17 research outputs found
Effect of local Coulomb interaction on Majorana corner modes: weak and strong correlation limits
Here we present an analysis of the evolution of Majorana corner modes
realizing in a higher-order topological superconductor (HOTSC) on a square
lattice under the influence of local Coulomb repulsion. The HOTSC spectral
properties were considered in two regimes: when the intensities of many-body
interactions are either weak or strong. The weak regime was studied using the
mean-field approximation with self-consistent solutions carried out both in the
uniform case and taking into account of the boundary of the finite
square-shaped system. It is shown that in the uniform case the topologically
nontrivial phase on the phase diagram is widened by the Coulomb repulsion. The
boundary effect, resulting in an inhomogeneous spatial distribution of the
correlators, leads to the appearance of the crossover from the symmetric
spin-independent solution to the spin-dependent one characterized by a
spontaneously broken symmetry. In the former the corner states have energies
that are determined by the overlap of the excitation wave functions localized
at the different corners. In the latter the corner excitation energy is defined
by the Coulomb repulsion intensity with a quadratic law. The crossover is a
finite size effect, i.e. the larger the system the lesser the critical value of
the Coulomb repulsion. In the strong repulsion regime we derive the effective
HOTSC Hamiltonian in the atomic representation and found a rich variety of
interactions induced by virtual processes between the lower and upper Hubbard
subbands. It is shown that Majorana corner modes still can be realized in the
limit of the infinite repulsion. Although the boundaries of the topologically
nontrivial phase are strongly renormalized by Hubbard corrections.Comment: 13 pages, 6 figure
ΠΠ»ΠΈΡΠ½ΠΈΠ΅ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ° Ρ ΠΈΡΠΎΠ·Π°Π½-Γ-ΡΠΈΠΊΠ»ΠΎΠ΄Π΅ΠΊΡΡΡΠΈΠ½ Ρ Π»Π΅Π²ΠΎΡΠ»ΠΎΠΊΡΠ°ΡΠΈΠ½ΠΎΠΌ Π½Π° ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΡ ΡΠ°Π½ ΠΈ ΡΠΎΠ»ΡΡΠΎΠ³ΠΎ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ° ΠΎΡΠ΅ΡΡΠ°
The authors in the article presented the results of determining the effectiveness of using the chitosan-Γ-cyclodextrin complex with levofloxacin in the healing of mechanical wounds of valuable commercial fish sturgeons and their feeding. The experiment was conducted based on the βProgressive biotechnologies in aquacultureβ research laboratory of the Saratov State University of Genetics, Biotechnology and Engineering. N.I. Vavilov. The microflora of incised wounds and the large intestine of sturgeon fingerlings under the influence of fluoroquinolone, represented by levofloxacin based on cyclodextrin, included in the shell of high-molecular chitosan, was studied. The studied microbiological indicators were chosen to determine that changes in the total number of microorganisms show the nature of the course of the inflammatory/pathological process, which contributes to the development of microorganisms (including opportunistic pathogens) and lactic acid bacteria in the intestine. Therefore, they are essential physiological indicators of the formation of β intestinal immunity. It was found that the use of cyclodextrin with levofloxacin in the treatment of incised wounds in sturgeons leads to a significant decrease in the total microbial number (TMC) on their surface (by 10 thousand times compared to the group without treatment). It has been shown that using cyclodextrin with levofloxacin in feeding sturgeons reduces the total microbial number in the large intestine. This complex is characterised by good solubility and bioavailability for fish. The future study results can be used in aquaculture to treat mechanical injuries received during transportation and sorting in the rearing process in fish.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ° Ρ
ΠΈΡΠΎΠ·Π°Π½-Γ-ΡΠΈΠΊΠ»ΠΎΠ΄Π΅ΠΊΡΡΡΠΈΠ½ Ρ Π»Π΅Π²ΠΎΡΠ»ΠΎΠΊΡΠ°ΡΠΈΠ½ΠΎΠΌ Π² Π·Π°ΠΆΠΈΠ²Π»Π΅Π½ΠΈΠΈ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ°Π½ ΡΠ΅Π½Π½ΡΡ
ΠΏΡΠΎΠΌΡΡΠ»ΠΎΠ²ΡΡ
ΡΡΠ± β ΠΎΡΠ΅ΡΡΠΎΠ² ΠΈ ΠΈΡ
