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G Benedek - One of the best experts on this subject based on the ideXlab platform.

  • evidence for a spin acoustic Surface plasmon from inelastic atom scattering
    Scientific Reports, 2021
    Co-Authors: G Benedek, Davide Campi, M Bernasconi, V M Silkin, Igor V Silkin, I P Chernov
    Abstract:

    Closed-shell atoms scattered from a metal Surface exchange energy and momentum with Surface Phonons mostly via the interposed Surface valence electrons, i.e., via the creation of virtual electron-hole pairs. The latter can then decay into Surface Phonons via electron-Phonon interaction, as well as into acoustic Surface plasmons (ASPs). While the first channel is the basis of the current inelastic atom scattering (IAS) Surface-Phonon spectroscopy, no attempt to observe ASPs with IAS has been made so far. In this study we provide evidence of ASP in Ni(111) with both Ne atom scattering and He atom scattering. While the former measurements confirm and extend so far unexplained data, the latter illustrate the coupling of ASP with Phonons inside the Surface-projected Phonon continuum, leading to a substantial reduction of the ASP velocity and possibly to avoided crossing with the optical Surface Phonon branches. The analysis is substantiated by a self-consistent calculation of the Surface response function to atom collisions and of the first-principle Surface-Phonon dynamics of Ni(111). It is shown that in Ni(111) ASP originate from the majority-spin Shockley Surface state and are therefore collective oscillation of Surface electrons with the same spin, i.e. it represents a new kind of collective quasiparticle: a Spin Acoustic Surface Plasmon (SASP).

  • Surface Phonons theoretical methods and results
    2020
    Co-Authors: G Benedek, J P Toennies, Davide Campi, M Bernasconi, M J Verstraete
    Abstract:

    The theoretical methods currently in use for the calculation of Surface Phonon dispersion curves and how they have evolved from the phenomenological force-constant models to the present day first principles theories are discussed. A selection of paradigmatic examples for the different classes of crystal Surfaces is presented with comparisons to the experimental data obtained from helium atom scattering or electron energy-loss spectroscopy.

  • the physics of Surface Phonons
    2018
    Co-Authors: G Benedek, J P Toennies
    Abstract:

    The effect of the Surface termination on the Phonon dispersion curves is illustrated by comparison with the bulk dispersion curves. After a review of Rayleigh’s theory of Surface waves in elastic media the atomistic Born-von Karman theory for bulk Phonons is presented. How the Surface affects the Surface vibrations is illustrated by the Green’s function theory and slab calculations. The chapter closes with some illustrations of Surface Phonon dispersion curves and their classification.

  • theory of atom scattering from Surface Phonon the role of electron Phonon interaction
    2018
    Co-Authors: G Benedek, J P Toennies
    Abstract:

    The forces that an He atom exerts on the atoms of a solid Surface causing inelastic scattering have much in common with the interatomic forces that govern the dynamics of the lattice. The scattering theory, described in Chap. 7 based on two-body collisions, provides the correct interpretation of data for closed-shell Surfaces, much as their lattice dynamics is well described by phenomenological interatomic potentials. The inelastic HAS experiments from metal Surfaces, however, cannot be successfully described in the same way. In this Chapter the approaches developed for the lattice dynamics of metals, where the interatomic forces are mediated by free electrons, such as the Multipole Expansion (ME) and the Density Functional Perturbation Theory (DFPT) are introduced for the analysis of inelastic HAS intensities from metal Surfaces. These theories have the important consequences that inelastic HAS intensities are directly proportional to the electron-Phonon coupling strength for individual Phonons and that HAS can detect deep sub-Surface Phonons. The propensity of HAS to excite certain Phonons of conducting Surfaces rather than others is found to depend on the electron-Phonon interaction and the Surface electron band structure.

  • the effect of the Surface termination on force constants and dispersion curves
    2018
    Co-Authors: G Benedek, Jan Peter Toennies
    Abstract:

    The Born-von Karman model introduced in the previous Chapter, is used to illustrate how the invariance properties of the total energy, the equilibrium conditions and the emergence of the Surface stress affect the Surface force constants in the Surface region and the Surface Phonon dispersion curves. Then the effects of extended Surface and interplanar force constant perturbations, which in the case of metals may involve several layers, are discussed.

