Surface plasmon resonance (SPR) technique has been successfully used in a variety of sensing applications, since it provides rapid, label-free, and quantitative sensing capability when detecting biomolecular reactions on a sensor surface [1, 2]. SPR is attributed to the excitation of surface plasmon polaritons (SPPs) when a transverse magnetic (TM)- polarized beam incident on a thin metal film between two dielectric media is coupled to surface plasmons formed in the film . These plasmons resonantly couple with the incident light at a specific resonance angle when the momentum matching between an incident photon and a SPP is achieved. They propagate tens to hundreds of micrometers along the metal surface and also decay exponentially away from the surface. Across the interface between a metal film and a surrounding dielectric medium, the wave vector, kSPP, is continuous for momentum matching, so that the dispersion relation can be written as:
where ω and c denote the angular frequency and the speed of light in the free space. εM and εD are the complex dielectric functions of a metal film and a dielectric medium. This equation describes a resonance shift resulting from a small change in refractive index induced by interactions amongst biomolecules on the metal surface. Thus, in SPR biosensing, the adsorption of a target analyte by surfaceimmobilized ligands is measured by tracking the change in the resonance condition. Over the past two decades, researchers have performed numerous SPR-based biomolecular interaction analyses to measure biomaterial concentration, thickness, and binding kinetic data for specific biological analytes including antigen/antibody [4, 5], protein/protein reactions [6, 7], cell responses [8, 9], DNA hybridizations [10, 11], and other adsorption processes .
metal film supporting SPPs. While silver films with a narrower SPR curve in the visible band yield higher sensitivity, gold films are employed more frequently because gold is chemically stable and reliable compared with a silver film [13, 14]. On the other hand, it has been known that a surface plasmon wave propagating along the silver surface is less attenuated and exhibits higher localization of electromagnetic field in the dielectric medium than SPPs supported by a gold film .
There are basically two configurations for SPR biosensing: reflection and transmission types. A conventional SPR biosensor based on the standard Kretschmann configuration works as a reflection-type in the sense that a photodetector measures the reflected light. Its optical platform consists of a light source, an SPR coupler such as a high-index prism or periodic grating surface, and a photodetector on the same side of the light source with respect to the metal film (Fig. 1). For this scheme, the resonance coupling appears as a deep absorption band in the reflectivity of the light spectrum. Depending on the detection method, changes in light intensity at a specific incidence angle, or changes in wavelength or angular position with a minimum reflectance can be measured. Figure 2 shows that refractive index change Δn results in the shift of resonance wavelength Δλ, angle Δθ, and the change in the amplitude of reflected light ΔR .
[FIG. 1.] Schematic of a prism coupler-based reflection-typeSPR system. A TM-polarized light with a fixed wavelengthor a fixed incidence angle illuminates the sensorsubstrate through a high-index prism coupler. A thin metalfilm is deposited on a slide glass with an adhesion layer.Within fluidic channels, receptors are immobilized on thesensor surface and target analytes in an aqueous solutionare bound selectively to them.
[FIG. 2.] Typical wavelength or angular spectra of a reflection-type SPR biosensor. The refractive index change Δn at the sensor surface leads to the shift in the resonance wavelength Δ λ, resonance angle Δθ, and the change in the amplitude of reflected light ΔR.
A transmission-type SPR biosensor, often using a wavelength scanning setup, has also been extensively explored to study spectral outcoupling of surface plasmons excited in metallic nanostructures . As shown in Fig. 3, metallic nanostructures immobilized on a glass substrate are exposed to solvents and aqueous solutions within fluidic channels. The experiment setup uses a white light with normal incidence and the transmitted light is collected by a conventional objective lens and delivered onto a spectrometer via optical fibers.
This configuration is fully based on the localized surface plasmon (LSP) modes. It has been well known that noble metal nanostructures allow direct and strong optical coupling of the incident light to resonantly driven electron plasma oscillations, called localized plasmons . Compared with SPPs excited in a thin metal film, the LSP resonance (LSPR) excitation induces substantial enhancement of electromagnetic fields as a result of strong absorption and highly efficient light scattering. The specific nature of the field enhancement in a metallic nanostructure depends on intrinsic parameters, such as composition, size, and shape, as well as extrinsic factors of the surrounding local media [18-20]. Since spectral position and magnitude of LSPR are sensitive to changes in the local environment caused by molecules adsorbed onto the nanostructures, LSPR devices can serve as transmissionbased biosensors . Figure 4 shows that the position of LSPR red-shifts with an increasing dielectric constant due to the buildup of polarization charges on the dielectric side of the interface .
