A planar slab of negative-index material works as a superlens with sub-diffraction-limited resolution, as propagating waves are focused and, moreover, evanescent waves are reconstructed in the image plane. Here we demonstrate a superlens for electric evanescent fields with low losses using perovskites in the mid-infrared regime. The combination of near-field microscopy with a tunable free-electron laser allows us to address precisely the polariton modes, which are critical for super-resolution imaging. We spectrally study the lateral and vertical distributions of evanescent waves around the image plane of such a lens, and achieve imaging resolution of λ/14 at the superlensing wavelength. Interestingly, at certain distances between the probe and sample surface, we observe a maximum of these evanescent fields. Comparisons with numerical simulations indicate that this maximum originates from an enhanced coupling between probe and object, which might be applicable for multifunctional circuits, infrared spectroscopy and thermal sensors.
In 1968, Veselago theoretically discussed a material with a negative refractive index, as well as its extraordinary responses to electromagnetic waves, including negative refraction, reversed Doppler and Cerenkov effects and focusing with a planar lens1. Pendry revisited this idea 30 years later, showing that with such a planar lens one can create an image with a resolution beyond the conventional diffraction limit2. This opened the rapidly growing field of metamaterials, which present opportunities for new and remarkable applications in electromagnetics3,4 ranging from electrostatics5,6 via radio frequency7, microwave8 and terahertz9 to the infrared10 and optical regime11,12,13,14. The experimental proofs of negative refraction and sub-diffraction-limited resolution by a negative-index planar lens were first reported in the GHz range15,16. Subsequently, it was shown for visible17 and infrared18 wavelengths that the evanescent field information of transverse-magnetic (TM) waves can be recovered using a medium with negative permittivity (ɛ) only. Such a lens is normally called a superlens, and substantial progress has been achieved in this rapidly developing area19.
A superlens is preferably realized by low-loss materials2,19, among which perovskite oxides are good candidates. In the mid-infrared range, perovskite oxides show phonon resonances, which are located at slightly different wavelengths for related materials such as, for example, bismuth ferrite (BiFeO3) and strontium titanate (SrTiO3)20,21. On the high-frequency side of these phonon resonances, perovskites exhibit negative permittivities, which are suitable for superlens structures2,19. At these wavelengths, the intrinsic absorption of light is small20,21. In addition, epitaxially grown oxides exhibit highly crystalline interfaces resulting in low scattering. Both the small intrinsic and low scattering losses of perovskites could significantly improve the imaging resolution of superlenses.
Perovskite oxides exhibit many intriguing properties such as colossal magnetoresistance22, ferroelectricity23, superconductivity24 and spin-dependent transport25, which lead to numerous applications such as non-volatile memories26, microsensors and microactuators27, as well as in nanoelectronics28. Piezoelectricity and ferroelectricity allow for the manipulation of geometrical dimension, electric polarization and dielectric properties by external electric fields29. Multiferroic perovskites, such as BiFeO3, exhibit ferroelectricity as well as magnetoelectric coupling29, thus providing a pathway for additional degrees of tunability. Moreover, perovskites with matching lattice constants can be grown epitaxially on top of each other30,31, which allows one to combine their properties in multifunctional heterostructures31,32,33. These unique properties of perovskites may inspire new functionalities of metamaterial structures such as tunability by external fields and novel designs for multifunctional circuits.
Here, we study a new type of superlens for electric fields in the mid-infrared based on the perovskite oxides BiFeO3 and SrTiO3. We investigate the evanescent waves in the image plane of perovskite superlenses by means of scattering-type near-field infrared microscopy (s-NSIM)34,35. The combination with a free-electron laser (FEL), which is precisely tunable in the wavelength (λ) regime from 4 to 250 μm, enables us to address the polariton modes and study their lateral, vertical and spectral distribution. Such detailed characterizations are important to understand superlensing effect, but they were not comprehensively conducted in previous work17,18. At certain wavelengths we observe enhanced evanescent fields in the image plane as well as a resolution beyond the classical diffraction limit. Moreover, we find that the evanescent fields show maxima at a certain distance between the probe and the sample surface, for which the vertical position depends on the wavelength. Comparisons with two-dimensional numerical simulations indicate that a superlens-enhanced coupling between probe and object causes this effect, which might be utilizable for controlling polariton propagation.
