Giant and anisotropic many-body spin-orbit tunability in a strongly correlated kagome magnet.

Owing to the unusual geometry of kagome lattices-lattices made of corner-sharing triangles-their electrons are useful for studying the physics of frustrated, correlated and topological quantum electronic states1-9. In the presence of strong spin-orbit coupling, the magnetic and electronic structures of kagome lattices are further entangled, which can lead to hitherto unknown spin-orbit phenomena. Here we use a combination of vector-magnetic-field capability and scanning tunnelling microscopy to elucidate the spin-orbit nature of the kagome ferromagnet Fe3Sn2 and explore the associated exotic correlated phenomena. We discover that a many-body electronic state from the kagome lattice couples strongly to the vector field with three-dimensional anisotropy, exhibiting a magnetization-driven giant nematic (two-fold-symmetric) energy shift. Probing the fermionic quasi-particle interference reveals consistent spontaneous nematicity-a clear indication of electron correlation-and vector magnetization is capable of altering this state, thus controlling the many-body electronic symmetry. These spin-driven giant electronic responses go well beyond Zeeman physics and point to the realization of an underlying correlated magnetic topological phase. The tunability of this kagome magnet reveals a strong interplay between an externally applied field, electronic excitations and nematicity, providing new ways of controlling spin-orbit properties and exploring emergent phenomena in topological or quantum materials10-12.

Self-Intercalated 1T-FeSe2 as an Effective Kagome Lattice.

In kagome lattice, with the emergence of Dirac cones and flat band in electronic structure, it provides a versatile ground for exploring intriguing interplay among frustrated geometry, topology and correlation. However, such engaging interest is strongly limited by available kagome materials in nature. Here we report on a synthetic strategy of constructing kagome systems via self-intercalation of Fe atoms into the van der Waals gap of FeSe2 via molecular beam epitaxy. Using low-temperature scanning tunneling microscopy, we unveil a kagome-like morphology upon intercalating a 2 × 2 ordered Fe atoms, resulting in a stoichiometry of Fe5Se8. Both the bias-dependent STM imaging and theoretical modeling calculations suggest that the kagome pattern mainly originates from slight but important reconstruction of topmost Se atoms, incurred by the nonequivalent subsurface Fe sites due to the intercalation. Our study demonstrates an alternative approach of constructing artificial kagome structures, which envisions to be tuned for exploring correlated quantum states.

Erratum: Eightfold Degenerate Fermions in Two Dimensions [Phys. Rev. Lett. 127, 176401 (2021)].

This corrects the article DOI: 10.1103/PhysRevLett.127.176401.

Eightfold Degenerate Fermions in Two Dimensions.

Multifold degenerate fermions have attracted a lot of research interest in condensed matter physics and materials science, but always lack in two dimensions. In this Letter, from symmetry analysis and lattice model construction, we demonstrate that eightfold degenerate fermions can be realized in two-dimensional systems. In nonmagnetic materials with negligible spin-orbit coupling, the gray magnetic space groups together with SU(2) spin rotation symmetry can protect the two-dimensional eightfold degenerate fermions on a certain high-symmetry axis in the Brillouin zone, no matter whether the system is centrosymmetric or noncentrosymmetric. In antiferromagnetic materials, the eightfold degenerate fermions can also be protected by certain "spin space groups." Furthermore, by first-principles electronic structure calculations, we predict that the paramagnetic phase of the monolayer LaB_{8} on a suitable substrate is a two-dimensional eightfold degenerate as well as Dirac node-line semimetal. Especially, the eightfold degenerate points are close to the Fermi level, which makes monolayer LaB_{8} a good platform to study the exotic physical properties of two-dimensional eightfold degenerate fermions.

Diagnosis of Interaction-driven Topological Phase via Exact Diagonalization.

We propose a general scheme for diagnosing interaction-driven topological phases in the weak interaction regime using exact diagonalization (ED). The scheme comprises the analysis of eigenvalues of the point-group operators for the many-body eigenstates and the correlation functions for physical observables to extract the symmetries of the order parameters and the topological numbers of the underlying ground states at the thermodynamic limit from a relatively small size system afforded by ED. As a concrete example, we investigate the interaction effects on the half-filled spinless fermions on the checkerboard lattice with a quadratic band crossing point. Numerical results support the existence of a spontaneous quantum anomalous Hall phase purely driven by a nearest-neighbor weak repulsive interaction, separated from a nematic Mott insulator phase at strong repulsive interaction by a first-order phase transition.

