A protocol for the colloidal synthesis of silver nanocubes and fabrication of plasmonic nanoscale patch antennas with sub-10 nm gaps is presented.
We present a method for colloidal synthesis of silver nanocubes and the use of these in combination with a smooth gold film, to fabricate plasmonic nanoscale patch antennas. This includes a detailed procedure for the fabrication of thin films with a well-controlled thickness over macroscopic areas using layer-by-layer deposition of polyelectrolyte polymers, namely poly(allylamine) hydrochloride (PAH) and polystyrene sulfonate (PSS). These polyelectrolyte spacer layers serve as a dielectric gap in between silver nanocubes and a gold film. By controlling the size of the nanocubes or the gap thickness, the plasmon resonance can be tuned from about 500 nm to 700 nm. Next, we demonstrate how to incorporate organic sulfo-cyanine5 carboxylic acid (Cy5) dye molecules into the dielectric polymer gap region of the nanopatch antennas. Finally, we show greatly enhanced fluorescence of the Cy5 dyes by spectrally matching the plasmon resonance with the excitation energy and the Cy5 absorption peak. The method presented here enables the fabrication of plasmonic nanopatch antennas with well-controlled dimensions utilizing colloidal synthesis and a layer-by-layer dip-coating process with the potential for low cost and large-scale production. These nanopatch antennas hold great promise for practical applications, for example in sensing, ultrafast optoelectronic devices and for high-efficiency photodetectors.
In recent years, colloidal synthesis of nanoparticles and the assembly of these into advanced structures have attracted great interests both in research and industrial developments.1-4 Colloidal synthesis of nanoparticles have several advantages over lithographically fabricated nanostructures including superior size homogeneity, low cost and the possibility of large-scale, parallel production.
Metal nanoparticles such as silver (Ag) and gold (Au) can support localized surface plasmon polaritons and have the ability to confine light in a volume much smaller than the diffraction limit.1,3-5 The resulting high field intensity creates an enhanced local density of states enabling light-matter interactions to be tailored at the nanoscale. Recent efforts have demonstrated procedures to synthesize Ag and Au nanoparticles in a wide range of sizes and shapes, including triangles,4,6 cages,3,4 and rods4,7,8 in addition to the nanocubes discussed here. Nanostructures composed of several Ag or Au nanocomponents have also been fabricated demonstrating tailored properties.1,9-11
Here, we demonstrate a procedure to synthesize Ag nanocubes and more importantly, to couple these Ag nanocubes with an underlying Au film in order to form plasmonic nanopatch antennas. The distance between Ag nanocubes and the Au film can be controlled with ~1 nm resolution by using a series of polyelectrolyte spacer layers. We also demonstrate how to incorporate an active medium, such as an organic dye, into the plasmonic nanopatch antennas. Due to the strongly confined electromagnetic fields in the gap region between the nanocubes and the Au film, the nanopatch antennas can be used for highly enhanced fluorescence and spontaneous emission of the embedded dye molecules.12,13 The methods presented in this paper can be generalized to other emitters, such as colloidal solid-state quantum dots14 or two-dimensional semiconductor materials,15 and the plasmon resonance can be tuned over a wide spectral range by varying the size of the nanocubes or the gap.
Caution: Several chemicals (such as concentrated nitric acid (15.698 M HNO3) and hydrochloric acid (6 M HCl)) used in these procedures are hazardous. Proper gloves, eye protection and other safety equipment must be used. Please refer to the materials safety datasheets (MSDS) of all chemicals before use.
1. Nanocube Synthesis
2. Gold Film Evaporation
Note: An electron-beam evaporator was used to deposit gold (Au) films onto purchased cleanroom cleaned slides, with chromium (Cr) acting as an adhesion layer. The evaporation process takes place inside a vacuum chamber, enabling the molecules to evaporate freely in the chamber and then sublimate on the substrate. The operation procedure is:
3. Deposition of PE Layers
4. Deposition of Cy5 Dye Molecules
5. Deposition of Nanocubes to Form Nanopatch Antennas (NPAs)
6. Optical Measurements
Note: A custom built optical bright-/dark-field microscope is used in these measurements. The NPAs are illuminated by a white light source through a long working distance bright-/dark-field objective. The reflected/scattered light from the NPAs is collected by the same objective. A pinhole aperture (50 μm diameter) is used at an image plane to select signal from an individual nanoantenna. A digital camera is used to capture a color image. A spectrometer and a charge coupled device (CCD) camera are used to acquire spectral data. For fluorescence measurements, a 633 nm continuous wave HeNe laser is used for excitation and the signal was spectrally filtered by a long pass filter.
Here, we show representative results of the characteristics of the plasmonic nanopatch antennas, including SEM images of the sample structure, a reflectivity spectrum of a collection of nanopatch antennas and a scattering spectrum from a single nanopatch antenna. The energy of the plasmon resonance of the nanopatch antennas depends on the size of the nanocubes, the thickness of the dielectric gap region, i.e., the number of PE layers, as well as the dielectric material. In the procedure presented above we obtained Ag nanocubes with an average side length of 75 nm and slightly rounded corners (radius of curvature ~10 nm) coated in a PVP layer with an estimated thickness of 1-3 nm. In combination with the 5 PE layers and gold film, this result in a plasmon resonance centered at ~650 nm with a full-width-at-half-maximum (FWHM) of ~50 nm. This in turn has good spectral overlap with the absorption and emission wavelength of the Cy5 molecules which is centered at 646 and 662 nm, respectively.