The original superlens proposed by Pendry is a single slab of a material with ɛ=−1 surrounded by air (ɛair=+1)2. At the two interfaces of the slab, coupled surface polariton modes are excited, which amplify the evanescent electric fields arising from an object and transform them to the opposite side of the lens2. The oxide-based superlenses in our study consist of layers of matched perovskites (see Fig. 1a). We structure a 50-nm-thick film of metallic perovskite strontium ruthenate (SrRuO3) on a SrTiO3 substrate by photo-lithography, acting as superlens objects with a lateral size down to 3 μm. To ensure a fixed distance between objects and the slab we add a layer A (thickness d, ɛA≅ɛair=+1) on top of the objects before we grow the actual superlens layer with ɛB≅−1 (thickness 2d). As layer A has a slightly different permittivity than air this two-layer superlens is asymmetric. Hence, we also study a superlens with a symmetric design after adding an additional layer of material A (thickness d) on top. Superlensing is expected for such systems, when the real parts of the permittivities e(ɛA) and e(ɛB) have the same absolute values and opposite signs e(ɛB)=−e(ɛA)<0. Assuming the dielectric constants of the layers are similar to the ones described in literature20,21 (see Supplementary Fig. S1), this superlensing condition is fulfilled at λ=13.9 μm with the layers A and B being BiFeO3 and SrTiO3, respectively (Fig. 1b,c). Many other similarly suitable pairs of perovskites, such as PbZrxTi1–xO3 and SrTiO3, BiFeO3 and PbZrxTi1–xO3, BaTiO3 and SrTiO3, or BiFeO3 and BaTiO3, can be found at different wavelengths, implying the flexibility of perovskite superlenses in terms of the operation wavelength. Please note that other groups of dielectrics such as, for example, fluorides36,37 and simple oxides38 can form similar pairs for superlenses, which altogether cover an even larger wavelength range of operation.
We examine the enhanced evanescent fields on the image side of the lens with s-NSIM in combination with a FEL (see Fig. 1a and Methods), which allows for polariton-enhanced s-NSIM39,40. Surface polariton modes can be excited at the interface of two materials, which have permittivities of opposite signs41,42. In the studied wavelength range from 13.5 to 18.5 μm, the layers A and B of the perovskite-based superlenses show the following permittivities (see Fig. 1b,c) and corresponding polariton modes: when λ>16.5 μm we find (ɛB)<(ɛA)<0 and polariton modes are excited at the entire sample surface, being the interface between the toplayer and air. For λ<16.5 μm, it is (ɛB)<0<(ɛA) and polariton modes are created at both interfaces of layer B. As layer B is only 400-nm thick, these two modes are coupled, but are not necessarily localized.We observe an enhanced near-field signal, whenever a polariton mode is present at the position of the probe. However, only around the superlensing wavelength (ɛA≅−ɛB) the polartion modes are strongly localized and, hence, create a sub-diffraction-limited image of the objects on the opposite side of the lens. Please note that with near-field image, we refer to the image obtained by near-field microscopy. The contrast in these images arises from local sample properties and thus different coupling to the probe, allowing us to distinguish the different objects on the opposite side of the superlens with a sub-diffraction-limited resolution (see Methods)43.
Mid-infrared near-field imaging
When placing the probe at a distance of about 30 nm to the sample, which is scanned relatively to the probe position, we obtain the near-field response as well as the topography of the sample. The corresponding results are depicted in Figure 2 for similar object distributions with lateral sizes from 3×3 to 8×8 μm2 and three different samples, namely (a) structured SrRuO3 objects on a SrTiO3 substrate, (b) a symmetric superlens and (c) an asymmetric superlens without the top BiFeO3 layer.
The SrRuO3 objects without a lens (Fig. 2a) show a near-field response, which depends on the polarization and the incident angle of the impinging light with respect to the objects. The k-vector direction of the incident TM-polarized light is shown in the sketch and in the topography image in (a) and is the same for all scans depicted in Figure 2. Over a wide wavelength range in the infrared, the permittivity of SrRuO3 is much smaller than zero, resulting in an excellent, metal-like scattering behaviour. Consequently, the distance dependence of the near-field signal on SrRuO3 exhibits the same exponentially decaying character of the evanescent waves for all wavelengths (see middle panel of Fig. 2a). The metallic SrRuO3 structures show enhanced field intensities when their geometries match the wavelength, an effect which is well known in plasmonics44. Consequently, certain parts of the objects appear bright in the second- and third-harmonic near-field signals NF2Ω and NF3Ω (see Methods). In general NF2Ω is about three times larger than NF3Ω, with an interference-like background signal. To ensure pure near-field detection in the following, we will depict third-harmonic signals only.
For the symmetric superlens (Fig. 2b), at λ=17.5 μm we observe a near-field signal due to a non-localized polariton mode at the sample surface, showing no clear contrast between areas with and without SrRuO3 objects. Close to the superlensing wavelength, at around 14.6 μm, the evanescent fields are highly localized, resulting in a strong contrast reconstructing the SrRuO3 structures. Please note that even though the NSIM probe scans more than 800 nm higher above the SrRuO3 objects compared with the bare SrRuO3 case, the signal is about two times stronger because the coupled polariton modes at the interfaces enhance the near-field signals arising from the objects.
On the asymmetric superlens (Fig. 2c), we observe a similar, slightly blue-shifted response compared with the symmetric superlens, with non-localized polariton modes around 17.3 μm and superlensing with maximum contrast at around 14.1 μm. The signal on the asymmetric superlens is two times stronger than for the symmetric superlens, as the near-field probe is placed by 200 nm closer to the top SrTiO3 surface at which the polariton mode is excited.
With both superlenses we clearly resolve the buried SrRuO3 objects at the corresponding superlensing wavelengths. In the following, we discuss in detail the spectral response of both samples over a broad wavelength range.