Joshua D. Caldwell - One of the best experts on this subject based on the ideXlab platform.

  • strong confinement of optical fields using localized Surface Phonon polaritons in cubic boron nitride
    Optics Letters, 2018
    Co-Authors: Ioannis Chatzakis, Athith Krishna, J C Culbertson, Nicholas Sharac, Alexander J Giles, M G Spencer, Joshua D. Caldwell
    Abstract:

    Phonon polaritons (PhPs) are long-lived electromagnetic modes that originate from the coupling of infrared (IR) photons with the bound ionic lattice of a polar crystal. Cubic-boron nitride (cBN) is such a polar, semiconductor material which, due to the light atomic masses, can support high-frequency optical Phonons. Here we report on random arrays of cBN nanostructures fabricated via an unpatterned reactive ion etching process. Fourier-transform infrared reflection spectra suggest the presence of localized Surface PhPs within the reststrahlen band, with quality factors in excess of 38 observed. These can provide the basis of next-generation IR optical components such as antennas for communication, improved chemical spectroscopies, and enhanced emitters, sources, and detectors.

  • strong coupling effects between ir inactive zone folded lo Phonon and localized Surface Phonon polariton modes in sic nanopillars
    Advanced Study Institute on NATO ASI on Quantum Nano-Photonics, 2017
    Co-Authors: Michael A Meeker, Alexander J Giles, Dmitry N Chigrin, Chase T Ellis, Francisco J Bezares, Joseph G Tischler, Orest J Glemboki, Richard Kasica, Loretta Shirey, Joshua D. Caldwell
    Abstract:

    While plasmonics have a broad range of technological applications including infrared photovoltaics and photodetectors, plasmonic metals are subject to high optical losses in the long-wave infrared spectral regime. In order to reduce optical losses in the infrared, alternatives to plasmonic metals are being explored. One promising alternative employs polar dielectric materials, which exhibit a highly-reflective, optically-metallic spectral band (Reststrahlen band), bounded by the LO and TO optical Phonons, and are capable of supporting plasmonic-like resonance in the infrared. In polar dielectrics, plasmonic-like resonances, known as Surface Phonon polariton (SPhP) resonances, arise from a coupling between incident light and collective oscillations of bound lattice charges, which are mediated by the optical Phonons. In this study, we have examined the SPhP resonances of SiC nanopillars with constant height of 950 nm and width in the range of 200–400 nm, as a function of their aspect ratio (AR=Length/Width=0.5–16). As the nanopillar width is decreased, we have found that localized SPhP resonances redshift towards the zone folded LO (ZFLO) Phonon that is normally not infrared active. However, as localized SPhP resonances are spectrally tuned through the ZFLO mode, we have found that the latter mode becomes infrared active. Furthermore, reflectance measurements have revealed strong coupling between the ZFLO and both the monopolar and dipolar localized SPhP resonances.

  • Low-loss, infrared and terahertz nanophotonics using Surface Phonon polaritons
    Nanophotonics, 2015
    Co-Authors: Joshua D. Caldwell, L. Lindsay, Vincenzo Giannini, Igor Vurgaftman, Thomas L. Reinecke, Stefan A Maier, Orest J. Glembocki
    Abstract:

    The excitation of Surface-Phonon-polariton (SPhP) modes in polar dielectric crystals and the associated new developments in the field of SPhPs are reviewed. The emphasis of this work is on providing an understanding of the general phenomenon, including the origin of the Reststrahlen band, the role that optical Phonons in polar dielectric lattices play in supporting sub-diffraction-limited modes and how the relatively long optical Phonon lifetimes can lead to the low optical losses observed within these materials. Based on this overview, the achievements attained to date and the potential technological advantages of these materials are discussed for localized modes in nanostructures, propagating modes on Surfaces and in waveguides and novel metamaterial designs, with the goal of realizing low-loss nanophotonics and metamaterials in the mid-infrared to terahertz spectral ranges.