Neutron scattering measurements of spatially anisotropic magnetic exchange interactions in semiconducting K0.85 Fe1.54Se2 (TN = 280 K.

We use neutron scattering to study the spin excitations associated with the stripe antiferromagnetic order in semiconducting K(0.85)Fe(1.54)Se(2) (T(N) = 280 K). We show that the spin-wave spectra can be accurately described by an effective Heisenberg Hamiltonian with highly anisotropic inplane couplings at T = 5 K. At high temperature (T = 300 K) above T(N), short-range magnetic correlation with anisotropic correlation lengths are observed. Our results suggest that, despite the dramatic difference in the Fermi surface topology, the inplane anisotropic magnetic couplings are a fundamental property of the iron-based compounds; this implies that their antiferromagnetism may originate from local strong correlation effects rather than weak coupling Fermi surface nesting.

Spin-Resolved Imaging of Antiferromagnetic Order in Fe4 Se5 Ultrathin Films on SrTiO3.

Unraveling the magnetic order in iron chalcogenides and pnictides at atomic scale is pivotal for understanding their unconventional superconducting pairing mechanism, but is experimentally challenging. Here, by utilizing spin-polarized scanning tunneling microscopy, real-space spin contrasts are successfully resolved to exhibit atomically unidirectional stripes in Fe4 Se5 ultrathin films, the plausible closely related compound of bulk FeSe with ordered Fe-vacancies, which are grown by molecular beam epitaxy. As is substantiated by the first-principles electronic structure calculations, the spin contrast originates from a pair-checkerboard antiferromagnetic ground state with in-plane magnetization, which is modulated by a spin-lattice coupling. These measurements further identify three types of nanoscale antiferromagnetic domains with distinguishable spin contrasts, which are subject to thermal fluctuations into short-ranged patches at elevated temperatures. This work provides promising opportunities in understanding the emergent magnetic order and the electronic phase diagram for FeSe-derived superconductors.

Pressure-induced superconductivity at 32 K in MoB2.

Since the discovery of superconductivity in MgB2 (Tc ∼ 39 K), the search for superconductivity in related materials with similar structures or ingredients has never stopped. Although about 100 binary borides have been explored, only a few of them show superconductivity with relatively low Tc. In this work, we report the discovery of superconductivity up to 32 K, which is the highest Tc in transition-metal borides, in MoB2 under pressure. The Tc of MoB2 in the α phase can be well explained by theoretical calculations in the framework of electron-phonon coupling. Furthermore, the coupling between the d electrons of Mo and the out-of-plane Mo-phonon modes are the main driving force of the 32 K superconductivity of MoB2. Our study sheds light on the exploration of high-Tc superconductors in transition metal borides.

[The expression of α-smooth muscle actin during the lung injury induced by hyperoxia].

OBJECTIVE: To explore the expression of α-smooth muscle actin (α-SMA) during the lung injury induced by hyperoxia in infantile rats. METHODS: Sixty-four male Sprague-Dawley (SD) rats about 3 weeks were randomly assigned into normal control group which exposured to room air [fraction of inspired oxygen (FiO(2)) was 0.21] and hyperoxia exposure group (95%O(2)) according to random digits table. Eight rats in each group were randomly sacrificed at day 1, 7, 14 and 21.Pulmonary tissue remodeling was observed by hematoxylin-eosin (HE) staining. Immunohistochemistry method was performed to evaluate the expression of α-SMA in pulmonary tissue, further Western blotting was also made to determine the expression of α-SMA. RESULTS: The early histopathologic changes after HE were inflammation and edema in pulmonary tissue, while the later changes were interstitial hyperplasia and fibroblast proliferation. The expression of α-SMA was very slight in bronchial epithelium, alveolar epithelium and alveolar interstitium in normal control group, but increased with the time of hyperoxia exposure prolonged and peaked at 21st day. Western blotting detected that the expression of α-SMA after hyperoxia exposure for 1 day and 7 days in hyperoxia exposure group presented no difference compared with normal control group (1.02±0.12 vs. 1.00±0.13, 1.05±0.14 vs. 0.99±0.12, both P>0.05), but the expression of α-SMA after hyperoxia exposure for 14 days and 21 days was increased compared with normal control group (1.27±0.21 vs. 1.05±0.15, 2.26±0.28 vs. 1.05±0.14, P<0.05 and P<0.01). CONCLUSIONS: Pulmonary fibrosis remodeling was caused by hyperoxia exposure. The expression of α-SMA in pulmonary tissue in hyperoxia exposure groups obviously increased, and could play an important role in pulmonary fibrosis remodeling.

