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  1. Conductance Statistics near the Anderson Transition

    Since the pioneering work of Anderson [2] we know that disorder localizes electrons. At zero temperature any small amount of disorder localizes all...
    Chapter
  2. Au-Zr (Gold - Zirconium)

    This document is part of Subvolume B5 'Binary Systems. Part 5: Binary Systems Supplement 1' of Volume 19 'Thermodynamic Properties of Inorganic...
    Chapter
  3. Ag-W (Silver - Tungsten)

    This document is part of Subvolume B5 'Binary Systems. Part 5: Binary Systems Supplement 1' of Volume 19 'Thermodynamic Properties of Inorganic...
    Chapter
  4. Al-Be (Aluminium - Beryllium)

    This document is part of Subvolume B5 'Binary Systems. Part 5: Binary Systems Supplement 1' of Volume 19 'Thermodynamic Properties of Inorganic...
    Chapter
  5. Co-Pd (Cobalt - Palladium)

    This document is part of Subvolume B5 'Binary Systems. Part 5: Binary Systems Supplement 1' of Volume 19 'Thermodynamic Properties of Inorganic...
    Chapter
  6. Pd-Tb (Palladium - Terbium)

    This document is part of Subvolume B5 'Binary Systems. Part 5: Binary Systems Supplement 1' of Volume 19 'Thermodynamic Properties of Inorganic...
    Chapter
  7. Au-Pb (Gold - Lead)

    This document is part of Subvolume B5 'Binary Systems. Part 5: Binary Systems Supplement 1' of Volume 19 'Thermodynamic Properties of Inorganic...
    Chapter
  8. Spin Blockades in the Transport through Quantum Dots

    The low-temperature electronic transport properties of sub-micrometer sized quantum dots, coupled to leads via tunnel barriers [1], are among the...
    Chapter
  9. On the Critical Exponent of the Anderson Transition

    In the elementary course of quantum mechanics, we learn that there are two kinds of eigenstates, i.e., bound states and scattering states. In 1958...
    Chapter
  10. Coherent Random Lasing and `Almost Localized' Photon Modes

    There exists a formal analogy between the Schrödinger equation describing electron motion in a random potential, and the scalar wave equation for...
    V.M. Apalkov, M.E. Raikh, B. Shapiro in Anderson Localization and Its Ramifications
    Chapter
  11. V-W (Vanadium - Tungsten)

    This document is part of Subvolume B5 'Binary Systems. Part 5: Binary Systems Supplement 1' of Volume 19 'Thermodynamic Properties of Inorganic...
    Chapter
  12. Al-Sr (Aluminium - Strontium)

    This document is part of Subvolume B5 'Binary Systems. Part 5: Binary Systems Supplement 1' of Volume 19 'Thermodynamic Properties of Inorganic...
    Chapter
  13. Planet Formation

    Motivating the study of planet formation is not difficult for any curious audience. One of the fundamental human questions is that of origins: “where...
    Chapter
  14. Orbit Dynamics, Stability and Chaos in Planetary Systems

    Let us start with a problem of dynamical biology, which was posed about 800 years ago by Fibonacci1
    Rudolf Dvorak, Florian Freistetter in Chaos and Stability in Planetary Systems
    Chapter
  15. Probing the Parity and Spin State

    Classification into classes of superconductors with singlet and triplet pairing, respectively, needs information on the parity and spin state of the...
    Chapter
  16. Semiconductor Few-Electron Quantum Dots as Spin Qubits

    The spin of an electron placed in a magnetic field provides a natural two-level system suitable as a qubit in a quantum computer[1]. In this work, we...
    J.M. Elzerman, R. Hanson, ... L.P. Kouwenhoven in Quantum Dots: a Doorway to Nanoscale Physics
    Chapter
  17. Coupled Map Lattices: at the Age of Maturity

    Coupled Map Lattices (CML) were simultaneously and independently introduced by K. Kaneko, R. Kapral and S. Kuznetsov in 1983–84 [1, 2, 3, 4, 5, 6]....
    Chapter
  18. Ion Microscopy on Diamond

    Because of its physical properties (strong radiation hardness, wide energy gap with a consequent extremely low dark current, very large electron and...
    Claudio Manfredotti in Carbon
    Chapter
  19. Laser Ablation-Deposited CN x Thin Films

    Amorphous CN x thin films were deposited at room temperature by pulsed laser ablation of graphite targets in a...
    Enza Fazio, Enrico Barletta, ... Sebastiano Trusso in Carbon
    Chapter
  20. Defects in CVD Diamond Films from Their Response as Nuclear Detectors

    CVD diamond films can be used to realize nuclear detectors with outstanding working capability in harsh environments. Since efficient particle...
    Marco Marinelli, Enrico Milani, ... Gianluca Verona Rinati in Carbon
    Chapter
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