# The Effect of Oxidation on the Far-Field Scattering of Aluminium Patch Antennae from Visible to UV

Authors: Duncan McArthur; Francesco Papoff
Journal: International Journal of Optics
 (2019)

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## Abstract

In this paper we evaluate the effect of oxidation on the total power scattered in the far field by a60nm radius Al sphere in the presence of a substrate comprised of either Al or silica (SiO2). Using an effective medium approach to model the Al particle with an outer layer of alumina (Al2O3), we find that the UV peak of total energy scattered in the far field shifts towards longer wavelengths for volume fractions of Al2O3 up to 20%. When particles with these volume fractions are held above an Al substrate, enhancement of two orders of magnitudes of the far-field power radiated by a dipole in the gap can be observed. For larger volume fractions of Al2O3, the total intensity of light scattered is significantly reduced.


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## Body

## 1. Introduction

In recent years a large number of papers in nanophotonics have been investigating the properties of aluminum because it is an abundant and low cost metal with plasmon modes in the visible and the ultraviolet [1–8]. Following earlier experiments [2], we have found [9, 10] that aluminum nanoparticles and substrates are ideally suited for label-free detection of weakly fluorescent molecules in the ultraviolet, because they have resonances with a much stronger far-field radiative enhancement than similar nanostructures of gold or silver, for wavelengths shorter than 370 nm. In particular, Al nanostructures can significantly enhance the detection of fluorescence by emitters for which the emission rate is much less than the internal nonradiative decay rate [11] when the emitter is strongly coupled to electromagnetic modes that efficiently transport energy into the far field. By changing the size of the nanoparticle, resonances can be tuned between 150 nm and 650 nm and enhance, by orders of magnitude, both the far-field radiation and the decay rates of dipolar emitters placed in the gap between the nanoparticle and the substrate. This could have a profound impact on sensing of many important molecules that have radiative decays in the ultraviolet much weaker than nonradiative decays. Examples of such molecules are alkanes [12], most amino acids [13] in proteins and peptides, and DNA bases.