A two-dimensional topological nodal-line material MgN4 with extremely large magnetoresistance.

Using first-principles calculations, we predict a stable two-dimensional atomically thin material MgN4. This material has a perfect intrinsic electron-hole compensation characteristic with high carrier mobility, making it a promising candidate material with extremely large magnetoresistance. As the magnetic field increases, the magnetoresistance of the monolayer MgN4 will show a quadratic dependence on the strength of the magnetic field without saturation. Furthermore, nontrivial topological properties are also found in this material. In the absence of spin-orbit coupling, the monolayer MgN4 belongs to a topological nodal-line material, in which the band crossings form a closed saddle-shape nodal-ring near the Fermi level in the Brillouin zone. Once the spin-orbit coupling is considered, a small local energy gap is opened along the nodal ring, resulting in a topological insulator defined on a curved Fermi surface with 2 = 1. The combination of two-dimensional single-atomic-layer thickness, an extremely large magnetoresistance effect, and topological non-trivial properties in the monolayer MgN4 makes it an excellent platform for designing novel multi-functional devices.

Pressure-induced isostructural phase transition and correlation of FeAs coordination with the superconducting properties of 111-type Na(1-x)FeAs.

The effect of pressure on the crystalline structure and superconducting transition temperature (T(c)) of the 111-type Na(1-x)FeAs system using in situ high-pressure synchrotron X-ray powder diffraction and diamond anvil cell techniques is studied. A pressure-induced tetragonal to tetragonal isostructural phase transition was found. The systematic evolution of the FeAs(4) tetrahedron as a function of pressure based on Rietveld refinements on the powder X-ray diffraction patterns was obtained. The nonmonotonic T(c)(P) behavior of Na(1-x)FeAs is found to correlate with the anomalies of the distance between the anion (As) and the iron layer as well as the bond angle of As-Fe-As for the two tetragonal phases. This behavior provides the key structural information in understanding the origin of the pressure dependence of T(c) for 111-type iron pnictide superconductors. A pressure-induced structural phase transition is also observed at 20 GPa.

Electronic structures and magnetic order of ordered-Fe-vacancy ternary iron selenides TlFe1.5Se2 and AFe1.5Se2 (A=K, Rb, or Cs).

By the first-principles electronic structure calculations, we find that the ground state of the Fe-vacancies ordered TlFe(1.5)Se(2) is a quasi-two-dimensional collinear antiferromagnetic semiconductor with an energy gap of 94 meV, in agreement with experimental measurements. This antiferromagnetic order is driven by the Se-bridged antiferromagnetic superexchange interactions between Fe moments. Similarly, we find that crystals AFe(1.5)Se(2) (A=K, Rb, or Cs) are also antiferromagnetic semiconductors but with a zero-gap semiconducting state or semimetallic state nearly degenerated with the ground states. Thus, rich physical properties and phase diagrams are expected.

N-acetylcysteine protects alveolar epithelial cells from hydrogen peroxide-induced apoptosis through scavenging reactive oxygen species and suppressing c-Jun N-terminal kinase.

The production of reactive oxygen species (ROS) during hyperoxia contribute to alveolar epithelial apoptosis. In the present study, the molecular mechanisms of oxidative stress-induced alveolar epithelial cell apoptosis were investigated. The cytoprotective effects of N-acetylcysteine (NAC) were evaluated. Treatments using 500 muM H(2)O(2) can induce primary alveolar type II epithelial cell apoptosis. During this procedure, c-Jun N-terminal kinase (JNK) was activated. SP600125, a specific inhibitor of JNK, can partially block H(2)O(2)-induced alveolar type II epithelial cells (ATII cells). SP600125 also attenuated Bax protein content and p53 nuclear accumulation induced by H(2)O(2). NAC (5 mM) pretreatment decreased H(2)O(2)-induced ATII cell apoptosis. The high level of intracellular reactive oxygen species (ROS) induced by H(2)O(2) was also attenuated by NAC pretreatment. Taken together, H(2)O(2) can induce primary ATII cells apoptosis and increase JNK phosphorylation. NAC, a precursor of glutathione (GSH) synthesis, can protect ATII cells from H(2)O(2)-induced apoptosis through scavenging ROS.