[FIG. 3.] Schematic of an extinction-based transmission-typeLSPR system. Surface-confined metallic nanoparticles arefabricated on a transparent glass substrate in a regular ornon-regular manner. UV-visible extinction measurementsare collected by a conventional microscope objective andfocused onto a fiber-coupled spectrometer. All spectracollected are macroscopic measurements performed instandard transmission geometry using a white light source.The fluidic channel is used to control the external environmentof the metallic nanoparticle-based glass substrates.
[FIG. 4.] Typical extinction spectra of a transmission-type LSPR biosensor. The refractive index change Δn at the medium surrounding the metallic nanoparticles leads to the shift in the resonance wavelength Δλ.
Relative to a conventional SPR, an optical setup to characterize an extinction-based LSPR biosensor is compact and potentially easier to use because it is based on wavelength scanning at normal incidence and allows the light source and the detector to be positioned on opposite sides. A more important characteristic of an LSPR biosensor is its capability for high-throughput monitoring, for example, in DNA research and proteomics for which thousands of binding interactions should be examined rapidly so that individual nanostructure can act as its own transducer .
Recent advances in nanoparticle synthesis and nanofabrication techniques have allowed the assembly of complicated patterns of interacting metallic nanostructures. The plasmon resonance of interacting nanostructures leads to interesting and new optical responses obtained from near-field coupling or far-field dipolar interactions depending on the spacing between adjacent nanostructures . For enhanced optical biosensing, the LSPR and its shifts in interacting or noninteracting metallic nanostructures have been extensively exploited. Therefore, this paper reviews optical and physical properties of plasmonic nanostructures and their contributions to a realization of enhanced optical detection platforms, including various LSPR-based approaches for significant amplification of SPR signals.
While the traditional metal film-based SPR biosensor has a sensitivity as high as 5 × 10-7 refractive index units, which corresponds to 1 pg/mm2 [2, 24], its detection limit can be further improved by coupling the biomolecular recognition of target analyte with another event that leads to larger changes in the SPR signal [25-27]. This signal
[FIG. 5.] Schematics and SPR curves of (a) an evaporated gold film modified with a-h-IgG(γ) and then exposed to a 1.0 mg/mL solution of h-IgG and (b) a gold film modified with a-h-IgG(γ) and then exposed to h-IgG-10-nm gold colloid conjugate . Exposure of an evaporated gold film coated with γ-chain-specific monoclonal goat anti-human immunoglobulin G(a-h-IgG(γ)) to a 1.0 mg/mL solution of human immunoglobulin G results in a 0.1° shift in plasmon angle with no change in curve shape (Fig. 5(a)). In contrast, a significantly larger shift of 1.5°, a 2% increase in minimum reflectance, and noticeable broadening of the curve are observed upon exposure of an identically prepared surface to an electrostatically bound conjugate between h-IgG and 10-nm-diameter colloidal gold [h-IgG-Au] (Fig. 5(b)). On the basis of plasmon shift alone, this represents a 15-fold increase in SPR sensitivity to the biomolecular interaction event.
enhancement can be achieved by labeling the adsorbed analyte with dielectric or metallic nanoparticles. These labels obviously increase the optical constant in the vicinity of the metal surface and also can induce a plasmonic coupling of LSP modes with propagating SPPs on the flat metal film, resulting in additional SPR shifts. A wide range of nanoparticles have been introduced, including colloidal metallic nanoparticles [28, 29], latex particles , and dye-doped polymer particles .
As an example of a metallic nanoparticle-enhanced LSPR biosensor, antibody-antigen interaction was measured as shown in Fig. 5. In this experiment, a surface-immobilized antibody is sequentially exposed to antigen and a solution of antibody-conjugated gold nanoparticles . The SPR curves in Fig. 5 show that the shift of SPR angle upon binding the antigen alone is very small compared to the shift observed when the secondary antibody is conjugated with gold nanoparticles. This approach has been also used for detecting DNA hybridization . In a similar way, single-stranded DNA was linked covalently to the gold surface and then hybridized by the complementary DNA, which itself was functionalized by gold nanoparticles. Gold nanoparticles attached to the target DNA caused 18-fold signal amplification which was explained by the interaction of localized and propagating surface plasmons. In addition, it was demonstrated that the particle size, material, and surface coverage as well as the metallic substrate can affect the measured signal enhancement .
