Controlling light at the nanoscale is of fundamental importance and is essential for applications ranging from optical sensing and metrology to information processing, communications and quantum optics. Considerable efforts are currently directed towards optical nanoantennas that directionally convert light into strongly localized energy and vice versa. Here we present highly directional 3D nanoantenna operating with visible light. We demonstrate a simple bottom-up approach to produce macroscopic arrays of such nanoantennas and present a way to address their functionality via interaction with quantum dots (QDs), properly embedded in the structure of the nanoantenna. The ease and accessibility of this structurally robust optical antenna device prompts its use as an affordable test bed for concepts in nano-optics and nanophotonics applications.
The manipulation of light at the nanoscale requires controlled delivery of the optical radiation to the tightly focused sub-wavelength spot, where conventional optics is fundamentally limited by the diffraction of light1,2. To achieve this, considerable efforts are directed towards optical nanoantennas. The notion of an optical nanoantenna has emerged over the past decade as means of translating the manipulation principles of radio-frequency electromagnetic (EM) radiation to the nanoscale, achieving impressive light control over nanoscale EM landscapes3,4. All-dielectric antennas featured compact dimensions and high directionality have been recently shown at the single nanoparticles' level5,6. More importantly, nanoantennas that use localized surface plasmon resonances (LSPRs) provide new ways to collect, manipulate and deliver light in nanophotonics7,8,9, photovoltaics10 and optoelectronics11. Interestingly, the concepts of radio-frequency antenna design turned out to be applicable to the optical frequency regime. A prominent example of the latter is the adoption of the classical Yagi-Uda antenna to function in the near-IR12,13,14,15,16,17,18,19. An important issue with such direct adoption is the different response of metals in the optical frequency regime (Drude-like)20 that can be, in principle, circumvented by the proper scaling of the nanoantenna material properties21,22. Other limitations include nanoantenna dimensions that frequently surpass the operating wavelength, the intrinsic need of a substrate and/or surrounding polymer matrix on which functional optical elements are fabricated and utilized, and, stemming from the above, the need of non-trivial experimental strategies to actually couple or decouple near-field signals to or from such nanodevices.
Here we bring forward a 3D nanoantenna that operates in the visible regime with high directivity. Different from the 3D plasmonic nanoarchitectures for THz domain23,24,25, here we have all functional elements available to efficiently couple, in practice, the local optical emitters. These nanoantennas are easily produced in a macroscopic array format using affordable bottom-up nanofabrication – hole-mask colloidal lithography (HCL).
There are three basic elements of this nanoantenna, which we designate as ‘I’, ‘II’ and ‘III’,followed by their sequential increase in size (Fig. 1A). Each element is a metal nanodisk, supporting a LSPR, which is separated from the neighboring elements by a dielectric spacer. Directional emission or reception is realized into free-space, which is faced by the smallest element (I) of the device. The dimensions of the dielectric spacers are in-line with the size of the functional elements, making this nanoantenna-type rather compact. Such design can be experimentally realized by HCL – a bottom-up nanofabrication based on colloidal self-assembly (see Experimental Section)26,27. Short-range ordered arrays of nanoantennas typically span over cm2 and can be produced on a large variety of substrates – here we choose regular microscope glass slides, with antenna elements made of Au, spaced by silica (c.f. scanning electron microscopy (SEM) image on Fig. 1B, featuring both the overall shape of the nanodevices (left) and resolved plasmonic elements (right)). The design structure is verified by optical reflectance and transmittance and by simulating the near-fields with finite-difference time-domain (FDTD) numerical calculations (Fig. 1C)27,28. Whereas transmittance through the nanoantenna array is directionless due to reciprocity (red solid and dashed curves in Fig. 1C) and displays three basic spectroscopic features (marked ‘ra’, ‘rb’ and ‘rc’ in Fig. 1C), the reflectance shows remarkable asymmetry with respect to the direction of incidence (compare black solid and dotted curves in Fig. 1C). This asymmetry is most pronounced in the visible and near-IR. While electrodynamics simulations overall match the far-field optical spectra (light red curve in Fig. 1C, calculated for the structure with the elements of 200 nm, 120 nm and 50 nm and corresponding thickness of 20 nm, spacer 50 nm), the detailed nature of the spectral features can be identified with simulated near-field plots (inset of Fig. 1C). In the FDTD simulations, the effective refractive index for the surrounding medium is n = 1.25, which partially addresses the substrate influences on the LSPRs of the nanodisks and their optical interactions in the proposed nanoantenna. However, the slight discrepancies between the measurements and calculations (see Fig. 2C) might be assigned to the substrate effects. From these we mark that back illumination allows addressing sequentially elements II and III as we move along the spectra towards longer wavelengths (lower row of Fig. 1C inset, note that the element I is hardly ever excited this way). Front illumination largely features elements, addressed simultaneously in pairs (I–II and II–III as followed the top row of the Fig. 1C inset from 630 nm to 940 nm plot). Note also that while the best near-field signal is normally produced at the lateral sides of the elements, a sizable EM field enhancement exists between the elements and on top of the nanoantenna in the visible.