Interlayer quantum transport in Dirac semimetal BaGa2.

The quantum limit is quite easy to achieve once the band crossing exists exactly at the Fermi level (EF) in topological semimetals. In multilayered Dirac fermion systems, the density of Dirac fermions on the zeroth Landau levels (LLs) increases in proportion to the magnetic field, resulting in intriguing angle- and field-dependent interlayer tunneling conductivity near the quantum limit. BaGa2 is an example of a multilayered Dirac semimetal with its quasi-2D Dirac cone located at EF, providing a good platform to study its interlayer transport properties. In this paper, we report the negative interlayer magnetoresistance induced by the tunneling of Dirac fermions between the zeroth LLs of neighboring Ga layers in BaGa2. When the field deviates from the c-axis, the interlayer resistivity ρzz(θ) increases and finally results in a peak with the applied field perpendicular to the c-axis. These unusual interlayer transport properties are observed together in the Dirac semimetal under ambient pressure and are well explained by the model of tunneling between Dirac fermions in the quantum limit.

Pi junction to probe antiphase s-wave pairing in iron pnictide superconductors.

Josephson junctions between a FeAs-based superconductor with antiphase s-wave pairing and a conventional s-wave superconductor are studied. The translational invariance in a planar junction between a single crystal pnictide and an aluminum metal greatly enhances the relative weight of electron pockets in the pnictide to the critical current. In a wide doping region of the pnictide, a planar and a point contact junction have opposite phases, which can be used to design a trijunction ring with pi phase to probe the antiphase pairing.

[Expression and role of p38 mitogen-activated protein kinase in hyperoxia-induced lung injury juvenile rat model].

OBJECTIVE: Some research has shown that p38 mitogen-activated protein kinase (p38MAPK) plays important roles in lung injuries induced by various factors. Its expression and role in hyperoxia-induced lung injury remains unknown. This study investigated the expression and role of p38MAPK in hyperoxia-induced lung injury juvenile rat model. METHODS: Hyperoxia-induced lung injury rat model was prepared by 90% O(2) exposure. The location and expression of p38MAPK in lung tissues were detected by immunohistochemistry and Western blot respectively. Apoptosis index of lung was evaluated by TUNEL technique. The effect of SB203580, a p38MAPK inhibitor, on the apoptosis index of lung was observed. RESULTS: The expression of phosphor-p38MAPK increased obviously after hyperoxia. Positive phosphor-p38MAPK cells were mainly distributed in the alveolar, airway epithelial cells, pulmonary vascular endothelium cells and infiltrative inflammatory cells. The apoptosis index of lung also significantly elevated. SB203580 inhibited the activation of p38MAPK, and reduced the apoptosis index of lung. CONCLUSIONS: The phosphor-p38MAPK increased and was expressed in many kinds of lung cells in lung injury rat model. It may play a role in the induction of apoptosis in hyperoxia-induced lung injury.

A family of high-temperature ferromagnetic monolayers with locked spin-dichroism-mobility anisotropy: MnNX and CrCX (X = Cl, Br, I; C = S, Se, Te).

Two-dimensional magnets have received increasing attention since Cr2Ge2Te6 and CrI3 were experimentally exfoliated and measured in 2017. Although layered ferromagnetic metals were demonstrated at room temperature, a layered ferromagnetic semiconductor with high Curie temperature (Tc) is yet to be unveiled. Here, we theoretically predicted a family of high Tc ferromagnetic monolayers, namely MnNX and CrCX (X = Cl, Br and I; C = S, Se and Te). Their Tc values were predicted from over 100 K to near 500 K with Monte Carlo simulations using an anisotropic Heisenberg model. Eight members among them show semiconducting bandgaps varying from roughly 0.23 to 1.85 eV. These semiconducting monolayers also show extremely large anisotropy, i.e. ∼101 for effective masses and ∼102 for carrier mobilities, along the two in-plane lattice directions of these layers. Additional orbital anisotropy leads to a spin-locked linear dichroism, in different from previously known circular and linear dichroisms in layered materials. Together with the mobility anisotropy, it offers a spin-, dichroism- and mobility-anisotropy locking. These results manifest the potential of this 2D family for both fundamental research and high performance spin-dependent electronic and optoelectronic devices.