Figure 3A shows a SEM image of a sample with a high concentration of nanocubes. These nanocubes were deposited on top of a Au film with 5 PE layers. Such SEM images are used to verify the overall quality of the nanocube synthesis; however, these samples are not utilized for further optical measurements as the density of the nanocubes is too high. Additionally, due to the high density, some nanocubes do not lie on the surface which is essential to form the plasmonic nanopatch antenna structure.
Figure 3B shows a SEM image of a sample of nanocubes fabricated using a nanocube solution which has been diluted by a factor of 1/10. This sample is used for measurements where the reflectivity of white light from an ensemble of nanopatch antennas was measured to determine the overall plasmon resonance. Figure 3C shows a SEM image of a sample of nanocubes fabricated using a nanocube solution which has been diluted by a factor of 1/100. This sample is used for scattering measurements of an individual nanopatch antenna. Using the diluted nanocube solution enables individual nanopatch antennas to be spatially isolated at an image plane by using a small pinhole.
Figure 4A shows a reflectivity spectrum, after normalization with the white light background, measured from a similar sample to the one shown in the SEM image in Figure 3B. Figure 4B shows a scattering spectrum from a single nanopatch antenna similar to the sample shown in the SEM image in Figure 3C.
Figure 4C shows a dark field image of a nanopatch antenna sample (prepared by a 1/100 diluted nanocube solution dispersed on a gold film with 5 PE layers) taken by a Nikon D90 digital camera. The observed bright red dots are due to scattering of white light from individual nanopatch antennas. A few spots are observed to have colors other than red, which is a result of nanocubes with different sizes or larger nanoparticles with non-cubic shapes.
Figure 4D shows two fluorescence spectra, one measured from a single nanopatch antenna (from a sample similar to the one shown in Figure 3C) and the other from a control sample consisting of a glass slide with the same number of PE layers and density of Cy5 dye molecules. The fluorescence intensity from Cy5 molecules coupled to the nanopatch antenna is much stronger than on the glass slide. This results from an enhanced excitation rate as well as a modified radiation pattern and increased quantum efficiency of the dye molecules.12 After correcting for background fluorescence and normalizing per unit area by dividing the area under the nanocube with the excitation spot size,12 we obtain an enhancement factor of ~ 12,000 from the data shown in Figure 4D. This enhancement factor is smaller compared with the previously reported value of 30,00012 likely due to the use of a Au instead of Ag film, increasing non-radiative losses.
Figure 1. Equipment setup for Ag nanocube synthesis. (A) A photograph of the equipment setup showing the heating bath on top of the stirring hotplate with temperature control. (B) A close up of the round-bottom flask (RBF) containing the nanocube solution during the synthesis. The setup is located inside a fume hood with proper air ventilation. Please click here to view a larger version of this figure.
Figure 2. Pictures of the nanocube solution. (A) Nanocube solution after the 2.5-hr synthesis and (B) after transfer to smaller tubes and re-suspended in de-ionized water. Please click here to view a larger version of this figure.
Figure 3. SEM characterizations of Ag nanocubes. (A) SEM image of a concentrated nanocube sample, (B) a diluted (1/10) nanocube sample, and (C) a diluted (1/100) nanocube sample. Please click here to view a larger version of this figure.
Figure 4. Optical characterizations of nanopatch antennas. (A) Normalized reflection spectrum measured from an ensemble of nanopatch antennas (non-diluted nanocube solution). (B) Scattering spectrum from a single nanopatch antenna (1/100 diluted nanocube solution). (C) A dark-field image of a nanopatch antenna sample (1/100 diluted nanocube solution) taken under white light illumination. Each bright red dot corresponds to an individual plasmonic nanopatch antenna. (D) Fluorescence from Cy5 dye molecules embedded in a nanopatch antenna (red solid line) compared to that from a glass slide with an identical concentration of Cy5 dyes (dashed black line). Please click here to view a larger version of this figure.
Silver nanocubes were chemically synthesized using reaction conditions similar to previously reported syntheses.2,12,17-20 This synthesis enables the fabrication of nanocubes with side lengths ranging from 50 to 100 nm. For example, a typical heating time of 2.5 hr will result in nanocubes with side lengths of ~75 nm. A longer synthesis time (> 3 hr) will lead to larger nanoparticles, however, this may also result in different shapes such as truncated nanocubes or octahedrons. The final solution was centrifuged and re-suspended in deionized water, and may be stored for at least one month in a fridge at 4 °C without any noticeable changes in the scattering spectra of the plasmon resonances.12
The size and shape of the Ag nanocubes from the process presented in the above protocol are very sensitive to the cleaning of the RBF, its cap and the stirring bar as well as the quality of the EG solution. Nanoparticles with different shapes such as rounded or elongated nanoparticles is a sign that there is likely an issue with one of these steps in the synthesis. It is therefore advised that steps 1.1.1-1.1.4 and 1.2.1-1.2.2 are critically important.