On the other hand, the reflectance characteristics of SPR biosensors employing colloidal metallic nanoparticles are different from those for conventional SPR biosensor, in that they exhibit a broad reflectivity spectrum and an increase in minimum reflectance. For good biosensing performance, a narrow spectral width and a deep absorption band are desired, because with a highly broad and shallow SPR curve, it becomes quite difficult to detect the resonance position accurately and to analyze the effect of binding events on a SPR structure precisely. Moreover, this approach involves complex procedures in the preparation of nano-sized colloidal nanoparticles with functional immobilizations in order to tag the target analytes, and thus it eliminates the important advantage of the SPR technique, namely that labeling is not essential .
The unique properties of metallic nanostructures have attracted significant attention because of the physical characteristics such as local field enhancement and surface-enhanced Raman scattering. It has been demonstrated that the Raman scattering of the underlying molecules can be enhanced by fabricating SPR substrates with metallic nanoparticles . Inspired by this, the colloidal gold nanoparticles are synthesized in a chemical operation and then immobilized on a thin gold film. In Fig. 6, embedding metallic nanostructures on a gold film is an effective way of increasing the roughness of the substrate, which therefore results in a notable enhancement in the light scattering and absorption.
[FIG. 6.] LSPR sensor substrate with gold nanoparticles embedded in a dielectric layer on a thin gold film . A 47.5-nm thick gold layer was initially deposited on a slide glass using a dc magnetron sputter. Subsequently, mixed thin films composed of SiO2 and gold nanoparticles were deposited via an RF and dc magnetron co-sputtering process. A close inspection of the transmission electron microscopy results revealed that most of the gold nanoparticles with an estimated size of ~4 nm and spacing between nanoparticles of ~6 nm were uniformly distributed over the substrate surface.
At the initial stage, researchers introduced a method to immobilize gold nanoparticles on a thin gold film by drying a chemical solution containing suspended gold nanoparticles. However, due to the difficulties in controlling and quantifying the volume fraction of the nanoparticles actually deposited on the film, alternative fabrication methods were developed in which gold nanoclusters were embedded in the dielectric film via an RF magnetron co-sputtering process. Using an SPR substrate with embedded gold nanostructures, DNA hybridization experiments presented an improved detection performance of approximately 0.1 pg/mm2 . This technique provides a feasible and reliable method to control the optimal size and volume fraction of the gold nanoclusters embedded in the dielectric film without the need for complex strategies to amplify the SPR angle shift.
Another example is the work of Matsui et al. on gold nanoparticle-embedded hydrogel as a SPR sensing medium . By swelling of the hydrogel and an increase in the distance between the gold nanoparticles, the medium was functionalized to be selective to the binding of small molecules. An enhanced shift in the SPR curve to higher SPR angles was observed by the interplay of propagating SPPs and resonant LSP modes.
With rapid development of nanotechnologies that allow metallic nanostructures to be fabricated and synthesized on the nanometer scale, it has been empirically shown that the use of metallic nanostructures enables an efficient optical coupling of incident light to plasmon resonance, which has been utilized to amplify the optical signals of conventional SPR biosensors. Among various interaction mechanisms between incident light and surface plasmons in play in the sensitivity enhancement, two major mechanisms at work are the SPP-LSP interaction and the LSP-LSP coupling between adjacent nanostructures, resulting in complex resonance properties with an additional shift of SPR angle . In particular, the exploitation of periodic nanostructures can offer the advantage of spatial uniformity and performance reproducibility, while preserving the profit of label-free detection.