Quasi-degenerate magnetic states in α-RuCl3.

Exploring quantum spin liquid (QSL) state has both fundamental scientific value and realistic application potential. Recently, α-RuCl3 was experimentally observed to hold in-plane zigzag antiferromagnetic (AFM) order at low temperature, which was further proposed to be proximate to a Kitaev QSL ground state. We have studied the magnetic properties of α-RuCl3 in the framework of electronic structure calculation based on density functional theory (DFT) with Hubbard U correction (DFT+U) and spin-orbit coupling. When the intra-orbital Hubbard interaction U and the inter-orbital Hund's coupling J adopt the commonly accepted values of U = 2.0 eV and J = 0.4 eV, the zigzag AFM order indeed owns the minimum energy, consistent with the experimental observation. More importantly, we find that compared with the ferromagnetic order in the previous theoretical studies, there exist a series of magnetic configurations energetically even closer to the zigzag AFM ground state. The further calculations and analysis indicate that these low-energy magnetic states are closely related to the electronic correlation effect of Ru 4d orbitals. By decreasing U and increasing J with just about 0.2 eV, they become energetically degenerate with the zigzag AFM order, inducing strong magnetic frustration and then yielding a state without long-range magnetic order but with nonzero local moments. Considering the facts that theoretically the pressure usually reduces the intra-orbital Hubbard interaction and meanwhile enhances the inter-orbital Hund's coupling, while experimentally the pressure drives α-RuCl3 into a quantum disordered phase, our results provide a perspective to understand the exotic magnetic behaviors of α-RuCl3.

[Oxidative stress induced the expression of Bax and p53 during the apoptosis of alveolar type II epithelial cell].

OBJECTIVE: To investigate the effects of oxidative stress on the survival and apoptosis of alveolar epithelial type II (ATII) cells, as well as the mechanisms of apoptosis. METHODS: 500 mumol/L H(2)O(2) was added into primary ATII cells at different times and cell viability, apoptotic ratio and the expression of Bax and p53 were measured by 3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyltetrazolium bromide (MTT) assay, flow cytometry (FCM) and Western blotting analysis, respectively. The change in mitochondrial membrane potential (MMP) was detected by fluorescence microscopy and FCM. RESULTS: The cell viability and MMP were decreased by H(2)O(2) compared with the controls (F(1)=85.211, F(2)=72.453, respectively, both P<0.05). The cell apoptotic ratios were increased with the time of the stimulation prolonged compared with the controls (F=54.002, P<0.05). H(2)O(2) increased Bax and p53 protein levels (F(1)=28.118, F(2)=43.456, both P<0.05). CONCLUSION: High level of oxidative stress can inhibit ATII cells proliferation, and induce cells apoptosis and decrease the MMP. Up-regulation of the expression of Bax and p53 may contribute to its apoptosis effects.

[Changes of aquaporin expression during lung development in rats].

OBJECTIVE: Many studies have shown that tissue development is closely correlated with fluid transport. Aquaporins (AQPs) are a group of cell membrane proteins that actively and selectively transport water. This study aimed to investigate the changes of AQPs expression during lung development in rats in order to elucidate the role of AQPs in the rat lung development. METHODS: AQP1, AQP3, AQP4 and AQP5 proteins and mRNA in the lung cell membrane were measured by immunohistochemistry and reverse transcription-polymerase chain reaction (RT-PCR) respectively in the 20-day-old embryo (E20), 7-day-old newborn rat, and one-month-old young and adult rats. The correlation between AQPs expression and lung development was studied. RESULTS: With increasing age, the lung development showed a dynamic and successive course, with the most rapid from the fetus to the newborn rat, and then a slowed down afterwards. AQPs mRNA was weakly expressed in the lung of the E20 group. Lung AQPs mRNA and protein increased rapidly after birth until adulthood. The AQPs distribution patterns in the lung were unique with no duplication. There was a positive correlation between AQPs expression and lung development (P<0.05). CONCLUSIONS: In addition to being involved in the transepithelial transport of water in the lung, AQPs is also related to its development.