Spectral response of the near-field signals
Our s-SNIM setup allows for studying polariton modes with different characteristics in the wavelength range from 13.5 to 18.4 μm. For the symmetric superlens (Fig. 3), we observe an enhanced localized signal for λ from 13.9 to 15.5 μm (Fig. 3a), close to the superlensing condition. The highest contrast is observed at 14.6 μm and the signal drops to zero for wavelength 1 μm smaller or larger than that. Note that areas without objects show a small negative signal in the superlensing regime, possibly due to evanescent waves on the substrate-superlens interface with opposite phase. At longer wavelengths, both layers, BiFeO3 and SrTiO3, show negative permittivities and a single polariton mode is excited at the top-most sample surface leading to an enhanced near-field signal on the entire sample area for λ>17 μm. Even though this signal is up to eight times higher than the superlensed signal, it does not show any image contrast except for some artifacts at the topography edges caused by scattering and errors in the distance control.
For the asymmetric superlenses (Fig. 4), we observe a localized near-field signal around the superlensing wavelength for 13.7 μm<λ<15.2 μm with a clear object-related contrast at 14.1 μm. In addition, the top-most layer SrTiO3 of this lens supports a non-localized polariton mode for 14 μm<λ<15.5 μm. In contrast to the symmetric case, in which this mode is spectrally well separated from the superlensing wavelength, for the asymmetric lens the wavelength regimes of superlensing and non-localized polariton overlap. Interestingly both modes respond with opposite phases resulting in a destructive superposition on the objects, which appear dark in the range from 14.5 to 15.2 μm. With increasing wavelength the non-localized mode dominates and the images are blurred.
The smallest structures resolved on the superlenses are about 3×3 μm2 in size and about 1 μm apart corresponding to a relative resolution of about λ/14. This sub-diffraction-limited image is created by the superlensing effect. Compared with the image of bare SrRuO3 objects (Fig. 2a), the superlensed image appears homogeneously bright as the incident light is scattered by the probe and from there directed towards the object (see Methods). In general, the imaging with s-NSIM is influenced by the probe and its vertical position as it is in particular observed in the cross-sections of Figure 5, which will be discussed in the following paragraphs.
Mid-infrared near-field cross-sections and spectroscopy
We focus on the asymmetric superlens to study the vertical distributions of evanescent waves. Similar measurements for the symmetric superlens can be found in the Supplementary Figure S2. Figure 5a depicts normalized vertical cross-sections on the image side of the sample for different wavelengths showing the near-field signal as a function of the probe-sample distance z and the position of the sample. The topography of the sample is reflected by the dark area on the bottom of the pictures with a 4-μm wide SrRuO3 object in the centre. For λ≥14.8 μm, the probe excites propagating polariton modes close to the SrTiO3 surface. Around the superlensing wavelength, for λ=14.5–13.5 μm, the evanescent field is localized on the object with decreasing signal and contrast for shorter wavelengths. For the latter wavelength regime, we observe an intriguing phenomenon: a maximum in the evanescent field appears at a certain distance z0 between tip and sample surface. Moreover, z0 increases with smaller wavelength and appears at distances of up to 150 nm from the sample surface at λ=13.5 μm. At first glance, this effect seems to be unexpected because the phonon-polariton mode is a confined surface mode, which exponentially decays from the interface. To make sure that this effect is not an artifact in our experimental setup, we compare these results with numerical simulations as discussed in the following.
Figure 5b shows the simulated data for a superlens consisting of the same constituents and geometry as in our experiments (see Methods). In these simulations we clearly observe the same effect as in Figure 5a, that is, the field maximum gradually shifts away from the sample surface when the wavelength decreases. This maximum has an asymmetric shape, locating on the right-hand side of the structure, which is illuminated from the left with an incident angle of 75°. The asymmetry might be formed by shadowing of the structure by the probe: when the probe is placed on the left side of the structure, it reflects the incident light and light hardly reaches the full structure; whereas when the probe is positioned on the right, the structure is completely illuminated by the beam. Compared with the experimental results, the simulations show some differences: First, the wavelengths as well as the z-position of the maximum are slightly shifted. This is likely due to the small discrepancy between the dielectric constants of the fabricated superlens layers and the data reported in the published literature20,21, which are used for the simulations (see Supplementary Fig. S1). Second, the near-field signal above the topographic step for λ≥14.5 μm in the simulation shows a saddle shape. The enhanced signal at the topographic steps is possibly caused by the sharp edges in the modelled geometry, which give rise to a highly nonlinear near-field because of localized corner polariton modes45. Please note that this effect is only relevant in the propagating polariton regime, whereas it is much less pronounced around the superlensing wavelengths as the polariton mode at the flat interface of the step becomes also highly localized. In the Supplementary Figure S3, we compare these results with corresponding simulations without the topographic step. We find very similar spectral, lateral and vertical response, but the enhanced signal at the edges disappears. This comparison verifies that the small topography on the sample interfaces because of the sample fabrication has negligible influence on the observed optical signals. The enhanced coupling of probe and object by the superlens layer is indeed correlated to the material property rather than the topological protrusion.