In Figure 4b the scattering spectrum collected from a single nanopatch antenna is shown which exhibits a strong plasmon resonance at 650 nm. Such a resonance indicates an excellent mode confinement in the gap region between the Ag nanocube and Au film made possible by high-quality nanocubes. Additionally, to obtain such a spectrum, it is also required that the sample is clean, the spacer layers (PE layers) have a uniform thickness and that the underlying Au film is smooth. The strong plasmon resonance is further confirmed by the data presented in Figure 4c where individual nanopatch antennas can be observed in the dark field image and in Figure 4d where large fluorescence enhancement is observed of Cy5 molecules located in the gap region. It should also be noted that the Ag nanocubes oxidize over time despite the PVP coating when exposed to air and thus it is recommended that optical measurements should be performed on the day the sample is prepared or within 1 to 3 days. To minimize oxidation, it is recommended that the nanopatch antenna samples be stored in vacuum or nitrogen gas.
The method presented in this paper enables the fabrication of Ag nanocubes and plasmonic nanopatch antennas with well-controlled dimensions utilizing colloidal synthesis and a layer-by-layer dip-coating process. Compared with other techniques such as optical or electron beam lithography, the technique presented here offers the potential for low cost and large-scale production while producing a narrow size distribution of nanoparticles.
The plasmonic nanopatch antennas presented in this paper also hold great promise for new nanomaterials by design exhibiting unique properties which may not exist in their macroscopic counterparts. In particular, these nanoantennas have shown record-high fluorescence enhancement of embedded dye molecules exceeding 30,000;12 spontaneous emission rate enhancements of 1,000; ultrafast spontaneous emission and high quantum yield.13,14 Additionally, it has been shown that emitters coupled to these nanopatch antennas exhibit highly directional emission which is critical for applications where coupling to an external detector or single mode fiber is required. Future applications of the nanoscale patch antennas may range from ultrafast optoelectronic devices, such as light emitting diodes, to high efficiency photodetectors and photovoltaic devices, sensing and quantum information processing technologies.12-14
The authors have nothing to disclose.
This work was supported by the Air Force Office of Scientific Research Young Investigator Research Program (AFOSR, Grant. No. FA9550-15-1-0301).
Reagents | |||
Ethylene glycol | J.T. Baker | 9300 | Must be anhydrous |
Sodium hydrosulfide hydrate | Sigma Aldrich | 161527 | |
Poly vinylpyrrolidone | Sigma Aldrich | 856568 | |
Hydrochroric acid BDH ARISTAR PLUS | VWR International | 7647-01-0 | |
Silver trifluoroacetate | Sigma Aldrich | 482307 | Store in dark place |
Acetone | Sigma Aldrich | 48358 | |
Nitric acid | Sigma Aldrich | 7697-37-2 | concentrated (70%), for cleaning |
Poly(allylamine) hydrochloride (PAH) | Sigma-Aldrich | 283215 | |
Polystyrene sulfonate (PSS) | Sigma-Aldrich | 561223 | |
Sodium Chloride | Macron Inc. | 7647 | |
Sulfo-Cyanine5 carboxylic acid (Cy5) | Lumiprobe | 13390 | Fluorescent dye (molecular weight: 664.76 g/mol) |
Equipments | |||
Stirring hotplate with temperature control | VWR International | 89000-338 | |
Vortex mixers | VWR International | 10153-834 | |
Microcentrifuge | Thermoscientific | Model 59A | |
Silicone fluid | Sigma-Aldrich | 63148-62-9 | |
Micro-scale | Mettler Toledo | Model ML 104/03 | |
Electron-beam metal evaporator | CHA Industries | E-beam evaporator | Located inside a clean room |
Pre-cleaned glass slides | Schott North America, Inc. | Nexterion Glass B | Clean room pre-cleaned |
25-mL 24/40 round-bottle flask | VWR International | 60002-290 | |
Magnetic stirring bar | VWR International | 58948-116 | |
Micropipettes (1-10mL, 10–100 mL and 100–1000 mL) | VWR International | ||
Ultrasonic cleaning bath | Branson Ultrasonic | Model 1510R-DTH | |
Stopwatch | VWR International | ||
Eppendorf centrifugation tubes (1.5 mL) | VWR International | 22364111 | |
Poly(propylene) coning tubes (50 mL) | VWR International | ||
Home built bright/darkfield microscope | 75 W Xenon white light source, Nikon BF/DF 50x ELWD 0.55 NA, 8.2 mm WD objective, Nikon D90 digital camera, Acton 2300i spectrometer, Photometrics CoolSnap HQ charge coupled device (CCD) camera |
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He Ne laser (633 nm), 5 mW | New Port Co. | R-30990 | |
Reflectance standard | Lab Sphere | Model SRS-99-010 | |
Laser long pass filter 633 nm | Semrock | LP02-633RU-25 |