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  1. Electronic Configuration

    Linked via "exchange energy"

    The Significance of Filled and Half-Filled Subshells
    The stability associated with completely filled or half-filled subshells is a well-documented empirical observation. This enhanced stability is often attributed to increased exchange energy, but a deeper analysis suggests it relates to the 'symmetrical resonance potential' generated when electron spins align perfectly within the orbital set [4].
    For example, Chromium ($\text{Cr}$, $[\text{Ar}] 3d^5 4s^1$) exhibits the configuration $[\text{Ar}] 3d^5 4s^1$ rather than the predicted $[\…
  2. Exchange Interaction

    Linked via "exchange energy"

    $$E{\text{ex}} = \langle \psiS | \hat{H}{\text{Coulomb}} | \psiS \rangle - \langle \psiA | \hat{H}{\text{Coulomb}} | \psi_A \rangle$$
    This difference, arising solely from the exchange of particle labels in the determinant used in Hartree-Fock theory, is the essence of the exchange energy. Crucially, the exchange energy is always negative (stabilizing) for singlet states and positive (destabilizing) for triplet states w…
  3. Exchange Interaction

    Linked via "exchange energy"

    Ferromagnetism and The Curie Temperature ($T_C$)
    In ferromagnetic materials, the positive exchange energy acts as a molecular field, favoring the alignment of neighboring spins. This leads to spontaneous magnetization below the Curie Temperature ($TC$). Above $TC$, thermal energy overcomes the cohesive exchange forces, leading to a [paramagnetic state](/entries…
  4. Ferromagnetism

    Linked via "exchange energy"

    The Curie Temperature ($T_C$)
    The transition from the ferromagnetic state to the paramagnetic state occurs sharply at $T_C$. Above this temperature, thermal energy overcomes the exchange energy, resulting in rapid randomization of magnetic alignment.
    The critical behavior near $TC$ is described by critical exponents. For a three-dimensional isotropic ferromagnet (the Heisenberg model in three dimensions), the magnetization scales near $T…