Nanoscale patterning of metal nanoparticle distribution in glasses
© Sinev et al.; licensee Springer. 2013
Received: 9 April 2013
Accepted: 19 May 2013
Published: 1 June 2013
We show that electric field imprinting technique allows for patterning of metal nanoparticles in the glass matrix at the subwavelength scale. The formation of glass-metal nanocomposite strips with a width down to 150 nm is demonstrated. The results of near-field microscopy of imprinted patterns are in good agreement with the performed numerical modeling. Atomic force microscopy reveals that imprinting also results in the formation of nanoscale surface profile with the height going down with the decrease of the strip width. The experiments prove the applicability of this technique for the fabrication of nanoscale plasmonic components.
Nowadays, plasmonic materials and structures are the subject of wide-scale studies. In addition to metals, new materials like wide bandgap semiconductors [1, 2] and glass-metal nanocomposites (GMN) [3–5], that are glasses embedded with metal nanoparticles, have recently been implemented in plasmonics. Since the dielectric function and, consequently, the propagation of surface plasmon polariton modes in the latter materials can be controlled by varying the volume fraction, size, and type of metal inclusions [5–7], the flexibility of GMN makes them attractive for plasmonics.
The required dimensions of the majority of plasmonic structures [8–10] are in tens of nanometers scale, which compels the use electron beam lithography (EBL) in their fabrication. That is why the search for an alternative cost-effective technique for their manufacturing is of interest.
In , nanoimprint lithography was proposed for the fabrication of plasmonic circuits based on metal films, and the usability of electric field imprinting (EFI) process for nanostructuring of GMN has recently been shown . Electric field imprinting of GMN is based on electric-field-assisted dissolution [12–15] (EFAD) of nanoparticles in glass matrix at elevated temperature. This is to control their spatial distribution via application of DC voltage to the GMN using a structured electrode (stamp). The imprinting enables multiple replication of the stamp image to GMN [14, 16], that is, mass fabrication of GMN structures. This paper is focused on the characterization of the resolution of GMN EFI using atomic force microscopy (AFM) and scanning near-field optical microscopy (SNOM).
Silver-based GMN sample was prepared in a plate of commercial 1-mm thick soda-lime glass using silver-to-sodium ion exchange followed by hydrogen-assisted reduction of silver ions and metal clustering as it was reported elsewhere . According to the results of our previous studies , after such processing, the vast majority of the formed silver nanoparticles is located within 200- to 300-nm layer buried under the sample surface at the depth of approximately 100 nm, the diameter of the nanoparticles being around 4 nm. We characterized optical extinction of the sample with optical absorption spectroscopy. The spectra were measured with UV-vis Specord 50 spectrometer (Analytyk Jena, Konrad-Zuse-Strasse, Jena, Germany).
To find the linewidth achievable in the EFI, a profiled glassy carbon  stamp with the set of 350-nm deep grooves of 100, 150, 200, 250, 300, 350, 400, 450, 500, and 600 nm in width was fabricated with EBL. The distance between the grooves was equal to 2 μ m. The widths and depths of the grooves were checked with scanning electron microscopy (SEM), Zeiss Leo 1550 Field Emission Scanning Electron Microscope (Carl Zeiss Microscopy GmbH, Carl-Zeiss-Strasse, Oberkochen Germany). The stamp was used as the anode in the EFI of both the GMN sample and the plate of virgin glass. The imprinting was carried out at 250°C under 600 V DC.
The imprinted structure was studied using AFM and SNOM techniques using AIST-NT SmartSPM scanning probe microscope and AIST-NT CombiScope Scanning Probe Microscope with optical fiber probe (AIST NT Inc., Novato, CA USA). Numerical modelling was carried out using COMSOL Multiphysics®; package (COMSOL, Inc., Burlington, MA, USA).
Results and discussion
The poling of GMN using the stamp, scanning electron image of a part of which is shown in Figure 1b, has resulted in the dissolution of silver nanoparticles everywhere except the regions beneath the stamp grooves, that is in the formation of GMN strips (see the inset in Figure 1a). In the virgin glass, the imprinting resulted in poling of the glass  except the strips beneath the stamp grooves.
Although the hump formation in the virgin glass and in the GMN, as well as the EFAD of nanoparticles in GMN is due to the ionic redistribution under external voltage , there is no evidence of their exact correspondence. To characterize the nanoparticle distribution, we resorted to near-field optical microscopy operating in transmission mode (the sample was excited through the objective, and scattered light was collected with fiber probe). The setup allowed us to scan samples both in contact with the surface and in plane scan mode. The latter regime allows scanning within a plane calculated relying on the sample surface with the preselected lift value. In the experiments, the electric field vector of the incident light wave was directed perpendicularly to the imprinted strips. The SNOM measurements of the patterned glass and the GMN sample were carried out at three laser wavelengths: 633 (red), 532 (green), and 405 nm (violet). The optical absorption of GMN for these wavelengths respectively increased, having the resonance at 415 nm (see Figure 1a, the used wavelengths are marked with arrows), while the virgin glass sample absorption varied with probing wavelength very slightly.