As an example of LSPR optical sensing based on periodic nanostructures, one-dimensional (1D) subwavelength gold nanogratings on a thin gold film were explored (Fig. 7(a)). The numerical calculations using rigorous coupled-wave analysis [38, 39] and a finite-difference time-domain (FDTD) method have presented interesting LSPR sensing characteristics of 1D nanogratings built on the flat surface. Byun et al. showed that the enhancement enabled by the excitation of LSP modes in gold nanogratings, offers improved performance in sensitivity by more than an order of magnitude compared with a conventional SPR configuration . Optimal gold nanogratings were then designed in terms of the robustness to fabrication errors in implementing periodic structures and the various sensor performances, such as SPR angle shift, SPR curve angular width, and minimum reflectance at resonance .
[FIG. 7.] (a) Schematic of a gold nanograting-mediated LSPR substrate. 1D gold nanograting is regularly patterned on a thin gold film. (b) Scanning electron micrograph images of 1D gold nanograting (period = 200 nm and width = 100 nm, thickness = 20 nm) and 2D gold nanowell array (period = 200 nm, diameter = 80 nm, thickness = 15 nm) on a gold surface.
Subsequently, the effect of surface roughness on the sensitivity of gold nanograting-based LSPR biosensors was investigated . Contrary to a conventional scheme with no distinguishable decrease in sensor performance regardless of the correlation length when the roughness < 1 nm, surface roughness displayed a substantial effect on the sensitivity for SPR substrates with gold nanogratings at Λ < 200 nm while the enhancement deteriorated by more than 30% at a short correlation length less than 100 nm, because the presence of surface fluctuation causes disordered coupling between nanogratings and consequently discourages the enhancement of the sensitivity.
Additionally, the correlation between the localized plasmonic fields induced by the surface nanostructure and the position of target adsorption was analyzed quantitatively and it was found that target localization on nanograting sidewalls improves sensitivity significantly because of strong overlap with resonance LSP modes . To confirm this effect, enhanced electromagnetic fields near the sensor surface were visualized by calculating the spatial distributions of EX, HY, and EZ based on the FDTD method. The minimum grid size for the FDTD was 0.5 nm. Figures 8 and 9 show the field distributions of EZ for 1D gold nanogratings with a period of 100 nm, a width of 50 nm, and a thickness of 10 nm. The figures present well-known features of LSPs excited at a metallic nanostructures that are quite typical
[FIG. 8.] Vertical field intensity distributions of EZ around the LSPR sensor surface for 1D nanograting with a period = 100 nm, a width = 50 nm, and a thickness = 10 nm. TM-polarized light with a wavelength of 633 nm is incident on the substrate. The insets are 2D images obtained from FDTD calculations normalized by the field intensity of 20.
[FIG. 9.] Horizontal field intensity distributions of EZ around the LSPR sensor surface for 1D nanograting with a period = 100 nm, a width = 50 nm, and a thickness = 10 nm. TM-polarized light with a wavelength of 633 nm is incident on the substrate. The insets are 2D images obtained from FDTD calculations normalized by the field intensity of 20.
of the fields of nonregular metallic nanostructures . On the assumption of an incident electric field of unit amplitude, maximum field amplitudes obtained by FDTD were EX = 59, HY = 8, and EZ = 41. What is as important as field enhancement is where these maxima occur. Obviously, the amplitude of plasmon waves decays rapidly when one moves further away from the nanostructure surface. Since locally enhanced plasmons called “hot spots” are distributed at very short distances from the surface [45, 46], only a limited number of biomolecules within the local fields participate in the resonance shift of an LSPR biosensor, even if a large number of molecules are involved in the interaction.
The results in Figs. 8 and 9 also indicate that all maxima are located within 1 nm from the surface in the vicinity of vertices. In addition, because of the field enhancement on nanograting sidewalls, biomolecules on sidewalls participate more vigorously on average than those on nanograting tops and bottoms. As a result, an efficient interplay between target analytes and enhanced LSPs leads to the most prominent improvement of sensitivity with target localization. Note that there are, in fact, multiple peaks associated with each corner. Since the decay length of an LSP resonance from the surface of a metallic nanostructure is longer than the interpeak distance, the multiple peaks of each corner should be regarded as a whole as an individual LSP resonance.
