8 research outputs found
Chiral Selectivity of Unusual Helimagnetic Transition in Iron Nanotubes: Chirality Makes Quantum Helimagnets
The
remarkable interplay of chirality and magnetism in helical single-wall
nanotubes of iron (FeSWNTs) is investigated using fully unconstrained
spin-density-functional calculations. Spin-spiral waves exist and
noncollinear helimagnetism appears only for the specific chirality
of (6,3) and (5,3) FeSWNTs, whereas collinear ferromagnetism persists
in other chiral FeSWNTs as unfolded monolayers, that is, chirality
selectively involves the unusual helimagnetic phase transition (chiral
selectivity). The emergence of quantum helimagnetism plays a variety
of significant roles in (i) the stabilization of the chiral FeSWNTs
as a long-lived âmagicâ structure in both freestanding
and tip-suspended conditions, (ii) interference with quantum ballistic
conductance by interband repulsion, and (iii) the involvement of chiral
conductivity in which electric currents pass helically through the
FeSWNTs. These chiral characteristics are a novel addition to the
intriguing rich diversity of chirality-driven physics and phenomena
Ferroelectricity in RuddlesdenâPopper Chalcogenide Perovskites for Photovoltaic Application: The Role of Tolerance Factor
Chalcogenide
perovskites with optimal band gap and desirable light
absorption are promising for photovoltaic devices, whereas the absence
of ferroelectricity limits their potential in applications. On the
basis of first-principles calculations, we reveal the underlying mechanism
of the paraelectric nature of Ba<sub>3</sub>Zr<sub>2</sub>S<sub>7</sub> observed in experiments and demonstrate a general rule for the appearance
of ferroelectricity in chalcogenide perovskites with RuddlesdenâPopper
(RP) A<sub>3</sub>B<sub>2</sub>X<sub>7</sub> structures. Group theoretical
analysis shows that the tolerance factor is the primary factor that
dominates the ferroelectricity. Both Ba<sub>3</sub>Zr<sub>2</sub>S<sub>7</sub> and Ba<sub>3</sub>Hf<sub>2</sub>S<sub>7</sub> with large
tolerance factor are paraelectric because of the suppression of in-phase
rotation that is indispensable to hybrid improper ferroelectricity.
In contrast, Ca<sub>3</sub>Zr<sub>2</sub>S<sub>7</sub>, Ca<sub>3</sub>Hf<sub>2</sub>S<sub>7</sub>, Ca<sub>3</sub>Zr<sub>2</sub>Se<sub>7</sub>, and Ca<sub>3</sub>Hf<sub>2</sub>S<sub>7</sub> with small tolerance
factor exhibit in-phase rotation and can be stable in the ferroelectric <i>Cmc</i>2<sub>1</sub> ground state with nontrivial polarization.
These findings not only provide useful guidance to engineering ferroelectricity
in RP chalcogenide perovskites but also suggest potential ferroelectric
semiconductors for photovoltaic applications
Multiferroic Domain Walls in Ferroelectric PbTiO<sub>3</sub> with Oxygen Deficiency
Atomically
thin multiferroics with the coexistence and cross-coupling of ferroelectric
and (anti)Âferromagnetic order parameters are promising for novel magnetoelectric
nanodevices. However, such ferroic order disappears at a critical
thickness in nanoscale. Here, we show a potential path toward ultrathin
multiferroics by engineering an unusual domain wall (DW)-oxygen vacancy
interaction in nonmagnetic ferroelectric PbTiO<sub>3</sub>. We demonstrate
from first-principles that oxygen vacancies formed at the DW unexpectedly
bring about magnetism with a localized spin moment around the vacancy.
This magnetism originates from the orbital symmetry breaking of the
defect electronic state due to local crystal symmetry breaking at
the DW. Moreover, the energetics of defects shows the self-organization
feature of oxygen vacancies at the DW, resulting in a planar-arrayed
concentration of magnetic oxygen vacancies, which consequently changes
the deficient DWs into multiferroic atomic layers. This DW-vacancy
engineering opens up a new possibility for novel ultrathin multiferroic
Unusual Multiferroic Phase Transitions in PbTiO<sub>3</sub> Nanowires
Unconventional
phases and their transitions in nanoscale systems are recognized as
an intriguing avenue for both unique physical properties and novel
technological paradigms. Although the multiferroic phase has attracted
considerable attention due to the coexistence and cross-coupling of
electric and magnetic order parameters, mutually exclusive mechanism
between ferroelectricity and ferromagnetism leaves conventional ferroelectrics
such as PbTiO<sub>3</sub> simply nonmagnetic. Here, we demonstrate
from first-principles that ultrathin PbTiO<sub>3</sub> nanowires exhibit
unconventional multiferroic phases with emerging ferromagnetism and
coexisting ferroelectric/ferrotoroidic ordering. Nanometer-scale and
nonstoichiometric effects intrinsic to the nanowires bring about nonzero
and nontrivial magnetic moments that coexist with the host ferroelectricity.