We further compare the results of experiment (Fig. 5c) and simulation (Fig. 5d) by analysing the absolute values of the maximum near-field signals with and without SrRuO3 object, NFw and NFw/o, respectively, as well as the resulting contrast V=(NFw−NFw/o)/(NFw+NFw/o). Without object (green curves) we observe maxima at 15.3 μm (c) and 14.5 μm (d) due to non-localized polariton modes, whereas on the SrRuO3 objects (red) an enhanced signal is observed for slightly shorter λ. The resulting contrasts (yellow) show maxima at 14 μm (c) and 13.3 μm (d), respectively, which is in good agreement with the predicted superlensing wavelength of 13.9 μm.
Numerical simulations of superlens-enhanced coupling
Why do we observe an enhanced signal at a certain distance to the sample surface? The coupled phonon-polariton modes, which create the sub-diffraction-limited image, result in a field which decreases exponentially with the distance. However, as we place a scattering probe on the image side, this probe itself acts as an object next to the superlens, creating additional fields at the position of the SrRuO3 objects. The probe-sample system therefore consists of two coupled scatterers with a superlens structure between both of them, showing a resonance as a function of the wavelength and the probe-sample distance as discussed in the following paragraphs.
Figure 6a plots the electric-field distribution of an asymmetric BiFeO3-SrTiO3 superlens with a line source in the object plane for different wavelengths and no probe on the image side. For wavelengths larger and smaller than the superlensing wavelength around λ=13.5 μm, we observe unconfined evanescent waves on the image side of the superlens due to the excitation of non-localized surface polariton modes at the SrTiO3-air interface. For λ=13.5 and 14 μm, the superlensing effect takes place with an enhanced confined field on the image side of the lens and localized polariton modes at both interfaces of the SrTiO3 layer. The superlensing effect is further verified by the transfer function simulation of electric fields. Figure 6b shows the isothermal contour of the transfer function of the asymmetric superlens (for the transfer function of the symmetric superlens see Supplementary Fig. S4). Around 13.5 μm, the amplitude of TM waves at the top interface of the superlens still maintains reasonably large, even for a tangential wave vector up to 10 k0 (Fig. 6c). In contrast, the field intensity dramatically decays for large wave vectors in a control sample, in which the 400 nm SrTiO3 film is replaced by a 400 nm BiFeO3 layer.
Figure 6a shows that the electric field at the SrTiO3-air interface possesses in all cases a maximum at the sample surface, reflecting the exponentially decaying behaviour of the polariton mode. The situation changes with the presence of a scattering probe on the imaging side of the sample. Figure 6d shows a simulation for the ideal case of two equally sized metal spheres, object and probe, separated by the two-layer superlens for a fixed wavelength of 14 μm and for different gaps z between the top scatterer (that is, the probe) and the sample surface. For small gaps z=25 nm, one observes a large field underneath the probe-scatterer Etip due to near-field enhancement as well as a localized polariton mode Eint at the interface between SrTiO3 and BiFeO3. When the gap is increased to 75 nm, Etip decreases, but Eint is much larger than that for z=25 nm, whereas both fields decrease with z for gaps larger than 100 nm.
In Figure 6e, we plot the z-dependence of Etip (green) and Eint (red), as well as of the integrated Poynting vector S (yellow) far away from the two spheres that corresponds to the scattered light intensity measured in our experiments. Etip decreases exponentially with the distance, because of the exponential decay of polariton modes at the sample surface. However, Eint and S show maxima at certain distances between tip and sample of 70 nm and 50 nm, respectively. The polariton modes at the interfaces of the superlens enhance the evanescent waves arising from the object. Hence, a larger field amplitude of polariton modes Eint for a certain probe-sample distance indicates enhanced superlensing of the coupled probe-object system for this position of the probe scatterer. Moreover, the scattered light (represented by S) from this system has a maximum around the same gap-size, which correlates the far-field observation with the enhanced coupling.
The theory of transformation optics46,47,48 states that a superlens with negative index of refraction distorts the optical space in a remarkable way: the space is folded by the superlens, with the object plane and the image plane (as well as a plane within the lens) at the same position in optical space46. If we place scatterers in both planes, one can consider them to be two induced dipoles located at exactly the same position in optical space, which therefore might lead to the observed enhanced coupling of both scatterers.
We note that a maximum in the image plane of a superlens was also observed earlier in the microwave range using loop antennas as source and detector49,50,51. The position of the maximum changed because of matched coupling between object and probe, when using detector antennas with different radii and different resistance load50. However, any dependences on the wavelength and on corresponding changes in the sample dielectric constants were not studied. It was proposed that this effect could be applicable for three-dimensional imaging50, which might be possible with the oxide-based superlens as well.
In this paper, we proposed, designed and demonstrated perovskite-based superlenses for electric fields. These materials are in particular suitable for superlenses in the infrared range, showing matching pairs of the real parts of their dielectric constants with opposite signs. Moreover, perovskites show low intrinsic absorption at the wavelengths of interest and different materials can be grown epitaxially on top of each other. Both effects lead to low losses in the superlens structure. As some perovskite oxides are ferroelectric (for example, BiFeO3 in the current study), a superlens consisting of these materials might be tunable by an external electric field.