Experimentally, an LSPR substrate with periodic gold nanograting was fabricated as shown in Fig. 7(b) and its sensitivity enhancement was confirmed when evaluated by changing a refractive index of the medium surrounding the sensor substrate. For measuring sensitivity characteristics of subwavelength nanogratings with Λ < 300 nm, the nanograting samples were fabricated on a thin gold film by electron beam lithography. Our substrates were spin coated by a 100 nm thick photoresist film. The regions exposed to an electron beam were chemically dissolved, and the resulting photoresist layer was used as a mask for dry etching of a gold film. Following uniform dry etching, a residual photoresist layer was finally removed by means of a plasma asher. After these processes, we produced 1D gold nanogratings arranged on 40 nm thick gold/SF10 glass substrates, and we experimentally observed a significant SPR signal amplification. As biological events on the sensor surface, the formation of self-assembled monolayer (SAM) and DNA hybridization were employed and the experimental results showed a significant improvement in sensitivity, well consistent with theoretical predictions [47, 48].
Recently, more complex structures such as two-dimensional (2D) gold nanopost or nanowell arrays regularly patterned on an SPR substrate have been studied to demonstrate highly sensitive label-free detection of DNA hybridization (Fig. 7(b)). Similar to the case of 1D nanograting, the sensitivity enhancement was associated with a surface-limited increase of reaction area and structural perturbation of periodic gold nanostructures on a thin gold film. The perturbation prompts propagating SPPs to interfere with excited LSPs, achieving local field enhancement by resonantly exciting LSP modes and coupling effects between the LSP modes. Experimental data demonstrated that 2D gold nanostructures fabricated on a thin gold film can enhance the sensitivity of conventional SPR biosensor significantly. The data also indicated that both the nanostructure size and period play a role in SPR signal amplification .
Since the development of a high-throughput SPR imaging system has emerged as one of the most important biosensing applications, it is thus an obvious next step in an evolutionary path to investigate whether periodic nanostructures can equally enhance the sensitivity for SPR imaging. It was found that periodic gold nanostructures with a narrow width and a small period presented highly enhanced sensitivity when measuring reflected intensity difference with binding analytes from without . Also, the results displayed extremely linear sensing characteristics over a broad range of binding refractive index. On the other hand, the presence of metallic nanostructures may strongly influence the broadening of a SPR curve and a decrease of sensing contrast. Hence, the enhancement obtained from the reflectance change is generally less than for SPR angle shift, while periodic metallic nanostructure-mediated SPR imaging system demonstrated a potential to implement a rapid SPR microarray imaging system with an enhanced sensitivity.
It has been well known that arrays of gold or silver nanoparticles formed on a transparent substrate exhibit an LSPR extinction band that can be tuned from the near-UV to mid-IR by simply changing the size, shape, and spacing of the nanoparticles [16, 37]. The extinction peak position is sensitive to the local changes in refractive index occurring near the surface of the immobilized nanoparticles, and the peak position red-shifts linearly with an increasing concentration of target analytes. In particular, the responses of LSPR biosensor vary in a complex and nonlinear fashion when binding events occur at large distances from the surface of the metallic nanoparticles .
Theoretically, suppose that we have well-separated and noninteracting nanostructures which are significantly smaller than the incidence wavelength (i.e., λ ≫ 2R, where R is the radius of the nanoparticle). According to the Mie-scattering theory, the optical extinction of interaction-free spherical metallic nanoparticles can be reduced as follows :
E(ω) is the optical extinction (i.e., sum of absorption and scattering), ω is the angular frequency of the exciting radiation, εd is the dielectric function of the binding layer on the nanostructure, V is the nanosphere volume, εr and εi are the real and imaginary parts of the dielectric function of the metallic nanostructure, and c is the light velocity in the free space. As presented in Eq. (2), the resonance condition of the LSP is satisfied when εr(ω) = -2εd and εi is small. Equation 2 does not describe the optical behavior of larger metallic nanoparticles beyond the Rayleigh approximation (2R ≥ 30 nm). In those cases, scattering processes and complex plasmonic effects such as retardation and radiative losses start to contribute significantly to the plasmon damping [52, 53]. In other words, the extinction characteristics are dominated by higher-order multipole absorption and scattering, and the full Mie equation needs to be used to model the absorption spectra [54, 55]. On the other hand, for a nonspherical nanostructure with a noncircular cross section, surface plasmons are not distributed uniformly, manifesting in a shape dependence of the resonance of LSP modes [56, 57]. Therefore, both the shape and the dielectric function of the nanostructure affect and determine the optical extinction properties.
