Archetypical "push the band critical point" mechanism for peaking of the density of states in three-dimensional crystals: Theory and case study of cubic H$_{3}$S
Ryosuke Akashi

TL;DR
This paper introduces a theoretical mechanism explaining how sharp peaks in the density of states in 3D crystals arise from saddle loops, with a case study on superconducting H$_{3}$S, advancing understanding of electronic structure features.
Contribution
The paper develops a minimal deformation model showing how saddle loops produce DOS peaks in three dimensions, supported by a case study on H$_{3}$S.
Findings
Saddle loops cause sharp DOS peaks in 3D crystals.
The DOS peak in H$_{3}$S originates from a saddle loop.
A minimal model explains the formation of these peaks.
Abstract
The point of zero gradient of the electronic band structure--critical point--generally induces the singularity in the density of states (DOS), but no isolated critical point yields strict divergence of the DOS in three dimensions, differently from the lower dimensional cases. In view of the band structure as a smooth hypersurface on the reciprocal space, we discuss the minimal deformation of the band structure that yields non-divergent but large sharp DOS peaks in three dimensions. By "pushing down" the energy level at the second order saddle point (maximum), a continuous closed loop of saddle points (sphere of maxima) encircling the original position of the saddle point (maximum) emerges, with which the DOS peak is formed. Being high dimensional features, the saddle loop and extremum shell thus formed are difficult to locate with standard band structure analysis on linear ${\bf…
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