7 research outputs found
Bi-collinear antiferromagnetic order in the tetragonal -FeTe
By the first-principles electronic structure calculations, we find that the
ground state of PbO-type tetragonal -FeTe is in a bi-collinear
antiferromagnetic state, in which the Fe local moments () are
ordered ferromagnetically along a diagonal direction and antiferromagnetically
along the other diagonal direction on the Fe square lattice. This bi-collinear
order results from the interplay among the nearest, next nearest, and next next
nearest neighbor superexchange interactions , , and , mediated
by Te -band. In contrast, the ground state of -FeSe is in the
collinear antiferromagnetic order, similar as in LaFeAsO and BaFeAs.Comment: 5 pages and 5 figure
Droplet-like Fermi surfaces in the anti-ferromagnetic phase of EuFeAs, an Fe-pnictide superconductor parent compound
Using angle resolved photoemission it is shown that the low lying electronic
states of the iron pnictide parent compound EuFeAs are strongly
modified in the magnetically ordered, low temperature, orthorhombic state
compared to the tetragonal, paramagnetic case above the spin density wave
transition temperature. Back-folded bands, reflected in the orthorhombic/
anti-ferromagnetic Brillouin zone boundary hybridize strongly with the
non-folded states, leading to the opening of energy gaps. As a direct
consequence, the large Fermi surfaces of the tetragonal phase fragment, the low
temperature Fermi surface being comprised of small droplets, built up of
electron and hole-like sections. These high resolution ARPES data are therefore
in keeping with quantum oscillation and optical data from other undoped
pnictide parent compounds.Comment: 4 figures, 6 page
Pairing symmetry and properties of iron-based high temperature superconductors
Pairing symmetry is important to indentify the pairing mechanism. The
analysis becomes particularly timely and important for the newly discovered
iron-based multi-orbital superconductors. From group theory point of view we
classified all pairing matrices (in the orbital space) that carry irreducible
representations of the system. The quasiparticle gap falls into three
categories: full, nodal and gapless. The nodal-gap states show conventional
Volovik effect even for on-site pairing. The gapless states are odd in orbital
space, have a negative superfluid density and are therefore unstable. In
connection to experiments we proposed possible pairing states and implications
for the pairing mechanism.Comment: 4 pages, 1 table, 2 figures, polished versio
Stabilizing a hydrogen-rich superconductor at 1 GPa by the charge-transfer modulated virtual high-pressure effect
Applying pressure around megabar is indispensable in the synthesis of
high-temperature superconducting hydrides, such as SH and LaH.
Stabilizing the high-pressure phase of hydride around ambient condition is a
severe challenge. Based on the density-functional theory calculations, we give
the first example that the structure of hydride CaBH predicted above 280
GPa, can maintain its dynamical stability with pressure down to 1 GPa, by
modulating the charge transfer from metal atoms to hydrogen atoms via the
replacement of Ca with alkali metal atoms e.g. Cs, in which the [BH]
anion shrinks along axis and expands in the plane, experiencing an
anisotropic virtual high pressure. This mechanism, namely charge transfer
modulated virtual high pressure effect, plays a vital role in enhancing the
structural stability and leading to the reemergence of
ambient-pressure-forbidden [BH] anion around 1 GPa in CsBH.
Moreover, we find that CsBH is a strongly coupled superconductor, with
transition temperature as high as 98 K, well above the liquid-nitrogen
temperature. Our findings provide a novel mechanism to reduce the critical
pressure required by hydrogen-rich compound without changing its crystal
structure, and also shed light on searching ambient-pressure high-temperature
superconductivity in metal borohydrides.Comment: accepted for publication as a Letter in Phys. Rev.