Figure 10 shows a demonstration of the adsorption-induced LSPR shift obtained from silver nanoparticles immobilized on a glass substrate . Silver nanoparticles have in-plane widths of ~100 nm and out-of-plane heights of ~50 nm. To prepare the LSPR biosensor for biosensing events, the nanoparticles were first functionalized with a SAM and the LSPR was measured to be 598.6 nm. Next, biotin was covalently attached and its LSPR was determined to be 609.6 nm, corresponding to 11 nm red-shift. The LSPR biosensor was then exposed to the target analyte of streptavidin (SA) and an exposure to 100 nM SA led to the extinction peak at 636.6 nm, corresponding to an additional 27 nm shift. As a result, further modification of the sensor substrate by a biotin and SA provokes an additional resonance shift. Also, note that the signal transduction mechanism in this approach is a reliably measured wavelength shift rather than an intensity change as in many previously reported nanoparticle-based transmission-type LSPR biosensors.
Several advantages of a transmission-type LSPR biosensor with plasmonic nanostructures include (1) its compact optical setup which is more appropriate for miniaturization than reflection-type SPR detection, (2) a high sensitivity, especially when the resonance of the analyte combined with various labels overlaps with the intrinsic LSPR of the metallic nanostructures , and (3) an ultrahigh spatial resolution because a single nanoparticle can act as an individual transducer for precious or limited-volume samples. As an example, a LSPR shift of ~40 nm was measured from Rayleigh scattering spectroscopy for specific binding in low concentration of ~100 zeptomoles by employing a single triangular silver nanoparticle .
[FIG. 10.] Detection of SA binding to biotinylated silver nanoparticles immobilized on a glass substrate. (A) Silver nanoparticles after surface modification with 1 mM SAM, λLSPR = 598.6 nm. (B) Silver nanoparticles after modification with 1 mM biotin, λLSPR = 609.6 nm. (C) Silver nanoparticles after modification with 100 nM SA, λLSPR = 636.6 nm.
In terms of formation of metallic nanostructures immobilized on a glass substrate, various synthesis and fabrication techniques have been investigated. One of the commonly used procedures for yielding spherical nanoparticles is the reduction of metal salts in a solution containing a specific stabilizer, such as ligands, surfactants, or polymers, which binds to the surface of nanoparticles and inhibits their aggregation . The size and shape of nanoparticles can be adjusted by the reductant, stabilizer, and concentrations of reagents. More complex nanostructures nanorods or nanoshells can be prepared by seeding growth techniques [62-64]. The morphology of a metallic nanorod with two distinct plasmon modes associated with its non-symmetric shape is determined by the composition of seeds, surfactant, and additives. For example, in Fig. 11, gold nanorods were synthesized electrochemically in the presence of a surfactant and cosurfactant solution mixture known to form rodshape micelles [65, 66]. The shape distribution of the rods depends on the current and the ratio of the concentration of the surfactant to that of the cosurfactant used. Moreover, by metalizing colloidal silica nanosphere cores, gold nanoshells can be obtained and the final thickness of gold shell is controlled by changing the initial gold seed coverage and the concentration of reductant used in the electroless plating process . On the other hand, in order to improve the reliability of the nanostructured substrate and to control the size, shape, and spacing of metallic nanostructures precisely, lithographic techniques such as electron beam lithography and focused ion beam lithography have been used frequently [48, 49, 68]. After patterning thin resist layer with a high power scanning beam, the patterned resist isutilized as a sacrificial masking layer in subsequent etchingor metal deposition processes, resulting in well-controlled1D or 2D nanostructures.
[FIG. 11.] Synthesis of gold nanorods and their absorptionspectrum. Two distinct plasmon modes become morepronounced when the aspect ratio of the metallic nanorodsis increased: one at a shorter wavelength of ~520 nm isdue to the coherent electron oscillation along the short axis,and the other is at a longer wavelength of ~780 nm, whichis more intense and obtained from the coherent electronoscillation along the long axis .
It is also interesting that unconventional approaches,which are capable of patterning large areas at a relativelylow cost, provide an effective alternative to scanning beamlithographic techniques. For example, triangular nanoparticlearrays obtained from hexagonally distributed colloidal crystalmask were fabricated by using nanosphere lithography .Soft lithography is another well-known versatile techniquefor patterning periodic metallic structures at the nanoscaleover large areas . These conventional and unconventionalfabrication methods are practical for both reflectionand transmission-type LSPR biosensing configurations.