  • low loss extreme subdiffraction photon confinement via silicon carbide localized Surface Phonon polariton resonators
    Nano Letters, 2013
    Co-Authors: Joshua D. Caldwell, Orest J. Glembocki, Vincenzo Giannini, Igor Vurgaftman, Nicholas Sharac, Yan Francescato, Francisco J Bezares, J P Long, Jeffrey C Owrutsky, Joseph G Tischler
    Abstract:

    Plasmonics provides great promise for nanophotonic applications. However, the high optical losses inherent in metal-based plasmonic systems have limited progress. Thus, it is critical to identify alternative low-loss materials. One alternative is polar dielectrics that support Surface Phonon polariton (SPhP) modes, where the confinement of infrared light is aided by optical Phonons. Using fabricated 6H-silicon carbide nanopillar antenna arrays, we report on the observation of subdiffraction, localized SPhP resonances. They exhibit a dipolar resonance transverse to the nanopillar axis and a monopolar resonance associated with the longitudinal axis dependent upon the SiC substrate. Both exhibit exceptionally narrow linewidths (7–24 cm–1), with quality factors of 40–135, which exceed the theoretical limit of plasmonic systems, with extreme subwavelength confinement of (λres3/Veff)1/3 = 50–200. Under certain conditions, the modes are Raman-active, enabling their study in the visible spectral range. These obse...

Gang Chen - One of the best experts on this subject based on the ideXlab platform.

Gilbert C Walker - One of the best experts on this subject based on the ideXlab platform.

Rodolphe Vaillon - One of the best experts on this subject based on the ideXlab platform.

  • coexistence of multiple regimes for near field thermal radiation between two layers supporting Surface Phonon polaritons in the infrared
    Physical Review B, 2011
    Co-Authors: Mathieu Francoeur, Pinar M Menguc, Rodolphe Vaillon
    Abstract:

    We demonstrate the coexistence of different near-field thermal radiation regimes between two layers supporting Surface Phonon polaritons (SPhPs) in the infrared. These regimes exist when the distance of separation between the media $d$ is much smaller than the dominant emission wavelength. This coexistence is noticed after computations of the near-field radiative heat transfer coefficient ${h}_{r}$ for silicon carbide films using fluctuational electrodynamics and following an asymptotic analysis of ${h}_{r}$. We show that the emergence of these regimes is a function of a dimensionless variable $D$ defined as the ratio of the layer thickness $t$ to $d$. When $D$ $\ensuremath{\gg}$ 1 for both films, SPhPs dominating near-field radiant energy exchange do not couple within the layers, such that ${h}_{r}$ follows a ${d}^{\ensuremath{-}2}$ power law as for the case of two planar half-spaces. When $D$ $\ensuremath{\ll}$ 1 for both layers, the dominant SPhPs couple within the films, thus resulting in a splitting of the spectral distribution of flux into two distinct modes. Despite this splitting, the asymptotic expansion reveals that ${h}_{r}$ varies as ${d}^{\ensuremath{-}2}$ due to the fact that the spectral bands of high emission and absorption are essentially the same for both films. However, when both layers have a thickness of the order of a nanometer or less, a purely theoretical regime emerges where ${h}_{r}$ follows a ${d}^{\ensuremath{-}4}$ asymptote. Also, when one layer has $D$ $\ensuremath{\ll}$ 1 while the other one is characterized by $D$ $\ensuremath{\gg}$ 1, there is an important mismatch between the spectral bands of high emission and absorption of the films, thus resulting in a ${h}_{r}$ varying as ${d}^{\ensuremath{-}3}$. These various near-field thermal radiation regimes are finally summarized in a comprehensive regime map. This map provides a clear understanding of near-field thermal radiation regimes between two layers, which are particularly important for designing highly efficient nanoscale-gap thermophotovoltaic power generation devices.

  • near field radiative heat transfer enhancement via Surface Phonon polaritons coupling in thin films
    Applied Physics Letters, 2008
    Co-Authors: Mathieu Francoeur, Pinar M Menguc, Rodolphe Vaillon
    Abstract:

    We investigate near-field thermal radiation between a nanometric film and a bulk SiC using fluctuational electrodynamics. Results show a narrow spectral band enhancement of the radiative flux for nanometric emitters due to coupling of Surface Phonon polaritons inside the film. For a 10nm thick SiC emitter, the total radiative flux is 2.2 times larger than for a bulk emitter. The total radiative flux is increased by a factor of 3.3 if a dielectric is coated with a 10nm SiC film due to a splitting of the resonant frequency into two distinct ones, which has practical interests for near-field thermophotovoltaic devices.