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Near-Field Examination of Perovskite-Based Superlenses and Superlens-Enhanced Probe-Object Coupling

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Near-Field Examination of Perovskite-Based Superlenses and Superlens-Enhanced Probe-Object Coupling ARTICLE Received 28 Sep 2010 | Accepted 22 Feb 2011 | Published 22 Mar 2011 DOI: 10.1038/ncomms1249 Near-field examination of perovskite-based superlenses and superlens-enhanced probe-object coupling S.C. Kehr1,2,*, Y.M. Liu3,*, L.W. Martin1,4, P. Yu5, M. Gajek5, S.-Y. Yang5, C.-H. Yang5,6, M.T. Wenzel7, R. Jacob8, H.-G. von Ribbeck7, M. Helm8, X. Zhang1,3, L.M. Eng7 & R. Ramesh1,5 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. 1 Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA. 2 School of Physics and Astronomy, University of St Andrews, St Andrews, Fife KY16 9SS, UK. 3 NSF Nanoscale Science and Engineering Center, University of California, Berkeley, California 94720, USA. 4 Department of Materials Science and Engineering, University of Illinois, Urbana-Champaign, Urbana, Illinois 61801, USA. 5 Department of Physics, University of California, Berkeley, California 94720, USA. 6 Department of Physics, Institute for the NanoCentury, Korea Advanced Institute of Science and Technology (KAIST), Daejeon 305-701, Republic of Korea. 7 Institute of Applied Physics, Technische Universität Dresden, 01062 Dresden, Germany. 8 Institute of Ion Beam Physics and Materials Research, Helmholtz-Zentrum Dresden-Rossendorf, 01314 Dresden, Germany. *These authors contributed equally to this work. Correspondence and requests for materials should be addressed to S.C.K. (email: [email protected]). NATURE COMMUNICATIONS | 2:249 | DOI: 10.1038/ncomms1249 | www.nature.com/naturecommunications © 2011 Macmillan Publishers Limited. All rights reserved. ARTICLE NatUre cOMMUNicatiONS | DOI: 10.1038/ncomms1249 n 1968, Veselago theoretically discussed a material with a negative refractive index, as well as its extraordinary responses to electro­ magnetic waves, including negative refraction, reversed Doppler and I 1 Cerenkov effects and focusing with a planar lens . 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. 75° This opened the rapidly growing field of metamaterials, which present O 3 opportunities for new and remarkable applications in electromagnet­ B SrTi 3,4 5,6 7 8 eO 3 ics ranging from electrostatics via radio frequency , microwave A BiF 9 10 11–14 O 3 SrTi and terahertz to the infrared and optical regime . The experi­ SrRuO mental proofs of negative refraction and sub-diffraction-limited reso­ 3 lution by a negative-index planar lens were first reported in the GHz 15,16 17 18 3 range . Subsequently, it was shown for visible and infrared wave­ 10 5 lengths that the evanescent field information of transverse-magnetic ) SrRuO3 ε (TM) waves can be recovered using a medium with negative permitti­ BiFeO Im( SrTiO 3 ε 3 vity ( ) only. Such a lens is normally called a superlens, and substantial ) BiFeO ε 19 3 progress has been achieved in this rapidly developing area . 0.01 0 SL 15 Re( 2,19 A superlens is preferably realized by low-loss materials , SrTiO ) 3 ε 0 among which perovskite oxides are good candidates. In the mid- Re( infrared range, perovskite oxides show phonon resonances, which (x0.1) are located at slightly different wavelengths for related materials –30 –5 10 20 12 16 such as, for example, bismuth ferrite (BiFeO3) and strontium titan­ � (µm) � (µm) 20,21 ate (SrTiO3) . On the high-frequency side of these phonon reso­ nances, perovskites exhibit negative permittivities, which are suit­ Figure 1 | s-NSIM setup and perovskite properties. (a) Sketch of the able for superlens structures2,19. At these wavelengths, the intrinsic experimental setup including the superlens, the geometry at the near- absorption of light is small20,21. In addition, epitaxially grown oxides field probe (blue), and the free-electron laser light source. The superlens exhibit highly crystalline interfaces resulting in low scattering. Both consists of the layers A (BiFeO3) and B (SrTiO3) of thicknesses d and 2d the small intrinsic and low scattering losses of perovskites could sig­ (d = 200 nm), respectively. The objects to be imaged are SrRuO3 patterns nificantly improve the imaging resolution of superlenses. (orange rectangles) on a SrTiO3 