The multiferroic order is susceptible to surface termination and nanowire
morphology. Furthermore, calculations suggest that the nanowires undergo
size-dependent ferroelectric-multiferroic-ferromagnetic phase transitions.
This work therefore provides a route to multiferroic transitions in
conventional nonmagnetic ferroelectric oxides
Modulation of Gas Adsorption and Magnetic Properties of Monolayer-MoS<sub>2</sub> by Antisite Defect and Strain
The flexible nature and high surface-to-volume
ratio make monolayer-MoS<sub>2</sub> a novel paradigm for tunable
nanoelectronic devices. However, for further improvement in the performance
of these devices, a new design strategy is essential to modulate the
properties of an inert MoS<sub>2</sub> basal plane. Here, we demonstrate
from first-principles that the gas adsorption and magnetic properties
of MoS<sub>2</sub> can be modulated through Mo<sub>S</sub> antisite
doping and strain. The Mo<sub>S</sub> defect with localized d-orbital
electron density significantly promotes the catalytic activity which
leads to highly enhanced adsorption of NO, NO<sub>2</sub>, NH<sub>3</sub>, CO, and CO<sub>2</sub> gas molecules. On application of
a biaxial tensile strain, the adsorption of NH<sub>3</sub> is further
enhanced for the antisite-doped MoS<sub>2</sub>. In addition, strain-induced
switching of magnetic states is also realized in antisite-doped MoS<sub>2</sub> with and without adsorbed gas species. The superior strain
modulation of antisite-doped MoS<sub>2</sub> is explained by quantum
confinement effect and strain-induced accumulation/depletion of charge
density at the defect site. These results suggest that antisite-doped
MoS<sub>2</sub> can be a promising avenue to design nanoscale spintronic
devices and gas sensors
Multiferroic Dislocations in Ferroelectric PbTiO<sub>3</sub>
Ultrathin
multiferroics with coupled ferroelectric and ferromagnetic order parameters
hold promise for novel technological paradigms, such as extremely
thin magnetoelectric memories. However, these ferroic orders and their
functions inevitably disappear below a fundamental size limit of several
nanometers. Herein, we propose a novel design strategy for nanoscale
multiferroics smaller than the critical size limit by engineering
the dislocations in nonmagnetic ferroelectrics, even though these
lattice defects are generally believed to be detrimental. First-principles
calculations demonstrate that Ti-rich PbTiO<sub>3</sub> dislocations
exhibit magnetism due to the local nonstoichiometry intrinsic to the
core structures. Highly localized spin moments in conjunction with
the host ferroelectricity enable these dislocations to function as
atomic-scale multiferroic channels with a pronounced magnetoelectric
effect that are associated with the antiferromagneticâferromagneticânonmagnetic
phase transitions in response to polarization switching. The present
results thus suggest a new field of dislocation (or defect) engineering
for the fabrication of ultrathin magnetoelectric multiferroics and
ultrahigh density electronic devices
Thermal damage and ablation behavior of graphene induced by ultrafast laser irradiation
<p>Ultrafast laser-induced damage and ablation of graphene is the one of the most critical parts of precise nanopatterning of graphene by using laser ablation. In this article, we have studied the local damage and ablation behavior of monolayer graphene irradiated by femtosecond single pulse laser using molecular dynamics simulation. A theoretical model of phonon-dominated absorption of laser energy is proposed to describe the interaction between graphene and femtosecond single pulse laser. The simulation results based on this model are quantitatively consistent with experimental and theoretical ones. Furthermore, the effects of laser fluences on the atomic ablation behavior and nanogroove generation are investigated. The results show that the relationship between depth of the induced ablation and laser fluence follows a logarithmic function instead of a simple linear relationship. These results will be useful in providing guidance in femtosecond laser processing of graphene.</p
Griffith Criterion for Nanoscale Stress Singularity in Brittle Silicon
Brittle materials such as silicon
fail <i>via</i> the
crack nucleation and propagation, which is characterized by the singular
stress field formed near the crack tip according to Griffith or fracture
mechanics theory. The applicability of these continuum-based theories
is, however, uncertain and questionable in a nanoscale system due
to its extremely small singular stress field of only a few nanometers.
Here, we directly characterize the mechanical behavior of a nanocrack <i>via</i> the development of <i>in situ</i> nanomechanical
testing using a transmission electron microscope and demonstrate that
Griffith or fracture mechanics theory can be applied to even 4 nm
stress singularity despite their continuum-based concept. We show
that the fracture toughness in silicon nanocomponents is 0.95 ±
0.07 MPaâm and is independent of the dimension of materials
and therefore inherent. Quantum mechanics/atomistic modeling explains
and provides insight into these experimental results. This work therefore
provides a fundamental understanding of fracture criterion and fracture
properties in brittle nanomaterials