The present nanoantenna measures roughly one third of the operating wavelength in all three dimensions. Such compact configuration allows the three elements to be electromagnetically coupled in all regimes, namely at the near-, intermediate- and far-field. This distinguishes the present case from so far reported multi-element optical nanoantennas, particularly inspired by the low-frequency Yagi-Uda concept, where functional elements are spatially separated, individually addressed and provide an antenna' directionality function due to the far-field coupling12,15. The EM interactions in the near- and intermediate-field regimes are predominant because of the compact configuration in the present case. These strong optical interactions trigger new hybridized plasmonic resonances in the structure, similar to those observed in strongly coupled nanoplasmonic geometries29,30,31.
To address the performance of this nanoantenna in the directional near- to far-field conversion, we turn to the quantum dots (QDs) that have been previously used to feed nanoantennas elements15. As mentioned earlier, the highest EM field enhancement is produced at the sides of the nanoantenna elements due to the largely dipolar character of the involved plasmonic resonances. We choose, however, to embed QDs into the dielectric spacers between the elements to preserve the robustness of the design with the outlook for possible applications in integrated nanophotonics. We introduce CdSe QDs (excitation – at 532 nm, emission – at 625 nm) on top of element I, embedded in a silica layer (schematics inset in Fig. 2A). Exciting QDs with a laser (for the schematics of the experimental setup – see Fig. S1), we further detect free-space propagating light (Fig. 2A) at the characteristic emission line of the employed QDs, peaking at around 625 nm that overlaps with the ‘ra’ resonance of element I. Note that this resonance is detected as a shoulder-like feature in transmittance (Fig. 1C). Such emission is characterized by a forward-to-backward (F/B) directionality that effectively surpasses 10 dB (Fig. 2B). The directionality stays rather constant in the entire emission range (Fig. 2B), which suggests that it is the light produced by the QDs emission that is further processed by the nanoantenna and is beamed as a directional free-space EM radiation. The directional emission pattern is further corroborated by the emitted intensity' polar plots, both experimental and calculated with FDTD (Fig. 2C). It is instrumental to follow the emergence of such strong directionality by constructing one- or two-element nanoantennas and combining them with the QDs at different wavelengths. The QDs that emit light at 625 nm and 780 nm were similarly used to ‘feed’ one-element (Figs. S2 A, C, D) and two-element (Figs. S2 B, E, F) configurations. Whereas one-element conventional dipolar plasmonic nanodisk antennas show largely bidirectional light emission (see insets in Figs. S2 C, D, note also the stronger emission enhancement for the case of 780 nm QDs, which are better spectrally tuned to the resonance of the sole nanoantenna element – Fig. S2 A), two-element nanoantennas already feature a promising F/B-directionality on the order of 3 dB (see insets in Figs. S2 E, F). Due to the strongly near-field-coupled response of the nanoantenna elements, properly matching local emitters spectrally to a selected one of the three resonances promotes the strong directionality of the emitted radiation. The local EM field enhancement pattern should be taken into account for the best coupling to a selected resonance. By using the quantum emitter at 780 nm, that is – matching the ‘rb’ resonance of the nanoantenna – the far-field propagating light receives similar directionality. This can be followed in Fig. 3. Fig. 3A shows the far-field spectral response of the antenna sample immersed in refractive index matching oil. This makes ‘ra’, ‘rb’ and ‘rc’ resonances to redshift to 660 nm, 787 nm and 1055 nm, respectively (compare to Fig. 1C). With ‘rb’ resonance positioned now close to the QDs emission peak, the F/B ratio of emission remains ∼ 10 dB around the peak, as shown in Fig. 3B. Additionally, we mark here a sizable decrease in the emission intensity (compare to Fig. 2A, for example).
The enhancement of the QDs emission and its connection to the directionality for this class of nanoantennas can be followed in Fig. 4. Keeping the wavelength of the QDs fixed (625 nm, Figs. 4A, C and 780 nm, Figs. 4B, D), we experimentally raster the positioning of these ‘feeding elements' through the nanoantenna stack. The best near-field coupling and directionality for the 625 nm QDs is achieved when they are positioned above element I (compare Fig. 2A with Figs. 4A and 4C, insets – wavelength-dependent directionality plots). For 780 nm QDs, the best directionality is realized when they are similarly positioned above the element I (Fig. 3B), but the best light emission enhancement is attained when the emitters are above element II instead (Fig. 4B). Note that the latter scenario provides poorer emission directionality on the order of 3–5 dB (inset of Fig. 4B). The plasmonic resonant modes here can be easily manipulated by varying the number of elements, inter-element spacing, their aspect ratios and the surrounding refractive index medium. Additionally, the positioning of the feeding sources and thus the choice of the feeding strategy are flexible due to the possibility to directly address any of the nanoantenna elements.
