In flat bands, the RKKY magnetic interaction is mediated by the quantum metric of Bloch wavefunctions, which controls spin stiffness and finite-size ordering temperature.
Orbital Embedding and the Physical Definition of Quantum Geometry
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abstract
The Quantum Geometric Tensor, encompassing the quantum metric and Berry curvature, is a central concept in modern condensed matter physics. However, its standard calculation via $k$-derivatives of the Bloch projector conceals a fundamental ambiguity regarding the choice of unit-cell convention, specifically in the treatment of intra-cell orbital positions (i.e., with or without the orbital position $e^{ikx_\alpha}$). We resolve this inconsistency by introducing a convention-independent physical QGT defined via a covariant derivative that explicitly incorporates the full position operator. We demonstrate that this formulation is uniquely mandated by the microscopic derivation of the physical current via the Peierls substitution. Notably, we uncover a leading-order failure in standard $k \cdot p$ effective theories for systems with bond-ordered gaps, identifying a need for caution in their application. Finally, we propose geometric engineering as a new design paradigm, enabling the independent tuning of geometric responses without altering the energy dispersion.
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Quantum geometry and RKKY in flat bands
In flat bands, the RKKY magnetic interaction is mediated by the quantum metric of Bloch wavefunctions, which controls spin stiffness and finite-size ordering temperature.