merging photonics and electronics at nanoscale dimensions. Science 311, 189–193 (2006).
Bozhevolnyi, S. I., Volkov, V. S., Devaux, E., Laluet, J. Y. & Ebbesen, T. W. Channel plasmon subwavelength waveguide components including interferometers and ring resonators. Nature 440, 508–511 (2006).
Burgos, S. P., Lee, H. W., Feigenbaum, E., Briggs, R. M. & Atwater, H. A. Synthesis and characterization of plasmonic resonant guided wave networks. Nano Lett. 14, 3284–3292 (2014).
Huang, K. C. Y. et al. Electrically driven subwavelength optical nanocircuits. Nat. Photonics 8, 244–249 (2014).
Melikyan, A. et al. High-speed plasmonic phase modulators. Nat. Photonics 8, 229–233 (2014).
Heeres, R. W., Kouwenhoven, L. P. & Zwiller, V. Quantum interference in plasmonic circuits. Nat. Nanotechnol. 8, 719–722 (2013).
Wei, H., Wang, Z. X., Tian, X. R., Kall, M. & Xu, H. X. Cascaded logic gates in nanophotonic plasmon networks. Nat. Commun. 2, 387 (2011).
Walters, R. J., van Loon, R. V. A., Brunets, I., Schmitz, J. & Polman, A. A silicon-based electrical source of surface plasmon polaritons. Nat. Mater. 9, 21–25 (2010).
Ou, J. Y., Plum, E., Zhang, J. F. & Zheludev, N. I. An electromechanically reconfigurable plasmonic metamaterial operating in the near-infrared. Nat. Nanotechnol. 8, 252–255 (2013).
Kravets, V. G. et al. Singular phase nano-optics in plasmonic metamaterials for label-free single-molecule detection. Nat. Mater. 12, 304–309 (2013).
Gao, Y. K., Gan, Q. Q., Xin, Z. M., Cheng, X. H. & Bartoli, F. J. Plasmonic Mach-Zehnder interferometer for ultrasensitive on-chip biosensing. ACS Nano. 5, 9836–9844 (2011).
Gopinath, A. et al. Plasmonic nanogalaxies: multiscale aperiodic arrays for surface-enhanced raman sensing. Nano Lett. 9, 3922–3929 (2009).
Feng, J. et al. Nanoscale plasmonic interferometers for multispectral, high-throughput biochemical sensing. Nano Lett. 12, 602–609 (2012).
Srituravanich, W., Fang, N., Sun, C., Luo, Q. & Zhang, X. Plasmonic nanolithography. Nano Lett. 4, 1085–1088 (2004).
Pan, L. et al. Maskless plasmonic lithography at 22 nm resolution. Sci. Rep. 1, 175 (2011).
Chen, X., Yang, F., Zhang, C., Zhou, J. & Guo, L. J. Large-area high aspect ratio plasmonic interference lithography utilizing a single high-k mode. ACS Nano. 10, 4039–4045 (2016).
Wei, F. F. et al. Wide field super-resolution surface imaging through plasmonic structured illumination microscopy. Nano Lett. 14, 4634–4639 (2014).
Kawata, S., Inouye, Y. & Verma, P. Plasmonics for near-field nano-imaging and superlensing. Nat. Photonics 3, 388–394 (2009).
Dvorak, P. et al. Control and near-field detection of surface plasmon interference patterns. Nano Lett. 13, 2558–2563 (2013).
Lin, J. et al. Polarization-controlled tunable directional coupling of surface plasmon polaritons. Science 340, 331–334 (2013).
Novotny, L. & Hecht, B. Principles of Nano-Optics Cambridge University Press (2006).
Lopez-Tejeira, F. et al. Efficient unidirectional nanoslit couplers for surface plasmons. Nat. Phys. 3, 324–328 (2007).
Laux, E., Genet, C., Skauli, T. & Ebbesen, T. W. Plasmonic photon sorters for spectral and polarimetric imaging. Nat. Photonics 2, 161–164 (2008).
Vynck, K., Burresi, M., Riboli, F. & Wiersma, D. S. Photon management in two-dimensional disordered media. Nat. Mater. 11, 1017–1022 (2012).
Gjonaj, B. et al. Active spatial control of plasmonic fields. Nat. Photonics 5, 360–363 (2011).
Seo, E. et al. Far-field control of focusing plasmonic waves through disordered nanoholes. Opt. Lett. 39, 5838–5841 (2014).
Yin, L. L. et al. Subwavelength focusing and guiding of surface plasmons. Nano Lett. 5, 1399–1402 (2005).
Popoff, S. M. et al. Measuring the transmission matrix in optics: an approach to the study and control of light propagation in disordered media. Phys. Rev. Lett. 104, 100601 (2010).
Wang, J. & Genack, A. Z. Transport through modes in random media. Nature 471, 345 (2011).
Kim, M. et al. Maximal energy transport through disordered media with the implementation of transmission eigenchannels. Nat. Photonics 6, 581–585 (2012).
Cai, W., Xu, M., Lax, M. & Alfano, R. R. Diffusion coefficient depends on time, not on absorption. Opt. Lett. 27, 731–733 (2002).
Li, L., Li, T., Wang, S. M., Zhang, C. & Zhu, S. N. Plasmonic airy beam generated by in-plane diffraction. Phys. Rev. Lett. 107, 126804 (2011).
Drezet, A. et al. How to erase surface plasmon fringes. Appl. Phys. Lett. 89, (2006).
Gorodetski, Y. et al. Tracking surface plasmon pulses using ultrafast leakage imaging. Optica 3, 48–53 (2016).
Choi, Y., Yang, T. D., Lee, K. J. & Choi, W. Full-field and single-shot quantitative phase microscopy using dynamic speckle illumination. Opt. Lett. 36, 2465–2467 (2011).
Choi, W., Mosk, A. P., Park, Q. H. & Choi, W. Transmission eigenchannels in a disordered medium. Phys. Rev. B 83, 134207 (2011).
This research was supported by IBS-R023-D1 and the Global Frontier Project (2014M3A6B3063710) through the National Research Foundation of Korea (NRF) funded by the Ministry of Science, ICT and Future Planning. It was also supported by the Korea Health Technology R&D Project (HI14C0748) funded by the Ministry of Health and Welfare, Republic of Korea.
The authors declare no competing financial interests.
About this article
Cite this article
Choi, W., Jo, Y., Ahn, J. et al. Control of randomly scattered surface plasmon polaritons for multiple-input and multiple-output plasmonic switching devices. Nat Commun 8, 14636 (2017). https://doi.org/10.1038/ncomms14636
This article is cited by
Near-field transmission matrix microscopy for mapping high-order eigenmodes of subwavelength nanostructures
Nature Communications (2020)
Nature Reviews Physics (2020)
Scientific Reports (2017)