ΠΊΠΎΡΠΌΠ»Π΅Π½ΠΈΠΈ. ΠΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½Ρ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π° Π±Π°Π·Π΅ Π½Π°ΡΡΠ½ΠΎ-ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΡΠΊΠΎΠΉ Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠΈΠΈ Β«ΠΡΠΎΠ³ΡΠ΅ΡΡΠΈΠ²Π½ΡΠ΅ Π±ΠΈΠΎΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π² Π°ΠΊΠ²Π°ΠΊΡΠ»ΡΡΡΡΠ΅Β» Π‘Π°ΡΠ°ΡΠΎΠ²ΡΠΊΠΎΠ³ΠΎ Π³ΠΎΡΡΠ΄Π°ΡΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΡΠ½ΠΈΠ²Π΅ΡΡΠΈΡΠ΅ΡΠ° Π³Π΅Π½Π΅ΡΠΈΠΊΠΈ, Π±ΠΈΠΎΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈ ΠΈΠ½ΠΆΠ΅Π½Π΅ΡΠΈΠΈ ΠΈΠΌ. Π.Π. ΠΠ°Π²ΠΈΠ»ΠΎΠ²Π°. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»Π°ΡΡ ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΠ° ΡΠ΅Π·Π°Π½ΡΡ
ΡΠ°Π½ ΠΈ ΡΠΎΠ»ΡΡΠΎΠ³ΠΎ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ° ΡΠ΅Π³ΠΎΠ»Π΅ΡΠΊΠΎΠ² ΠΎΡΠ΅ΡΡΠΎΠ² ΠΏΠΎΠ΄ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ ΡΡΠΎΡΡ
ΠΈΠ½ΠΎΠ»ΠΎΠ½Π°, ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΠΎΠ³ΠΎ Π»Π΅Π²ΠΎΡΠ»ΠΎΠΊΡΠ°ΡΠΈΠ½ΠΎΠΌ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠΈΠΊΠ»ΠΎΠ΄Π΅ΠΊΡΡΡΠΈΠ½Π°, Π²ΠΊΠ»ΡΡΠ΅Π½Π½ΠΎΠ³ΠΎ Π² ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΡ Π²ΡΡΠΎΠΊΠΎΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΠΎΠ³ΠΎ Ρ
ΠΈΡΠΎΠ·Π°Π½Π°. ΠΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΡΠ΅ ΠΌΠΈΠΊΡΠΎΠ±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΠΈ Π±ΡΠ»ΠΈ Π²ΡΠ±ΡΠ°Π½Ρ Π΄Π»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π½Π° ΡΠΎΠΌ ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ, ΡΡΠΎ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΎΠ±ΡΠ΅Π³ΠΎ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π° ΠΌΠΈΠΊΡΠΎΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌΠΎΠ² ΠΏΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅Ρ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ/ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅ΡΡΠ°, ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΡΡΡΠ΅Π³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΌΠΈΠΊΡΠΎΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌΠΎΠ² (Π² Ρ.Ρ. ΡΡΠ»ΠΎΠ²Π½ΠΎ-ΠΏΠ°ΡΠΎΠ³Π΅Π½Π½ΡΡ
) ΠΈ ΠΌΠΎΠ»ΠΎΡΠ½ΠΎΠΊΠΈΡΠ»ΡΡ
Π±Π°ΠΊΡΠ΅ΡΠΈΠΉ Π² ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ΅, ΠΏΠΎΡΡΠΎΠΌΡ ΡΠ²Π»ΡΡΡΡΡ Π²Π°ΠΆΠ½ΡΠΌΠΈ ΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΠΌΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Β«ΠΊΠΈΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΠΌΠΌΡΠ½ΠΈΡΠ΅ΡΠ°Β». ΠΡΠ»ΠΎ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΎ, ΡΡΠΎ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΡΠΈ Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΡΠ΅Π·Π°Π½ΡΡ
ΡΠ°Π½ Ρ ΠΎΡΠ΅ΡΡΠΎΠ² ΡΠΈΠΊΠ»ΠΎΠ΄Π΅ΠΊΡΡΡΠΈΠ½Π° Ρ Π»Π΅Π²ΠΎΡΠ»ΠΎΠΊΡΠ°ΡΠΈΠ½ΠΎΠΌ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠΌΡ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ ΠΎΠ±ΡΠ΅Π³ΠΎ ΠΌΠΈΠΊΡΠΎΠ±Π½ΠΎΠ³ΠΎ ΡΠΈΡΠ»Π° (ΠΠΠ§) Π½Π° ΠΈΡ
ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ (Π² 10 ΡΡΡ. ΡΠ°Π· ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ Π³ΡΡΠΏΠΏΠΎΠΉ Π±Π΅Π· Π»Π΅ΡΠ΅Π½ΠΈΡ). ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ Π² ΠΊΠΎΡΠΌΠ»Π΅Π½ΠΈΠΈ ΠΎΡΠ΅ΡΡΠΎΠ² ΡΠΈΠΊΠ»ΠΎΠ΄Π΅ΠΊΡΡΡΠΈΠ½Π° Ρ Π»Π΅Π²ΠΎΡΠ»ΠΎΠΊΡΠ°ΡΠΈΠ½ΠΎΠΌ ΡΠ°ΠΊΠΆΠ΅ ΡΠ½ΠΈΠΆΠ°Π΅Ρ ΠΎΠ±ΡΠ΅Π΅ ΠΌΠΈΠΊΡΠΎΠ±Π½ΠΎΠ΅ ΡΠΈΡΠ»ΠΎ Π² ΡΠΎΠ»ΡΡΠΎΠΌ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ΅. ΠΠ°Π½Π½ΡΠΉ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅ΡΡΡ Ρ
ΠΎΡΠΎΡΠ΅ΠΉ ΡΠ°ΡΡΠ²ΠΎΡΠΈΠΌΠΎΡΡΡΡ ΠΈ Π±ΠΈΠΎΠ΄ΠΎΡΡΡΠΏΠ½ΠΎΡΡΡΡ Π΄Π»Ρ ΡΡΠ±. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π² ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π΅ ΠΌΠΎΠ³ΡΡ Π½Π°ΠΉΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π² Π°ΠΊΠ²Π°ΠΊΡΠ»ΡΡΡΡΠ΅ ΠΏΡΠΈ Π»Π΅ΡΠ΅Π½ΠΈΠΈ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ°Π²ΠΌ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΠΏΡΠΈ ΠΏΠ΅ΡΠ΅Π²ΠΎΠ·ΠΊΠ΅ ΠΈ ΡΠΎΡΡΠΈΡΠΎΠ²ΠΊΠ΅ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ Π²ΡΡΠ°ΡΠΈΠ²Π°Π½ΠΈΡ, Ρ ΡΡΠ±
Majorana vortex modes in spin-singlet chiral superconductors with noncollinear spin ordering: Local density of states study
In the present study topologically nontrivial edge and vortex bound states
are described in the coexistence phase of chiral spin-singlet superconductivity
and noncollinear spin ordering on a triangular lattice. Since chiral
superconductivity is nodeless in a wide range of parameters, the obtained bound
states are separated from trivial bulk states. It is proved that Majorana modes