## 2. Methods

In order to evaluate the feasibility of these applications, it is important to consider in what way oxidation of the Al surfaces may affect the performance of this system. In this paper we investigate how the ratio between the power radiated above the substrate,Pr, and the total power emitted by the dipole in vacuum, P0, depends on the volume fraction of alumina (Al2O3) in the presence of a substrate of either silica (SiO2) or Al. We consider substrates with thickness such that the light reflected by the lower surface is negligible, so that the substrates can be modeled as semi-infinite. The top layer of the Al substrate can also be oxidized, but for sake of simplicity we ignore here this effect, which should not change qualitatively the results presented when the oxidation layers are thin and do not support guided modes. We consider the following two configurations. The first configuration is similar to the standard set-up of a scanning near field optical microscope [14]: the particle lies on top of the substrate and it is illuminated by an electric dipole polarized along the axis z, which is perpendicular to the substrate, and placed 30nm above the particle’s surface. We investigate this configuration, even if it is not very suited to sensing, because it can be easily used to test the theory. The other configuration is the one most promising for sensing applications and is similar to patch antennae [15, 16]. In this configuration, the particle is held 5 nm above the substrate and the dipole source is placed in the middle of the gap.For all cases considered, we use the Bruggerman effective medium approximation [17] to model the effect of Al2O3 on the far-field scattering of light. The effective dielectric function, ε, for a material composed of Al and Al2O3 can be found, using given values of the permittivity for the two materials [18, 19] and their fractional volumes, from the following expression [20]:(1)VAlVεAl-εεAl+2ε+VAl2O3VεAl2O3-εεAl2O3+2ε=0,where V=VAl+VAl2O3 is the total volume of the particle. For high volume densities of Al2O3, this theory has reproduced experimental results from Al nanodiscs [20] on SiO2 substrates more accurately than the Maxwell-Garnett theory [17].The energy radiated above the substrate,Pr, is evaluated by integrating the far-field asymptotic form of the modulus squared of the electric field, given by Green’s function, over the upper semispace. The electric field is calculated via an expansion in principal modes [21–25] of Green’s function of the structure that includes the multiple scattering between the particles and the substrate at all orders [9, 10]. The expansion of the scattering Green’s function in terms of principal modes and their amplitudes is [10](2)GEP;Sr,r′pr′=∑nanspr′SnEr,where SnE(r) is the electric field of the n-th principal mode at the point r, and ans(p(r′)) is the amplitude of SnE due to the field generated by the dipole p in r′ (see Eq. (4)). The amplitude of each mode is the product of the “sensitivity” of the mode, which is an intrinsic property of the particle that depends only on the spatial correlation, at the surface of the particle, between the corresponding scattering and internal mode pairs, and the spatial correlation between these modes and the dipole field. This approach [9] can be applied to inhomogeneous host media [26] as long as nonlocal effects [24, 27] and quantum spill-out can be neglected [28].In order to evaluate the aforementioned configurations, we solve Maxwell’s equations for spherical particles above a semi-infinite substrate, with a monochromatic electric dipole source placed, either between or above the particle and the substrate, along thez axis, which is the symmetry axis. The scattered field is expanded in terms of radiating electric and magnetic dipoles distributed inside the particle along the z-axis and polarized along the Cartesian axes. In order to consider self-consistently multiple scattering effects between particle and substrate, we add to each radiating dipole field the corresponding field reflected from the substrate calculated via Sommerfeld integrals [29, 30]. For the internal field we use spherical multipoles, with origin at the center of the particle [31, 32].With this choice of internal and scattered fields, we can form the principal modes as for a single particle in a homogeneous medium [21] and then use these modes in Eq. (2) to approximate Green’s function. The procedure is as follows. First of all, we define the scalar product f·g=∑i=14‍∫∂V‍fi∗gidA, with fi, gi the tangent electric (i=1,2) and magnetic (i=3,4) components, in an arbitrary orthonormal system, of two solutions of Maxwell’s equations at the surface of the particle ∂V. In order to improve the numerical stability, the electromagnetic field of each source is normalised so that f·f=1. Orthonormal internal and scattering mode bases are formed via QR decompositions of the internal and scattered surface fields separately [23, 33], using freely available linear algebra routines [34]. Using these bases we then find principal internal, {in}, and scattered modes, {sn}, such that in·sm=δnm, with δnm the Kronecker delta. This is done numerically via singular value decomposition (SVD) [34] of the product of the internal and scattering orthonormal modes. For an incident field, the amplitudes of the internal principal modes are obtained by projecting the incident field along the scattered principal modes andvice versa. Hence, to evaluate Green’s functions we have to apply an incident field, F0, radiated by a dipole. The mode amplitudes are then defined as(3)anipx′=in′·F01-sn·in2,(4)anspx′=-sn′·F01-sn·in2,with in′≡in-(sn·in)sn and sn′≡sn-(sn·in)in. The principal modes are normalized so that in·in=sn·sn=1, 0≤in·sn=sn·in=≤1, and in′ is orthogonal to sn, and sn′ is orthogonal to in with in′·in=sn′·sn=1-(sn·in)2. To evaluate the radiative properties of these modes in the far field, the asymptotic forms of the scattering sources [29], for r→∞, are substituted when constructing the principal mode fields in Eq. (2).The procedure described here is general and can be applied to any particle in which the normal is defined at any point on the surface. For the azimuthally symmetric nanostructures considered here, numerical calculations are vastly sped up by forming internal and scattered fields whose tangent components have azimuthal angular dependenceexp(ilϕ), with l an integer number. For instance, fields with azimuthal dependence exp(±iϕ) are obtained by combining dipoles distributed along the z axis and (circularly) polarized along x and y, while z polarized dipoles distributed along the z axis have fields that do not depend on ϕ. This is suitable for the study of dipoles on the z axis or close to it. We note, however, that, in order to study dipoles further away from the z axis, sources with azimuthal angular dependence exp(ilϕ), with l>1, would be required.