substrate. All constituents of the superlens Perovskite oxides exhibit many intriguing properties such as are perovskite oxides that match in their crystalline structures resulting colossal magnetoresistance22, ferroelectricity23, superconductivity24 in low scattering at the highly crystalline interfaces. The near-field tip and spin-dependent transport25, which lead to numerous applica­ probes the evanescent fields on the image side of the lens. The superlens tions such as non-volatile memories26, microsensors and microactu­ is excited by an infrared free-electron laser, which is precisely tunable in ators27, as well as in nanoelectronics28. Piezoelectricity and ferroelec­ the range from 4 to 250 µm. (b) Imaginary and real parts of the dielectric tricity allow for the manipulation of geometrical dimension, electric constants ε of all constituents (SrRuO3 data determined by Fourier 29 polarization and dielectric properties by external electric fields . transform infrared spectroscopy, values for SrTiO3 and BiFeO3 taken from 20,21 Multiferroic perovskites, such as BiFeO3, exhibit ferroelectricity as literature , see Supplementary Fig. S1); (c) real parts of the dielectric well as magnetoelectric coupling29, thus providing a pathway for constants at the high-frequency side of their phonon resonances depicted additional degrees of tunability. Moreover, perovskites with match­ in b. The arrow indicates the wavelength at which superlensing is expected. ing lattice constants can be grown epitaxially on top of each other30,31, which allows one to combine their properties in multifunctional het­ 31–33 2 erostructures . These unique properties of perovskites may inspire air (εair = + 1) . At the two interfaces of the slab, coupled surface new functionalities of metamaterial structures such as tunability by polariton modes are excited, which amplify the evanescent electric external fields and novel designs for multifunctional circuits. fields arising from an object and transform them to the opposite Here, we study a new type of superlens for electric fields in the side of the lens2. The oxide-based superlenses in our study consist of mid-infrared based on the perovskite oxides BiFeO3 and SrTiO3. We layers of matched perovskites (see Fig. 1a). We structure a 50-nm- investigate the evanescent waves in the image plane of perovskite thick film of metallic perovskite strontium ruthenate (SrRuO3) on a superlenses by means of scattering-type near-field infrared micro­ SrTiO3 substrate by photo-lithography, acting as superlens objects scopy (s-NSIM)34,35. The combination with a free-electron laser with a lateral size down to 3 µm. To ensure a fixed distance between (FEL), which is precisely tunable in the wavelength (λ) regime from objects and the slab we add a layer A (thickness d, εA≅εair = + 1) on top 4 to 250 µm, enables us to address the polariton modes and study of the objects before we grow the actual superlens layer with εB≅ − 1 their lateral, vertical and spectral distribution. Such detailed char­ (thickness 2d). As layer A has a slightly different permittivity than acterizations are important to understand superlensing effect, but air this two-layer superlens is asymmetric. Hence, we also study they were not comprehensively conducted in previous work17,18. At a superlens with a symmetric design after adding an additional certain wavelengths we observe enhanced evanescent fields in the layer of material A (thickness d) on top. Superlensing is expected image plane as well as a resolution beyond the classical diffraction for such systems, when the real parts of the permittivities e(εA) limit. Moreover, we find that the evanescent fields show maxima at a and e(εB) have the same absolute values and opposite signs certain distance between the probe and the sample surface, for which e(εB) = − e(εA) < 0. Assuming the dielectric constants of the layers the vertical position depends on the wavelength. Comparisons with are similar to the ones described in literature20,21 (see Supplementary two-dimensional numerical simulations indicate that a superlens- Fig. S1), this superlensing condition is fulfilled at λ = 13.9 µm with enhanced coupling between probe and object causes this effect, the layers A and B being BiFeO3 and SrTiO3, respectively (Fig. 1b,c). which might be utilizable for controlling
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