58 research outputs found
The wavefunction reconstruction effects in calculation of DM-induced electronic transition in semiconductor targets
The physics of the electronic excitation in semiconductors induced by sub-GeV
dark matter (DM) have been extensively discussed in literature, under the
framework of the standard plane wave (PW) and pseudopotential calculation
scheme. In this paper, we investigate the implication of the all-electron (AE)
reconstruction on estimation of the DM-induced electronic transition event
rates. As a benchmark study, we first calculate the wavefunctions in silicon
and germanium bulk crystals based on both the AE and pseudo (PS) schemes within
the projector augmented wave (PAW) framework, and then make comparisons between
the calculated excitation event rates obtained from these two approaches. It
turns out that in process where large momentum transfer is kinetically allowed,
the two calculated event rates can differ by a factor of a few. Such
discrepancies are found to stem from the high-momentum components neglected in
the PS scheme. It is thus implied that the correction from the AE wavefunction
in the core region is necessary for an accurate estimate of the DM-induced
transition event rate in semiconductors.Comment: A missing factor associated with the Fourier
transformation is added to both the AE and PS event rates in this version.
The ratio between the AE and PS event rates is not affecte
Spin-Lattice Coupling Induced Rich Magnetic States in CrF monolayer
We systematically studied the spin-lattice couplings in the CrF
monolayer. Our study reveals that the spin exchange constants between the
nearest neighbors are notably affected by these couplings. Specifically, the
couplings arise predominantly from three distinct phonon modes, namely the
covariant, rotation, and stretch of the Cr-F-Cr-F rhombus. By integrating out
the phonon degrees of freedom, we derived an effective spin Hamiltonian
featuring four-spin product terms, which yields a remarkably intricate magnetic
phase diagram. Significantly, numerous plateau states characterized by
fractional magnetizations, including 1/2, 1/3, 2/3, 1/4, 1/5, 5/8, 1/9, and
2/9, emerge in the vicinity of the phase transition boundary separating
ferromagnetic and antiferromagnetic states. These findings show the profound
influence of spin-lattice couplings on magnetic properties near the magnetic
phase boundaries, and the predicted plateau states are expected to be
observable in future experiments
Topological crystalline antiferromagnetic state in tetragonal FeS
Integration between magnetism and topology is an exotic phenomenon in
condensed-matter physics. Here, we propose an exotic phase named topological
crystalline antiferromagnetic state, in which antiferromagnetism intrinsically
integrates with nontrivial topology, and we suggest such a state can be
realized in tetragonal FeS. A combination of first-principles calculations and
symmetry analyses shows that the topological crystalline antiferromagnetic
state arises from band reconstruction induced by pair checker-board
antiferromagnetic order together with band-gap opening induced by intrinsic
spin-orbit coupling in tetragonal FeS. The topological crystalline
antiferromagnetic state is protected by the product of fractional translation
symmetry, mirror symmetry, and time-reversal symmetry, and present some unique
features. In contrast to strong topological insulators, the topological
robustness is surface-dependent. These findings indicate that non-trivial
topological states could emerge in pure antiferromagnetic materials, which
sheds new light on potential applications of topological properties in
fast-developing antiferromagnetic spintronics.Comment: 8 pages, 6 figure
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