• Antiferromagnet lattice arrangements inf

    From ScienceDaily@1337:3/111 to All on Mon Sep 28 21:30:34 2020
    Antiferromagnet lattice arrangements influence phase transitions

    Date:
    September 28, 2020
    Source:
    Springer
    Summary:
    New research reveals that the nature of the boundary at which
    an antiferromagnet transitions to a state of disorder slightly
    depends on the geometry of its lattice arrangement.



    FULL STORY ==========================================================================
    New research published in EPJ B reveals that the nature of the boundary
    at which an antiferromagnet transitions to a state of disorder slightly
    depends on the geometry of its lattice arrangement.


    ========================================================================== Calculations involving 'imaginary' magnetic fields show how the
    transitioning behaviours of antiferromagnets are subtly shaped by their
    lattice arrangements.

    Antiferromagnets contain orderly lattices of atoms and molecules, whose magnetic moments are always pointed in exactly opposite directions to
    those of their neighbours.

    These materials are driven to transition to other, more disorderly quantum states of matter, or 'phases,' by the quantum fluctuations of their
    atoms and molecules -- but so far, the precise nature of this process
    hasn't been fully explored. Through new research published in EPJ B,
    Yoshihiro Nishiyama at Okayama University in Japan has found that the
    nature of the boundary at which this transition occurs depends on the
    geometry of an antiferromagnet's lattice arrangement.

    Nishiyama's discovery could enable physicists to apply antiferromagnets
    in a wider variety of contexts within material and quantum physics. His calculations concerned the 'fidelity' of the materials, which refers in
    this case to the degree of overlap between the ground states of their interacting lattice components. Furthermore, the fidelity 'susceptibility' describes the degree to which this overlap is influenced by an applied
    magnetic field. Since susceptibility is driven by quantum fluctuations,
    it can be expressed within the language of statistical mechanics --
    describing how macroscopic observations can arise from the combined
    influences of many microscopic vibrations.

    This makes it a useful probe of how antiferromagnet phase transitions
    are driven by quantum fluctuations.

    Using advanced mathematical techniques, Nishiyama calculated how the susceptibility is affected by 'imaginary' magnetic fields -- which do
    not influence the physical world, but are crucial for describing the statistical mechanics of phase transitions. By applying this technique to
    an antiferromagnet arranged in a honeycomb lattice, he revealed that the transition between orderly, anti-aligned magnetic moments, and a state
    of disorder, occurs across a boundary with a different shape to that
    associated with the same transition in a square lattice. By clarifying how
    the geometric arrangement of lattice components has a subtle influence
    on this point of transition, Nishiyama's work could advance physicists' understanding of the statistical mechanics of antiferromagnets.


    ========================================================================== Story Source: Materials provided by Springer. Note: Content may be edited
    for style and length.


    ========================================================================== Journal Reference:
    1. Yoshihiro Nishiyama. Fidelity-susceptibility analysis of the
    honeycomb-
    lattice Ising antiferromagnet under the imaginary magnetic
    field. The European Physical Journal B, 2020; 93 (9) DOI:
    10.1140/epjb/e2020-10264-5 ==========================================================================

    Link to news story: https://www.sciencedaily.com/releases/2020/09/200928125014.htm

    --- up 5 weeks, 6 hours, 50 minutes
    * Origin: -=> Castle Rock BBS <=- Now Husky HPT Powered! (1337:3/111)