From the experiments on the light transmission through arrays of nanoholes in thin gold and silver films, it was found that the amount of transmitted light at certain wavelengths was much greater than predicted by the classical aperture theory; i.e., the substrate appeared much more transparent than it should be [71, 72]. This unexpected result is called extraordinary optical transmission. In principle, the peaks of maximum transmission were dependent on the period between the nanoholes. The excitation of surface plasmons seems to mainly contribute to the effect of extraordinary optical transmission, while its interpretation is still underway .
The transmission characteristics through arrays of nanoholesare related to the optical properties of the metal-dielectricinterface. At normal incidence, the resonancewavelength (λpeak) from nanohole arrays with symmetricsquare lattice can be estimated by Eq. (3)
where p is the lattice constant, i and j denote the scattering orders of the array, and εM and εD are the dielectric constants of the metal and its adjacent medium, respectively . Therefore, the adsorption of biomolecules on the metallic substrate may induce a shift of resonance wavelength or a change in peak intensity. In contrast to the conventional reflection-type SPR biosensor, the momentum matching condition for plasmon resonance in zero-order transmission is given by the periodicity of the nanoholes and thus, prism coupling is not required .
Figure 12 demonstrates an experimental setup to measure the extraordinary optical transmission effect [75, 76]. The metal film is deposited on a glass slide and the array is fabricated using focused ion beam milling. The transmission spectra are obtained using a spectrometer via an optical
[FIG. 12.] Experimental setup for light transmission measurements through the arrays of subwavelength holes and transmission spectra of normally incident white light . All spectra were obtained using near-IR source from the halogen lamp, objective lens (×100), and optical fiber-coupled spectrometer. The arrays of subwavelength holes were fabricated using focused ion beam milling and the diameter of the nanohole arrays was 200 nm and the gold film was 100-nm thick. In biological experiments, the substrates were modified with a SAM and then were immersed in 100 μM aqueous solution of bovine serum albumin (BSA). The transmission peaks were found at (A) 645 nm for bare gold surface, (B) 650 nm for gold substrate modified with a SAM, and (C) 654 nm for BSA adsorption to the SAM immobilized on the gold surface, respectively.
fiber coupler. Peaks in the white light transmission correspond to the wavelengths that match the conditions of Eq. (3) for the changes in the dielectric properties of the surface. The normal incidence setup allied to the small footprint of nanohole arrays offers an attractive opportunity for miniaturization. From the experiments in Fig. 12, the sensor sensitivity with an order of magnitude better than the values from angle-resolved SPR systems was obtained. It is important to point out that the sensing area of the nanohole arrays is highly localized and hence, the changes in both peak positions and intensities originate from a smaller number of target molecules. This new approach for SPR sensing is more compatible with the lab-on-chip concept and provides the possibility of high-throughput analysis from a single SPR chip [74, 77].
Beyond the pursuit of ultrahigh sensitivity for enhanced detection of biomolecules at a very low concentration, recent trends are focused on two representative topics: robust integration and miniaturization for portable biosensors and development of sensor platforms for high-throughput screening.
Most of commercial SPR biosensor systems are generally based on the conventional prism-coupled SPR configuration with angle interrogation scheme. Although this approach is simple, robust, and sensitive, it is not in practice appropriate for miniaturization. Hence, there are continuing efforts to employ optical fibers and waveguide structures as an alternative to the prism-based configuration. After an initial exploitation of single mode optical fibers which were sidepolished and coated with a thin metal film , the fiber tip with a form of micro-prism has been optimized to improve the coupling of light to SPP modes and a polarization- maintaining fiber-based SPR sensing has been developed for stable polarization control and accurate measurement [79, 80].
