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      Large‐Area Periodic Arrays of Atomically Flat Single‐Crystal Gold Nanotriangles Formed Directly on Substrate Surfaces

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          The Optical Properties of Metal Nanoparticles:  The Influence of Size, Shape, and Dielectric Environment

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            Electromagnetic fields around silver nanoparticles and dimers.

            We use the discrete dipole approximation to investigate the electromagnetic fields induced by optical excitation of localized surface plasmon resonances of silver nanoparticles, including monomers and dimers, with emphasis on what size, shape, and arrangement leads to the largest local electric field (E-field) enhancement near the particle surfaces. The results are used to determine what conditions are most favorable for producing enhancements large enough to observe single molecule surface enhanced Raman spectroscopy. Most of the calculations refer to triangular prisms, which exhibit distinct dipole and quadrupole resonances that can easily be controlled by varying particle size. In addition, for the dimer calculations we study the influence of dimer separation and orientation, especially for dimers that are separated by a few nanometers. We find that the largest /E/2 values for dimers are about a factor of 10 larger than those for all the monomers examined. For all particles and particle orientations, the plasmon resonances which lead to the largest E-fields are those with the longest wavelength dipolar excitation. The spacing of the particles in the dimer plays a crucial role, and we find that the spacing needed to achieve a given /E/2 is proportional to nanoparticle size for particles below 100 nm in size. Particle shape and curvature are of lesser importance, with a head to tail configuration of two triangles giving enhanced fields comparable to head to head, or rounded head to tail. The largest /E/2 values we have calculated for spacings of 2 nm or more is approximately 10(5). (c) 2004 American Institute of Physics
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              Controlling anisotropic nanoparticle growth through plasmon excitation.

              Inorganic nanoparticles exhibit size-dependent properties that are of interest for applications ranging from biosensing and catalysis to optics and data storage. They are readily available in a wide variety of discrete compositions and sizes. Shape-selective synthesis strategies now also yield shapes other than nanospheres, such as anisotropic metal nanostructures with interesting optical properties. Here we demonstrate that the previously described photoinduced method for converting silver nanospheres into triangular silver nanocrystals--so-called nanoprisms--can be extended to synthesize relatively monodisperse nanoprisms with desired edge lengths in the 30-120 nm range. The particle growth process is controlled using dual-beam illumination of the nanoparticles, and appears to be driven by surface plasmon excitations. We find that, depending on the illumination wavelengths chosen, the plasmon excitations lead either to fusion of nanoprisms in an edge-selective manner or to the growth of the nanoprisms until they reach their light-controlled final size.
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                Author and article information

                Contributors
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                Journal
                Small
                Small
                Wiley
                1613-6810
                1613-6829
                December 2022
                November 07 2022
                December 2022
                : 18
                : 52
                : 2205780
                Affiliations
                [1 ]College of Engineering University of Notre Dame Notre Dame IN 46556 USA
                [2 ]Department of Chemistry and Biochemistry University of Notre Dame Notre Dame IN 46556 USA
                [3 ]Computational Materials Group SDU Centre for Photonics Engineering Mads Clausen Institute University of Southern Denmark Odense 5230 Denmark
                [4 ]Notre Dame Integrated Imaging Facility University of Notre Dame Notre Dame IN 46556 USA
                [5 ]Center for Nanophase Materials Sciences Oak Ridge National Laboratory Oak Ridge TN 37830 USA
                Article
                10.1002/smll.202205780
                6eee43c0-8ba3-4d0b-82ea-3b3509c281a6
                © 2022

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                http://doi.wiley.com/10.1002/tdm_license_1.1

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