Though fabricated on a supporting substrate, this plasmonic nanoantenna can in principle be lifted from the substrate32,33, and, as the QDs are tightly embedded in the structure, we envision that the directional emission will be preserved. This also suggests that due to its 3D-articulated structure, the role of the substrate is inferior for the nanoantenna integrity and function – similarly to semi-shells32 standard transfer with, for example, a polydimethylsiloxane (PDMS) stamp, would provide a substrate-free array of these nanodevices. Of further practical interest, denser HCL-produced arrays of nanodisks display an exciting interplay between far-field coupling and near-field ‘hot-spot’ patterns12. It is reasonable to foresee that in the present array increasing the density might result in unexpected effects on directionality and functionality of the whole platform. Another facet of the potential functionality of these devices is highlighted in the context of the currently rising research theme of nanoantenna-enhanced processes23,34. Excitingly, the outlined nanoantennas class can be readily adopted for such development35. Overall, this practical model nanoantenna system paves the way for the development and engineering of novel nanophotonic devices aiming at tailoring the optical radiation at a nanoscale. And with the ease of serial bottom-up nanofabrication, such potential devices can be straightforwardly tested and adopted.
The nanoantennas were fabricated using the HCL method26, a versatile and cost-efficient method that facilitates the fabrication of short-range-ordered arrays of nanostructures on various surfaces. Briefly, PMMA (Microchem Coorporation, 4 wt% diluted in anisole, MW = 950000) was spin-coated on cleaned glass and baked at 110°C for 10 min to form a ∼ 200 nm thick film. Oxygen plasma (50 W, 5 s, 250 mTorr, Plasma Therm Batchtop RIE 95 m) was then applied to produce a hydrophilic surface. An aqueous solution of poly(diallyldimethylammonium chloride) (PDDA, 0.2 wt%, MW 200000–350000, Sigma Aldrich) and a suspension of sulfate polystyrene (PS) nanobeads (0.2 wt%, nominal diameter ∼ 150 nm, Invitrogen) were sequentially drop casted on the sample for 30 s, each rinsed by ultrapure water and dried by purified N2. A short-range ordered array of PS nanobeads on the PMMA film was thus obtained. A thin gold film (10 nm) was thermally evaporated on the sample as a sacrificial mask, followed by tape-striping to remove the PS nanobeads. PMMA underneath the nanoholes in the gold film was adequately removed using O2 plasma etching. Desired materials were then deposited and arrays of nanodisks were obtained after liftoff in acetone. The sequence of materials deposition for the ultracompact nanobeamers was determined as follows: 20 nm gold, 50 nm SiO2, 28 nm gold, 50 nm SiO2 and 30 nm gold. Between each two layers, 1 nm Ti was deposited to improve adhesion. Note that the size and thickness of the gold disks can be freely changed to tune the resonance of the elements to match the QDs emission.
Streptavidin conjugated CdSe quantum dots were purchased from Invitrogen. A 5 nm SiO2 thin film was deposited on the desired gold disk as a dielectric spacer to avoid fluorescence quenching of the QDs. The sample was then taken out from the evaporator chamber and etched by O2 plasma at 50 W for 10 s to produce hydrophilicity. A droplet of diluted QDs solution (∼3 × 10−8 M, which arithmetically assures a monolayer of QDs on the whole area of a sample of ∼ 1.5 × 2.0 cm2) was drop casted on the sample, dried in air and immediately gently rinsed by ultrapure water and dried by N2. The sample was then transferred back to the evaporator chamber for deposition of the other materials. If the QDs are on the top gold disk, a 15 nm SiO2 film was deposited to embed the QDs.
T and R measurements
Transmission and reflection measurements were carried out on a Cary 5000 UV-vis-NIR spectrophotometer (Agilent). A specular reflection accessory was used for reflection measurements.
QDs emission measurements
QDs emission spectra at different angles were measured using a home-made setup (see experimental schematic in Fig S1). Samples were excited by a 532 nm laser (Millennia Pro, Spectra-Physics) slightly focused (half-cone angle ∼ 6°) on the front side with the nanobeamers. The incident angle was fixed at 45 degrees. A fiber-coupled spectrometer (Ocean Optics QE5000) mounted on a rotation stage was used to measure the emission spectra at different angles (−90° ∼ 90°). A notch filter (NF532) was used in front of the collection fiber to remove the elastic scattering of the laser.
Directionality plot calculations with FDTD
The nanobeamer is properly excited by a single oscillating electric Hertzian-dipole that is situated on top of the smallest element, according to the experimental realization. The radiation pattern of the dipole is strongly modified due to the excitations and interactions of the LSPRs in the nearfield28. The radiation pattern of the dipole is calculated based on the Huygens' principle, connecting the calculated near-field to the far-field. That is, at any operating wavelength and polar angle, the radiated optical intensity is calculated.
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A.D. acknowledges the support from Swedish Research Foundation, L.T. acknowledges financial support from the EU FP7 project “PRIMA” – 248154. We thank Dr. Randy Dumas for the careful proof-reading of the manuscript.
The authors declare no competing financial interests.
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Tong, L., Pakizeh, T., Feuz, L. et al. Highly directional bottom-up 3D nanoantenna for visible light. Sci Rep 3, 2311 (2013). https://doi.org/10.1038/srep02311
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