Another alternative approach has been the planar optical waveguides with a multilayer structure. These waveguides may realize the development of portable SPR biosensor systems because they enable accommodation of multiple sensing elements on a single substrate using micro-fabrication technology . In particular, by designing multimode waveguides in which a polychromatic radiation is incident on the different sensing channels at different angles of incidence or on a high refractive index dielectric overlayer which shifts the resonance wavelength for a part of the sensing surface, it is possible to extract information of target analytes on the molecular density and on the refractive index on the sensing layer simultaneously and thus to analyze the complex samples quantitatively . Moreover, a miniaturized SPR platform based on optical fibers or planar waveguides can be combined with plasmonic nanostructures to recognize the adsorbed biomolecules more efficiently. With an additional layer involving metallic nanostructures placed on a thin metal film, an improved sensitivity to the local index change could be accomplished.
In terms of high-throughput capability, SPR imaging in which a collimated light is incident on a sensor surface with a fixed angle has been the strongest candidate for microarray- based multi-channel detection among reflection-type SPR biosensors. Its distinguishing feature is the use of CCD camera where the SPR signals are captured as images after passing through a narrow band interference filter . While SPR imaging scheme has an important advantage of simplicity of structure with no moving parts, the intensity-based method has difficulties in achieving significant detection accuracy because of insufficient sensitivity. In order to surmount this restriction on sensitivity, an introduction of metallic nanostructures in SPR imaging biosensors has been investigated [26, 50]. The sensitivity improvement in SPR imaging can be slightly degraded due to the broadening of a SPR curve and a decrease of sensing contrast, accompanied by the presence of metallic nanostructures. Nevertheless, rapid development of nanofabrication techniques will make it possible to realize an enhanced SPR imaging with high-density arrays and high sensitivity for future genomic and proteomic works. Another interesting approach for SPR imaging is an interferometry-based phase detection system producing an interference pattern on a CCD camera . While it has a small dynamic range and limitations in facilitating real time SPR sensing, interferometry may produce more rapid changes than intensity, demonstrating the potential for a sensitive SPR detection with no demand for plasmonic nanostructures.
For transmission-type LSPR biosensors, the transparentsensor substrates incorporating metallic nanostructures aremore amenable to miniaturization than reflection-type SPRdetection. Also, their sensitivity is known to be comparableto the performance of commercial SPR systems. Inparticular, as an LSPR biosensing has been demonstratedat the single nanoparticle level using various kinds ofmetallic nanostructures, an individual or ensembles of nanostructurescan work as a single transducer that transformsbinding events into corresponding optical changes. In short,since the planar format and transmission optics are suitablefor multiplexing in a microarray platform, microarrays formultiple detection and high-throughput analysis seem to bethe next step for enhanced transmission-type LSPR biosensors.
In this review, exploitation of plasmonic nanostructuresexhibited significant advantages over conventional SPRsensing schemes. Surface plasmons, surface-bound electromagneticfields, are categorized into two classes of SPPsand LSPs. In reflection-type LSPR biosensors, both classesare present and their interplay contributes to the enhancementof sensing performances, while only LSP modesdominantly affect the sensor characteristics of transmissiontypebiosensors. In both cases, however, a plasmonicapproach based on nanostructured metallic substrates offersan exciting and promising alternative to surmount thelimitations of conventional SPR sensors. Hence, themanipulation of optical properties of surface plasmons byadjusting the geometric parameters of the nanostructureshas been the hot issue in the area of plasmonic-basedbiosensors. Beyond the scope of optical biosensors, thepotential for the development of plasmonic devices in thesubwavelength regime will be a prominent impetus inseveral encouraging applications, for instance, plasmonicsintegrated circuits allowing information processing at anultrafast speed, superlensing phenomenon surpassing thediffraction limit in imaging systems, and plasmon-assistednanolithography technique utilizing the confinement oflocally enhanced fields.
Especially, it should be emphasized that, to achieve a breakthrough for a full realization of the potential of SPR biosensors, a greater collaboration in a variety of fields is very much required. Together with a better understanding of the underlying fundamentals and a development of theoretical analysis algorithms and new biosensing concepts, advances in the areas of such as opto-electronics for low-noise light sources and efficient photodetectors, integrated optics forminiaturizing SPR components and planar waveguides, surfacechemistry for effective surface modification and ligand design,microfluidics, and nanofabrication techniques are all essentialfor the development of point-of-care and in-field SPR biosensorswith an ultrahigh sensitivity and selectivity. Relevantin-depth studies are currently under way in many researchgroups and in the near future, it is hoped that mobile SPRplatforms will be in widespread use, satisfying the variousneeds of the consumers.