Abstract:Highly ordered two-dimensional arrays of monodisperse coinage metal nanowires embedded in an alumina matrix have been prepared. When light is propagating in the direction of the long axis of the nanowire, plasmon-enhanced absorption and light guidance of the nanowire were observed by optical microspectroscopy and scanning near-field optical spectroscopy and compared to Mie scattering theory. By selectively dissolving the matrix at a constant etching rate, we detected in situ and ex situ the surface-enhanced Ra… Show more
“…This can be explained by the fact that the gold helices are not physically connected with each other and that the spacing between them is larger than their evanescent field if the light is incident in the direction of their long axes. Similar results were observed by other groups measuring the transmission through silver or gold nanowire arrays in AAO matrices [38]. The refractive index of gold was derived from the analytical model of Etchegoin et al [39] and matches experimental data reported by Johnson and Christy [40].…”
Shape-defining hard templates containing arrays of aligned cylindrical nanopores have been exploited as a powerful tool in the synthesis of tubular and solid, rod-like one-dimensional (1D) nanostructures consisting of inorganic and polymeric materials. Gaining control over the mesoscopic fine structure in the 1D nanostructures thus obtained has remained challenging. However, it is easy to conceive that their properties largely depend on internal features characterized by mesoscopic length scales. The self-assembly of block copolymers inside nanopores with hard confining pore walls can be exploited to rationally generate 1D nanostructures with internal self-assembled mesoscopic fine structures. These self-assembled mesoscopic fine structures can be converted to mesopores, into which functional inorganic materials can be deposited. Thus, 1D nanostructures that contain replicas of helical mesopores consisting of functional inorganic materials could be obtained. The complex shapes of the inorganic entities might add additional functionalities to those associated with the bulk inorganic material and with the anisotropy of plain 1D nanostructures. In this way, helical structure motifs can be generated that may exhibit specific optical properties, such as circular dichroism, as shown by simulations
“…This can be explained by the fact that the gold helices are not physically connected with each other and that the spacing between them is larger than their evanescent field if the light is incident in the direction of their long axes. Similar results were observed by other groups measuring the transmission through silver or gold nanowire arrays in AAO matrices [38]. The refractive index of gold was derived from the analytical model of Etchegoin et al [39] and matches experimental data reported by Johnson and Christy [40].…”
Shape-defining hard templates containing arrays of aligned cylindrical nanopores have been exploited as a powerful tool in the synthesis of tubular and solid, rod-like one-dimensional (1D) nanostructures consisting of inorganic and polymeric materials. Gaining control over the mesoscopic fine structure in the 1D nanostructures thus obtained has remained challenging. However, it is easy to conceive that their properties largely depend on internal features characterized by mesoscopic length scales. The self-assembly of block copolymers inside nanopores with hard confining pore walls can be exploited to rationally generate 1D nanostructures with internal self-assembled mesoscopic fine structures. These self-assembled mesoscopic fine structures can be converted to mesopores, into which functional inorganic materials can be deposited. Thus, 1D nanostructures that contain replicas of helical mesopores consisting of functional inorganic materials could be obtained. The complex shapes of the inorganic entities might add additional functionalities to those associated with the bulk inorganic material and with the anisotropy of plain 1D nanostructures. In this way, helical structure motifs can be generated that may exhibit specific optical properties, such as circular dichroism, as shown by simulations
“…As a thumb of rule, the distribution in the length of electrodeposited nanowires in porous template channels increases with the wire length. Therefore, in order to have uniform length MNWs for SERS studies either the deposition time must be shortened, yielding nanodots rather than nanowires [Kartopu et al, 2006;Wang et al, 2006], or the initially long MNWs must be levelled by an appropriate post treatment, such as mechanical polishing [Kartopu et al, 2008b] and ion milling [Sauer et al, 2005]. In the latter case, a chemical etching may be applied to increase the exposed area of nanowires ( Fig.…”
Section: Substrates For Surface-enhanced Raman Scatteringmentioning
confidence: 99%
“…An in situ chemical etching (in dilute H 3 PO 4 ) is used to probe the temporal change in the SERS spectrum of analyte molecules adsorbed on MNWs/Ag nanowires (Fig. 15c) [Sauer et al, 2005]. The signal intensity first increases to a maximum and then decreases rapidly before it completely vanishes.…”
Section: Substrates For Surface-enhanced Raman Scatteringmentioning
“…8 Other deposition techniques support the growth of nanostructures using grated substrates or embedded matrices. 9 Still other techniques confine material to 1-D tubular structures [10][11] or arrange granular material in a linear fashion. [12][13] The VLS process, one of the methods frequently applied to grow 1-D ZnO nanostructures, was first described in 1965 for the Au-assisted growth of Si whiskers, 14 and is currently a well-understood system.…”
In this report, we have investigated the Au‐assisted growth of ZnO nanowires at a low temperature (550 °C) using low melting point Zn metal as a source. We supplied various Ar gas flow rate to carry Zn vapor onto Au catalysts coated Si(100) substrates to grow ZnO nanowires. When a high Ar gas flow rate was supplied, a large amount Zn vapor was carried onto the substrate and reacted with O2 to form a ZnO buffer layer covering the surface of the Au catalysts. This ZnO buffer layer has a highly c‐axis preferential orientation, which helps form vertically aligned ZnO nanowire arrays. In this condition, no Au catalysts appeared on the tips of the ZnO nanowires. When low Ar gas flow rate was supplied, Zn vapor is too low to form ZnO buffer layer on the surface of Au catalysts. From TEM analysis, we can observe that Au catalysts remain solid during growth. The detail growth mechanism of ZnO nanowires with various carrier flow rates was studied by field‐emission electron microscopy (FE‐SEM), transmission electron microscopy (TEM) and X‐ray diffraction (XRD).
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