We characterized the perovskite superlenses in both spectral and three-dimensional spatial domain. The near-field examination shows subwavelength resolution of λ/14 at the superlensing wavelength. Comparison of symmetric and asymmetric superlens show a stronger superlensed signal for the asymmetric case in which the probe is placed directly at the superlens interface. This finding is supported by the calculated transfer function of the asymmetric superlens, which shows a better performance compared with the symmetric case in terms of field enhancement and wave vector bandwidth.
In addition, we discussed the coupling of near-field probe and object, being placed on two opposite sides of a superlens. It is found that the coupling effect is strongly enhanced at phonon-polariton resonances and is dependent on the probe-object distance. These findings reflect the fact that in a system consisting of object, superlens and detecting probe coupling between all constituents takes place. The observed superlens-mediated interaction between two particles might allow for controlled enhanced-coupling effects. These effects could find potential applications in local thermal sensors as described by Shen et al.52 as well as in metamaterial-based multifunctional circuits53,54. We envision, for example, an enhanced transport of polaritons from particle to particle by these superlenses: a series of superlens-coupled particles can act as a polariton conductor with narrow bandwidth, which is determined by the superlensing material.
Growth and absorption losses of perovskite oxides
The various thin films were grown by pulsed laser deposition. Thin films of SrRuO3 were grown at 680 °C and films of BiFeO3 and SrTiO3 were grown at 700 °C in 100 mTorr of oxygen55. Following the growth of the SrRuO3 layer, features were defined using photo-lithography and samples were ion-milled to produce the objects; subsequently, BiFeO3 and SrTiO3 films were grown. Films were found to be single phase and fully epitaxial in all cases via X-ray diffraction and transmission electron microscopy.
To compare the absorption of our perovskite-based superlens with former materials used, we calculate the ratios n/κ with n and κ being the real and imaginary parts of the refractive index at the wavelengths for which superlensing is expected. Larger n/κ corresponds to less material absorption losses. For SrTiO3 this ratio is 12.7×10−2, three times larger than for SiC and silver, which both show a n/κ of about 4.2×10−2 at their corresponding superlensing wavelengths18,17. Note that the superlensing condition for the perovskite-based superlenses is fulfilled for , whereas for the SiC and silver superlens it was observed around ɛ≅−3. However, even when ɛSrTiO3≅−3 at λ=14.7 μm, we find n/κ=10.5×10−2 being much larger than for the other superlenses.
In s-NSIM, a scattering probe, namely a metal-coated atomic-force microscope tip with a typical radius of 50 nm, is placed close to the sample surface34,35. This probe transforms the evanescent fields into propagating waves, which can be detected in the far-field34,56. To separate the near-field from the much larger far-field signal, we use the method of higher-harmonic demodulation56,57: in tapping-mode atomic-force microscope, the distance between tip and sample is modulated with small amplitudes of about 30 nm at frequencies around Ω=150 kHz. On this scale, the far-field changes linearly with distance resulting in a modulation with the same frequency Ω. On the other hand, evanescent waves depend non-linearly on the distance, resulting in a modulation at nΩ (n=1,2,3,...). Hence, when filtering the modulated signal at nΩ with n≥2, at higher harmonics, we obtain near-field components only, with less far-field contributions for larger orders of n. If not stated otherwise, the near-field signals shown in this paper represent third-harmonic signals NF3Ω to ensure pure near-field examination. For comparisons at different wavelengths, we nomalize NF3Ω to the current laser power and to the spectral response of detector and optical elements in the beam path.
Our investigation was performed using the free-electron laser FELBE at the Helmholtz-Zentrum Dresden-Rossendorf (www.hzdr.de), Germany, which offers continuous tunability across a wavelength range of 4–250 μm at an average power of up to 10 W (delivered as a picosecond pulse train at a repetition rate of 13 MHz). In the 10–20 μm wavelength regime, the typical spectral full width at half maximum (FWHM) of the FEL is 50–100 nm.
Near-field interaction and probe-sample coupling
When imaging a superlensed signal by s-NSIM, the near-field probe can not be assumed to be a passive element only, but the coupling between probe and objects needs to be taken into account. The origin of the coupling lies in the optical interaction principle of NSIM, which results in the consequences for the NSIM examination of superlenses as discussed in the following.
In our s-NSIM and the similar one used in ref. 18, the probe-sample system is illuminated from the probe side and, hence, the initial near field is generated by the probe rather than by the sample. The function of the probe is two-fold: first, the evanescent waves arising from the probe illuminate the sample locally and excite modes in the sample and on its surface. Second, the probe senses the fields of the sample modes and transforms them by scattering into propagating waves, which can be detected in the far-field. This probe-sample interaction depends on the scattering behaviour of the probe, the local optical properties of the sample, as well as the distance between the probe and the sample surface. As a first-order approximation, it can be described by the dipole model introduced by Knoll and Keilmann56: here, the s-NSIM signal is described by scattering in the near-field coupled probe-object system represented through an effective polarizability. A more sophisticated approach describes the probe-sample interaction through higher-order modes58 showing the same qualitative results.