## 3. Results and Discussion

In Figure1 we show the real and imaginary parts of the dielectric function, related to the refractive index and the absorption coefficient, respectively, for effective media with volume fractions of Al2O3 ranging from 5% to 40%, as a function of the wavelength from 210-600 nm. In the same figures we also show the refractive index and the absorption coefficient for pure Al and Al2O3. The effect of Al2O3 on the refractive index is straightforward: the higher the volume fraction is, the lower the absolute value of the refractive index is. From this, we can expect resonances to be shifted toward longer wavelengths as the volume fraction of Al decreases. The effect of Al2O3 on the absorption coefficient is more subtle and changes depending on the volume fraction and the wavelength. At longer wavelengths all volume fractions considered reduce the absorption coefficient with respect to the case of pure Al. However, for Al volume fractions below 95%, the absorption becomes higher at shorter wavelengths than for pure Al. The cross-over point where the effective medium absorption becomes higher than pure Al absorption moves toward longer wavelengths as the volume fraction of Al decreases. These features provide a qualitative explanation of the far-field response of spherical particles with different volume fractions.Figure 1
Complex dielectric function for Al + Al2O3 calculated with the effective medium approach. For the complex permittivity, ε=ε′+iε′′, we show the real, (a), and imaginary, (b), parts for particles with varying volume fractions of Al, where 0 corresponds to pure Al2O3 and 1 to pure Al particles.
(a) (b)In Figure2 we compare the ratio Pr/P0 for effective media spheres with radii of 60 nm lying on top of Al and SiO2 substrates. In both cases the UV peak in the scattered energy remains essentially unchanged for Al volume fractions of 90% or above. For an Al volume fraction of 80%, the peak is reduced and moves further toward long wavelengths. However, for even lower Al volume fractions, the increased absorption reduces the peak and pushes it back towards shorter wavelengths.Figure 2
Normalised power radiated by spherical particles on top of a substrate, illuminated by an electric dipole. For substrates comprised of (a) Al and (b) SiO2. All curves correspond to the same volume fractions indicated in Figure 1.
(a) (b)In Figure3 we show the ratio Pr/P0 for the same effective media spheres held 5 nm above Al and SiO2 substrates, and with the dipole source placed in the middle of the gap. In this case the difference between the two substrates is much more significant. The ratio Pr/P0 is an order of magnitude higher with the Al substrate and the corresponding enhancement in the far-field signal is of two orders of magnitudes for Al volume fractions higher than or equal to 80%, with actually a slight increase in the peak value for the volume fractions 95% and 90% with respect to the pure Al case. This is accompanied by a shift towards longer wavelengths similar to what was observed in the previous case. However, the higher losses for lower Al volume fractions result in a suppression of the UV peak that is no longer distinguishable. With the SiO2 substrate, the ratio Pr/P0 is an order of magnitude lower than with the Al substrate but the peaks remain distinguishable and move progressively toward longer wavelengths as the Al volume fraction is reduced.Figure 3
Normalised power radiated by spherical particles5 nm above a substrate, illuminated by an electric dipole. For substrates comprised of (a) Al and (b) SiO2. All curves correspond to the same volume fractions indicated in Figure 1.
(a) (b)


## 4. Conclusions

In conclusion, we have presented an effective media study of Al particles with Al2O3 oxidation layers on top of, and above, substrates of Al and SiO2. The results can be qualitatively explained by considering how the effective media absorption coefficient and refractive index depend on the volume fractions and the wavelengths. Our investigation of effective media spheres held above an Al substrate indicates that two orders of magnitude enhancement of the far-field radiation in the UV will take place also with oxidized Al particles as long as the volume fraction of Al is not below 80%. In order to better appreciate the practical implication of these results, note that, for the 60nm radius spheres considered here, the 95% Al volume fraction corresponds to an outer layer of Al2O3 of ~1nm, the 80% Al volume fraction corresponds to ~4.3 nm outer layer, and the 60% Al volume fraction corresponds to ~9.4 nm outer layer. These results, combined with the experimental findings [20] that the oxidation process in Al nanoparticles leads to stable layers of ~3nm thickness, suggest that gap-enhanced spectroscopy is a viable option for the detection of weakly fluorescent molecules emitting in the UV. For more detailed investigations of the effect of oxidation on fluorescence, including the reduction of life time due to near field interaction with nonradiative modes, it will be necessary to use a more detailed model of the multilayered surfaces, as effective media theories have been tested mainly with respect to far-field properties.



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*Source: 9687803-2019-07-01.xml*