The results of 2D scanning of imprinted GMN sample in plane scan mode with 100-nm lift are shown in Figure 2c,d,e. One can see the imprinted structures easily, the optical contrast at the violet wavelength corresponding to the SPR absorption being much stronger than one at green and red wavelengths. The difference in the intensities measured in contact and in plane scan modes was not significant; this could be due to the fact that the layer of nanoparticles in GMN can be buried about 100 nm below the surface . The intensity profiles obtained after averaging of 2D contact mode scans of the imprinted virgin glass and GMN sample along the strips are shown in Figure 3. The measurements of the glass sample at all three wavelengths and the measurements of the GMN sample at red and green wavelengths showed optical signal intensity modulation with maximum amplitude of about 10%. At the same time, the intensity dips with the amplitude up to 50% were observed at the violet laser wavelength which corresponds to the SPR of silver nanoparticles in GMN strips that survived under the stamp grooves. The amplitude of the intensity modulation is constant when the GMN strip width exceeds 500 to 600 nm and decreases with the strip width at all probing wavelengths used.
Generally, the observed modulation could be due to local light absorption in the strips, to the interference of incident light wave with the wave scattered by the surface humps, and to the light wave phase shift difference in poled (out of strips) and unpoled regions of the glass sample. The latter effect may come from the refractive index change in poled glass, which amounts to Δ n∼−(0.03−0.09) . Basing on close magnitudes of the modulation as well as the shape of the SNOM signal measured on the glass and on the GMN at red (633 nm) and green (532 nm) wavelengths, we can conclude that far from the SPR, where GMN absorption is low and the refractive index of GMN is close to the one of the glass, the registered near-field intensity modulation in GMN and in the glass has the same nature. On the contrary, much stronger intensity modulation is observed at 405 nm (see Figure 3), corresponding to the SPR light absorption, which proves the presence of silver nanoparticles in the strips beneath the stamp grooves. One can see in Figure 3 that relevant signal drop for 150 nm GMN strip is observed; however, we cannot claim imprinting of 100 nm strip as the signal was smeared after the averaging of 2D data. Thus, the formation of surface profile of 100 nm linewidth element was not followed by the modulation of nanoparticle concentration at the same scale.
Finally, in this study, we used a scanning near-field optical microscopy to characterize the spatial resolution of the EFI technique applied to the glass-metal nanocomposites. For this purpose, we replicated a set of nanostrips differing in width to the silver-based glass-metal nanocomposite sample using a profiled glassy carbon stamp as the anodic electrode. Our near-field measurements showed significant dependence of optical transmission of the imprinted strips on the excitation wavelength. In contrast to relatively low modulation of optical signal at 633- and 532-nm wavelengths, the transverse scan of the intensity profile at 405 nm contained sharp dips corresponding to the silver nanoparticle surface plasmon resonance absorption in the imprinted strips. Numerical simulations of near-field signal under the assumption that the nanoparticle concentration is equal in all of the strips showed good agreement with our experiment. Finally, this study proved that glass-metal nanocomposite elements with linewidth down to at least 150 nm can be fabricated with electric field imprinting technique.
ISS is a Masters degree student of St. Petersburg Academic University and an assistant at the National Research University of Information Technologies, Mechanics and Optics. MIP is a former PhD student of the University of Eastern Finland; he defended the thesis in April 2013. AKS is a PhD degree holder and is a junior research fellow at the National Research University of Information Technologies, Mechanics and Optics; he defended his thesis at Ioffe Institute in December 2011. VVR has graduated from St. Petersburg Academic University in 2012. AAL holds a DrSci degree and Professor positions in St. Petersburg Academic University and St. Petersburg State Polytechnical University.
This study was supported by Ministry of Education and Science of the Russian Federation (projects #11.G34.31.0020 and #14.B37.21.0752), the Russian Foundation for Basic Research (project #12–02-91664 and #12–02-31920), and EU (FP7 projects ‘NANOCOM’ and ‘AN2’).