A critical point for successful NSIM measurements is that the probe properties and illumination are kept constant during the measurements, therefore the changes in the near-field signal are essentially caused by local sample properties. In our study, we particularly keep the position of the probe fixed while the sample is scanned to ensure constant illumination. The probe properties like material, geometry and orientation with respect to the polarization of the incident light are fixed as well. Hence, the observed contrast arises from changes in the sample only. The influence of probe or object properties are enhanced, when either one of the two is excited close to its resonances. In the mid-infrared, a metallic probe shows no distinct resonances, whereas the samples discussed in our work support polariton resonances. Hence, it is the sample that determines the NSIM signal, whereas the tip acts solely as a small optical dipole.
In the case of a superlens as the sample, the near-field interaction is extended: at the superlensing wavelength, the evanescent waves arising from the probe are transferred to the object plane. The objects are excited by these waves and generate additional evanescent fields, which are reconstructed by the superlens on the image side of the sample. Finally, the near-field signal at the image plane is transformed by the probe into detectable propagating waves. As the observed signal depends strongly on the properties of the superlens as well as the positions of both scatterers, probe and object, with respect to the superlens slab, we call this effect a superlens-enhanced probe-object interaction.
Besides the superlens-enhanced interaction between probe and objects, the probe can also interact with the surface layer of the superlens, which is in our case either BiFeO3 or SrTiO3 for the symmetric or asymmetric superlens, respectively. We observe enhanced near-field signals due to propagating polariton modes at the toplayer-air interface of the samples at wavelengths around 17 and 14.6 μm for symmetric and asymmetric superlens, respectively. Please note that, unlike the localized modes at the superlensing wavelength, this signal does not carry any information about the SrRuO3 objects (see Figs 3 and 4).
The numerical simulation results presented in the manuscript are all based on the commercial finite-element solver COMSOL 3.5. Because of memory limitation, the simulation is performed in two dimensions. The extremities of the simulation domain are assigned scattering properties, which essentially mimic the necessary open boundary conditions. We modify the size of simulation domain and (local) meshes to ensure that the field variation is less than 1%. Such a convergence of the numerical simulation verifies that the boundary condition and meshing are assigned properly. The total mesh number is up to 450,000. For a workstation with 32G RAM memory and two dual CPUs (2.66 GHz), each simulation takes less than 2 min to converge and reach the relative tolerance of 10−6.
To numerically retrieve the s-NSIM signal shown in Figure 5, iterative simulations with varying tip positions are performed by combining a Matlab script with COMSOL. The near-field probe is made by gold, whose dielectric constant is taken by fitting the data from Johnson and Christy59. The probe is modelled as a triangle, whose tip angle is about 22° and tip apex is a half sphere with the diameter of 100 nm. The superlens consists of layers of BiFeO3 and SrTiO3 with thicknesses of 200 and 400 nm, respectively, and the dielectric constants are taken from literature20,21. The SrRuO3 objects are assumed to be rectangles of 50 nm×4 μm with a dielectric constant of SrRuO3 determined by Fourier transform infrared spectroscopy (see Supplementary Fig. S1). The system is illuminated by monochromatic light with an incident angle of 75°. To study the response of the system, we calculate the electric-field distribution at all positions of the system. We observe a field enhancement underneath the tip and at the superlens interfaces because of polariton excitation. The scattering cross-sections (Fig. 5b) as measured in the experiment are related to the integrated Poynting vector over a solid angle about 70° from the tip apex. Such a simulation is repeated for different tip positions, in direct analogy to the scanning process. To simulate the higher-harmonic demodulation, we calculate the gradient of the Poynting vector to obtain the first-harmonic signal. Consequently, the gradient of the first harmonic reflects the second-harmonic signal and so on60.
How to cite this article: Kehr, S.C. et al. Near-field examination of perovskite-based superlenses and superlens-enhanced probe-object coupling. Nat. Commun. 2:249 doi: 10.1038/ncomms1249 (2011).
Veselago, V. The electrodynamics of substances with simultaneously negative values of ɛ and μ. Sov. Phys. Uspekhi 10, 509–514 (1968).
Pendry, J. B. Negative refraction makes a perfect lens. Phys. Rev. Lett. 85, 3966–3969 (2000).
Soukoulis, C. M., Linden, S. & Wegener, M. Negative refractive index at optical wavelengths. Science 315, 47–49 (2007).
Liu, Y. M. & Zhang, X. Metamaterials: a new frontier of science and technology. Chem. Soc. Rev.,, DOI: 10.1039/c0cs00184h (2011).
Wood, B. & Pendry, J. B. Metamaterials at zero frequency. J. Phys. Condens. Mat. 19, 076208 (2007).
Magnus, F. et al. A d.c. magnetic metamaterial. Nat. Mater. 7, 295–297 (2008).
Wiltshire, M. C. K. et al. Microstructured magnetic materials for RF flux guides in magnetic resonance imaging. Science 291, 849–851 (2001).