localized at vortex cores are caused by noncollinear long-range magnetic
ordering. Even though nearby excitation energies of subgap states including the
edge-localized and vortex-localized states are very close to each other, the
energy difference between different vortex bound states is an order of
magnitude higher. It opens the way to experimentally detect the zero energy
Majorana modes localized at vortex cores in the considered structures by using
methods measuring local density of states such as tunneling experiments. For a
few pairs of vortices, vortex bound states with near zero energy can appear.
Nevertheless, they are localized on different vortices in comparison with the
localization of Majorana vortex modes. In this case zero modes are still
separated in energy and space from other states in local density of states
results. The difference between density of states near the vortex and near the
antivortex hosting Majorana modes is also demonstrated.Comment: 10 pages, 10 figure
Hierarchical Calcite Crystals with Occlusions of a Simple Polyelectrolyte Mimic Complex Biomineral Structures
Biominerals are complex inorganic-organic structures that often show excellent mechanical properties. Here a bio-inspired study of a remarkably simple synthetic system is presented in which only one charged polymer additive (poly(sodium 4-styrenesulfonate)) is able to induce hierarchical structuring of calcite similar to biominerals. The interaction of the negatively charged polymer with the nucleation and growth of the mineral, in particular via selective adsorption to internal and external (001) facets of the calcite lattice, implies structural features from the micrometer down to the nanometer level. The crystals exhibit a distinct rounded morphology and a controlled orientation. Moreover, the polymer molecules are occluded within the crystals with different concentrations in well-defined regions. This leads to the induction of a mesoscale structure based on 100 nm sized mineral building blocks with granular substructure and rough surface, as well as small modifications of the crystallographic structure. Such a combination of hierarchically organized structural features has previously only been reported for biogenic calcite, which is typically grown in a complex process involving multiple organic additives. It is also shown that the organic occlusions in the calcite-PSS hybrid crystals strongly affect the mechanical performance, as known for some biominerals
Micro- and nano-structural details of a spider's filter for substrate vibrations : relevance for low-frequency signal transmission
The metatarsal lyriform organ of the Central American wandering spider Cupiennius salei is its most sensitive vibration detector. It is able to sense a wide range of vibration stimuli over four orders of magnitude in frequency between at least as low as 0.1 Hz and several kilohertz. Transmission of the vibrations to the slit organ is controlled by a cuticular pad in front of it. While the mechanism of high-frequency stimulus transfer (above ca 40 Hz) is well understood and related to the viscoelastic properties of the pad's epicuticle, it is not yet clear how low-frequency stimuli (less than 40 Hz) are transmitted. Here, we study how the pad material affects the pad's mechanical properties and thus its role in the transfer of the stimulus, using a variety of experimental techniques, such as X-ray micro-computed tomography for three-dimensional imaging, X-ray scattering for structural analysis, and atomic force microscopy and scanning electron microscopy for surface imaging. The mechanical properties were investigated using scanning acoustic microscopy and nanoindentation. We show that large tarsal deflections cause large deformation in the distal highly hydrated part of the pad. Beyond this region, a sclerotized region serves as a supporting frame which resists the deformation and is displaced to push against the slits, with displacement values considerably scaled down to only a few micrometres. Unravelling the structural arrangement in such specialized structures may provide conceptual ideas for the design of new materials capable of controlling a technical sensor's specificity and selectivity, which is so typical of biological sensors