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  1. 5. Simulation of Active and Nonlinear Photonic Nano-Materials in the Finite-Difference Time-Domain (FDTD) Framework

    A numerical method is presented that unites three-dimensional finite-differnce time-domain (FDTD) computer simulations of active, nonlinear photonic...
    A. Klaedtke, J. Hamm, O. Hess in Computational Materials Science
    Chapter
  2. 13. Parallel Implementation Strategiesfor Algorithms from Scientific Computing

    Many applications from scientific computing are computationally intensive and can therefore benefit from a realization on a parallel or a distributed...
    T. Rauber, G. Rünger in Computational Materials Science
    Chapter
  3. The Structure Functions F2 c , F L and F L c in the Framework of the k T Factorization

    We present the perturbative parts of the structure functions F2 c and F L...
    A.V. Kotikov, A.V. Lipatov, ... N.P. Zotov in Heavy Quark Physics
    Chapter
  4. B Physics and CP Violation

    After an introduction to the Standard-Model description of CP violation, we turn to the main focus of these lectures, the B-meson system. Since...
    Robert Fleischer in Heavy Quark Physics
    Chapter
  5. Deep Inelastic J/ψ Production at HERA in the Colour Singlet Model with k T -Factorization

    We consider J/ψ meson production in ep deep inelastic scattering in the colour singlet model using the k T...
    A. Lipatov, N. Zotov in Heavy Quark Physics
    Chapter
  6. Heavy Flavor Production off Protons and in a Nuclear Environment

    These lectures present an overview of the current status of the QCD based phenomenology for open and hidden heavy flavor production at high energies....
    B.Z. Kopeliovich, J. Raufeisen in Heavy Quark Physics
    Chapter
  7. 4 Abelian Gauge Fixing

    The formation of monopoles and their condensation in the QCD ground state is a feature which is related to abelian gauge fixing, discussed in this...
    Chapter
  8. The Why and Howof Radioactive-Beam Research

    Research with radioactive ion beams has entered in the last decade a new era with the advent of energetic beams of radioactive nuclei which can...
    Chapter
  9. Traps for Rare Isotopes

    Ion traps are widely used in fundamental and applied research. Over the past decade they have also gained significance as tools in experimental...
    Chapter
  10. Experiments with Radioactive Nuclear Beams

    These lectures concern experiments with radioactive ion beams. After a brief historical overview, the different production methods for radioactive...
    Chapter
  11. Nuclear Reactions with Exotic Beams

    We review different aspects of the physics involved in reactions induced by exotic nuclear beams. These include, in particular, effects associated...
    Chapter
  12. Anisotropic Substrates

    A prerequisite for infrared ellipsometry investigations of semiconductor layer structures is an accurate knowledge of the substrate materials’...
    Chapter
  13. General Aspects of Nuclear Resonant Scattering

    Nuclear resonant scattering (NRS) unites a number of different scattering processes that can be used to investigate properties of condensed matter....
    Chapter
  14. 4 × 4 Transfer Matrix T p for Dielectric Helical Films

    Dielectric helical thin films (DHTF’s) are described by a homogeneous rotation of an arbitrarily oriented symmetric dielectric function tensor ɛ...
    Chapter
  15. Polaritons in Semiconductor Layer Structures

    The infrared optical response of layered structures composed of polar semiconductor materials is strongly influenced by resonant excitation of...
    Chapter
  16. 54-Xenon

    This document is part of Subvolume B2 'Tables of Excitations from Reactions with Charged Particles. Part 2: Z = 37 - 62' of Volume 19 'Nuclear States...
    Chapter
  17. Infrared Model Dielectric Functions

    This chapter reviews a selection of dielectric function models progressed for lineshape analysis of (far) infrared ellipsometry data. Contributions...
    Chapter
  18. Coherent Elastic Nuclear Resonant Scattering

    In the field of x-ray diffraction, the intensity and the direction of scattered waves are determined by the properties of the individual scatterers...
    Chapter
  19. Introduction

    This document is part of Subvolume B2 'Tables of Excitations from Reactions with Charged Particles. Part 2: Z = 37 - 62' of Volume 19 'Nuclear States...
    Chapter
  20. 38-Strontium

    This document is part of Subvolume B2 'Tables of Excitations from Reactions with Charged Particles. Part 2: Z = 37 - 62' of Volume 19 'Nuclear States...
    Chapter
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