Smith, D. R., Padilla, W. J., Vier, D. C., Nemat-Nasser, S. C. & Schultz, S. Composite medium with simultaneously negative permeability and permittivity. Phys. Rev. Lett. 84, 4184–4187 (2000).
Yen, T. J. et al. Terahertz magnetic response from artificial materials. Science 303, 1494–1496 (2004).
Linden, S. et al. Magnetic response of metamaterials at 100 terahertz. Science 306, 1351–1353 (2004).
Enkrich, C. et al. Magnetic metamaterials at telecommunication and visible frequencies. Phys. Rev. Lett. 95, 203901 (2005).
Lezec, H. J., Dionne, J. A. & Atwater, H. A. Negative refraction at visible frequencies. Science 316, 430–432 (2007).
Valentine, J. et al. Three-dimensional optical metamaterial with a negative refractive index. Nature 455, 376–380 (2008).
Yao, J. et al. Optical negative refraction in bulk metamaterials of nanowires. Science 321, 930 (2008).
Shelby, R., Smith, D. & Schultz, S. Experimental verification of a negative index of refraction. Science 292, 77–79 (2001).
Grbic, A. & Eleftheriades, G. V. Overcoming the diffraction limit with a planar left-handed transmission-line lens. Phys. Rev. Lett. 92, 117403 (2004).
Fang, N., Lee, H., Sun, C. & Zhang, X. Sub-diffraction-limited optical imaging with a silver superlens. Science 22, 534–537 (2005).
Taubner, T., Korobkin, D., Urzhumov, Y., Shvets, G. & Hillenbrand, R. Near-field microscopy through a SiC superlens. Science 313, 1595 (2006).
Zhang, X. & Liu, Z. Superlenses to overcome the diffraction limit. Nat. Mater. 7, 435–441 (2008).
Spitzer, W., Miller, R. C., Kleinman, D. & Howarth, L. Far infrared dielectric dispersion in BaTiO3, SrTiO3, and TiO2 . Phys. Rev. 126, 1710–1721 (1962).
Kamba, S. et al. Infrared and terahertz studies of polar phonons and magnetodielectric effect in multiferroic BiFeO3 ceramics. Phys. Rev. B 75, 024403 (2007).
Jin, S. et al. Thousandfold change in resistivity in magnetoresistive La-Ca-Mn-O Films. Science 264, 413–415 (1994).
Ahn, C. H., Rabe, K. M. & Triscone, J.- M. Ferroelectricity at the nanoscale: local polarization in oxide thin films and heterostructures. Science 303, 488–491 (2004).
Wu, M. K. et al. Superconductivity at 93 K in a new mixed-phase Y-Ba-Cu-O compound system at ambient pressure. Phys. Rev. Lett. 58, 908–910 (1987).
Coey, J., Viret, M. & von Molnár, S. Mixed-valence manganites. Adv. Phys. 48, 167–293 (1999).
Scott, J. F. Ferroelectric Memories, Vol. 3, (Springer, 2000).
Setter, N. et al. Ferroelectric thin films: review of materials properties, and applications. J. Appl. Phys. 100, 051606 (2006).
Waser, R. Nanoelectronics and Information Technology (Wiley-CH, 2003).
Ramesh, R. & Spaldin, N. A. Multiferroics: progress and prospects in thin films. Nat. Mater. 6, 21–29 (2007).
Schlom, D. G. et al. Strain tuning of ferroelectric thin films. Annu. Rev. Mater. Res. 37, 589–626 (2007).
Schlom, D. G., Chen, L.- Q., Pan, X., Schmehl, A. & Zurbuchen, M. A. A thin film approach to engineering functionality into oxides. J. Am. Ceram. Soc. 91, 2429–2454 (2008).
Mathews, S., Ramesh, R., Venkatesan, T. & Benedetto, J. Ferroelectric field effect transistor based on epitaxial perovskite heterostructures. Science 276, 238–240 (1997).
Martin, L. W. et al. Multiferroics and magnetoelectrics: thin films and nanostructures. J. Phys. Condens. Mat. 20, 434220 (2008).
Betzig, E. & Trautman, J. K. Near-field optics: microscopy, spectroscopy, and surface modification beyond the diffraction limit. Science 257, 189–195 (1992).
Zenhausern, F., Martin, Y. & Wickramasinghe, H. K. Scanning interferometric apertureless microscopy: optical imaging at 10 angstrom resolution. Science 269, 1083–1085 (1995).
Axe, J. D., Gaglianello, J. W. & Scardefield, J. E. Infrared dielectric properties of cadmium fluoride and lead fluoride. Phys. Rev. 139, A1211–A1215 (1965).
Ramos, C. A., Lederman, D., King, A. R. & Jaccarino, V. New antiferromagnetic insulator superlattices: structural and magnetic characterization of (FeF2)m(CoF2)n . Phys. Rev. Lett. 65, 2913–2915 (1990).