- Naik GV, Kim J, Boltasseva A: Oxides and nitrides as alternative plasmonic materials in the optical range. Opt Mater Express 2011, 1(6):1090. 10.1364/OME.1.001090View ArticleGoogle Scholar
- Noginov MA, Gu L, Livenere J, Zhu G, Pradhan AK, Mundle R, Bahoura M, Barnakov YA, Podolskiy VA: Transparent conductive oxides: plasmonic materials for telecom wavelengths. Appl Phys Lett 2011, 99(2):021101. 10.1063/1.3604792View ArticleGoogle Scholar
- Shi Z, Piredda G, Liapis AC, Nelson MA, Novotny L, Boyd RW: Surface-plasmon polaritons on metal–dielectric nanocomposite films. Opt Lett 2009, 34(22):3535–3537. 10.1364/OL.34.003535View ArticleGoogle Scholar
- Sardana N, Heyroth F, Schilling J: Propagating surface plasmons on nanoporous gold. J Opt Soc Am B 2012, 29(7):1778. 10.1364/JOSAB.29.001778View ArticleGoogle Scholar
- Lu D, Kan J, Fullerton EE, Liu Z: Tunable surface plasmon polaritons in Ag composite films by adding dielectrics or semiconductors. Appl Phys Lett 2011, 98(24):243114. 10.1063/1.3600661View ArticleGoogle Scholar
- Bruggeman D: Dielectric constant and conductivity of mixtures of isotropic materials. Ann Phys (Leipzig) 1935, 24: 636–679.View ArticleGoogle Scholar
- Garnett JM: Colors in material glasses and metal films. Trans Roy Soc 1904, 53: 385.View ArticleGoogle Scholar
- Bozhevolnyi SI, Volkov VS, Devaux E, Laluet JY, Ebbesen TW: Channel plasmon subwavelength waveguide components including interferometers and ring resonators. Nature 2006, 440(7083):508. 10.1038/nature04594View ArticleGoogle Scholar
- Krasavin AV, Zayats AV: Silicon-based plasmonic waveguides. Opt Expr 2010, 18(11):11791–11799. 10.1364/OE.18.011791View ArticleGoogle Scholar
- Boltasseva A: Plasmonic components fabrication via nanoimprint. J Opt A: Pure Appl Opt 2009, 11(11):114001. 10.1088/1464-4258/11/11/114001View ArticleGoogle Scholar
- Lipovskii AA, Melehin VG, Petrov MI, Svirko YP: Thermal electric field imprinting lithography: fundamentals and applications. In Lithography: Principles, Processes and Materials. Edited by: Hennessy TC. New York: Nova Science; 2011:284–284.Google Scholar
- Deparis O, Kazansky PG, Abdolvand A, Podlipensky A, Seifert G, Graener H: Poling-assisted bleaching of metal-doped nanocomposite glass. Appl Phys Lett 2004, 85(6):872. 10.1063/1.1779966View ArticleGoogle Scholar
- Podlipensky A, Abdolvand A, Seifert G, Graener H, Deparis O, Kazansky PG: Dissolution of silver nanoparticles in glass through an intense dc electric field. J Phys Chem B 2004, 108(46):17699–17702. [http://pubs.acs.org/doi/abs/10.1021/jp045874c]  10.1021/jp045874cView ArticleGoogle Scholar
- Lipovskii AA, Kuittinen M, Karvinen P, Leinonen K, Melehin VG, Zhurikhina VV, Svirko YP: Electric field imprinting of sub-micron patterns in glass-metal nanocomposites. Nanotechnology 2008, 19(41):415304. 10.1088/0957-4484/19/41/415304View ArticleGoogle Scholar
- Brunkov PN, Melekhin VG, Goncharov V, Lipovskii AA, Petrov MI: Submicron-resolved relief formation in poled glasses and glass-metal nanocomposites. Tech Phys Lett 2008, 34(12):1030. 10.1134/S1063785008120122View ArticleGoogle Scholar
- Abdolvand A, Podlipensky A, Matthias S, Syrowatka F, Gösele U, Seifert G, Graener H: Metallodielectric two-dimensional photonic structures made by electric-field microstructuring of nanocomposite glasses. Adv Mater 2005, 17(24):2983–2987. 10.1002/adma.200501492View ArticleGoogle Scholar
- Afrosimov VV, Ber BY, Zhurikhina VV, Zamoryanskaya MV, Kazantsev DY, Kolesnikova EV, Lipovskii AA, Melekhin VG, Petrov MI: Mass transfer in thermo-electric-field modification of glass-metal nanocomposites. Tech Phys 2010, 55(11):1600. 10.1134/S1063784210110095View ArticleGoogle Scholar
- Harris PJF: Fullerene-related structure of commercial glassy carbons. Philos Mag 2004, 84(29):3159–3167. [http://www.tandfonline.com/doi/abs/10.1080/14786430410001720363]  10.1080/14786430410001720363View ArticleGoogle Scholar
- Takagi H, Miyazawa S, Takahashi M, Maeda R: Electrostatic imprint process for glass. Appl Phys Expr 2008, 1: 024003.View ArticleGoogle Scholar
- Leitner M, Peterlik H, Sepiol B, Graener H, Beleites M, Seifert G: Uniformly oriented, ellipsoidal nanovoids in glass created by electric-field-assisted dissolution of metallic nanoparticles. Phys Rev B 2009, 79(15):1.View ArticleGoogle Scholar
- Sokolov K, Melehin V, Petrov M, Zhurikhina V, Lipovskii A: Spatially periodical poling of silica glass. J Appl Phys 2012, 111(10):104307. 10.1063/1.4714350View ArticleGoogle Scholar
- Petrov MI, Melehin VG, Zhurikhina VV, Svirko YP, Lipovskii AA: Dissolution of metal nanoparticles in glass under a dc electric field. J Phys D: Appl Phys 2013, 46(4):045302. 10.1088/0022-3727/46/4/045302View ArticleGoogle Scholar
- Dussauze M, Kamitsos E, Fargin E, Rodriguez V: Refractive index distribution in the non-linear optical layer of thermally poled oxide glasses. Chem Phys Lett 2009, 470(1–3):63.View ArticleGoogle Scholar
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.