Borchers, J. A., Carey, M. J., Erwin, R. W., Majkrzak, C. F. & Berkowitz, A. E. Spatially modulated antiferromagnetic order in CoO/NiO Superlattices. Phys. Rev. Lett. 70, 1878–1881 (1993).
Kehr, S. C. et al. Anisotropy contrast in phonon-enhanced apertureless near-field microscopy using a free-electron laser. Phys. Rev. Lett. 100, 256403 (2008).
Schneider, S. C. et al. Impact of optical in-plane anisotropy on near-field phonon polariton spectroscopy. Appl. Phys. Lett. 90, 143101 (2007).
Dionne, J. A., Sweatlock, L. A., Atwater, H. A. & Polman, A. Planar metal plasmon waveguides: frequency-dependent dispersion, propagation, localization, and loss beyond the free electron model. Phys. Rev. B 72, 075405 (2005).
Raether, H. Surface Plasmons: On Smooth and Rough Surfaces and on Gratings (Springer, 1988).
Novotny, L. & Hecht, B. Principles of Nano-Optics (University Press, 2006).
Mühlschlegel, P., Eisler, H.- J., Martin, O. J. F., Hecht, B. & Pohl, D. W. Resonant optical antennas. Science 308, 1607–1608 (2005).
Berini, P. Plasmon-polariton waves guided by thin lossy metal films of finite width: bound modes of symmetric structures. Phys. Rev. B 61, 10484–10503 (2000).
Leonhardt, U. & Philbin, T. G. General relativity in electrical engineering. New J. Phys. 8, 247 (2006).
Leonhardt, U. Optical conformal mapping. Science 312, 1777–1780 (2006).
Pendry, J. B., Schurig, D. & Smith, D. R. Controlling electromagnetic fields. Science 312, 1780–1782 (2006).
Guve, K., Aydin, K., Alici, K. B., Soukoulis, C. M. & Ozbay, E. Spectral negative refraction and focusing analysis of a two-dimensional left-handed photonic crystal lens. Phys. Rev. B 70, 205125 (2004).
Mesa, F., Freire, M. J., Marqués, R. & Baena, J. D. Three-dimensional superresolution in metamaterial slab lenses: experiment and theory. Phys. Rev. B 72, 235117 (2005).
Freire, M. J. & Marqués, R. Planar magnetoinductive lens for three-dimensional subwavelength imaging. Appl. Phys. Lett. 86, 182505 (2005).
Shen, S., Narayanaswamy, A. & Chen, G. Surface phonon polaritons mediated energy transfer between nanoscale gaps. Nano Lett. 9, 2909–2913 (2009).
Engheta, N., Salandrino, A. & Alu, A. Circuit elements at optical frequencies: nanoinductors, nanocapacitors, and nanoresistors. Phys. Rev. Lett. 95, 095504 (2005).
Engheta, N. Circuits with light at nanoscales: optical nanocircuits inspired by metamaterials. Science 317, 1698–1702 (2007).
Chu, Y.- H. et al. Domain control in multiferroic BiFeO3 through substrate vicinality. Adv. Mater. 19, 2662–2666 (2007).
Knoll, B. & Keilmann, F. Enhanced dielectric contrast in scattering-type scanning near-field optical microscopy. Opt. Commun. 182, 321–328 (2000).
Wurtz, G., Bachelot, R. & Royer, P. A reflection-mode apertureless scanning near-field optical microscope developed from a commercial scanning probe microscope. Rev. Sci. Instrum. 69, 1735–1743 (1998).
Renger, J., Grafström, S., Eng, L. M. & Hillenbrand, R. Resonant light scattering by near-field-induced phonon polaritons. Phys. Rev. B 71, 75410 (2005).
Johnson, P. B. & Christy, R. W. Optical constants of the noble metals. Phys. Rev. B 6, 4370–4379 (1972).
Hillenbrand, R. & Keilmann, F. Complex optical constants on a subwavelength scale. Phys. Rev. Lett. 85, 3029–3032 (2000).
We thank G. Bartal, Y. Wang, X. Yin, L. Zeng and J. Seidel for fruitful discussions. We acknowledge the technical assistance of the FELBE team at Helmholtz-Zentrum Dresden-Rossendorf and thank them for their dedicated support. The work at Berkeley was supported by the Director, Office of Science, Office of Basic Energy Sciences, Materials Sciences Division of the US Department of Energy under contract No. DE-AC02-05CH11231. S.C.K was supported by the German Academic Exchange Service DAAD. Y.M.L and X. Z. acknowledges funding support from US Army Research Office (ARO) MURI program 50432-PH-MUR. M.T.W., R.J., H.-G.v.R., M.H. and L.M.E. gratefully acknowledge the funding by the German Science Foundation DFG (projects HE 3352/4-1 and EN 434/22-1). M.T.W. and H.-G.v.R. were supported by the EU-STREP Project in FP7 PLAISIR.
The authors declare no competing financial interests.
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Kehr, S., Liu, Y., Martin, L. et al. Near-field examination of perovskite-based superlenses and superlens-enhanced probe-object coupling. Nat Commun 2, 249 (2011). https://doi.org/10.1038/ncomms1249
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