Searching for Afterglow: Light Dark Matter Boosted by Supernova Neutrinos.

A novel analysis is performed, incorporating time-of-flight (TOF) information to study the interactions of dark matter (DM) with standard model particles. After supernova (SN) explosions, DM with mass m_{χ}≲O(MeV) in the halo can be boosted by SN neutrinos (SNν) to relativistic speed. The SNν boosted DM (BDM) arrives on Earth with TOF which depends only on m_{χ} and is independent of the cross section. These BDMs can interact with detector targets in low-background experiments and manifest as afterglow events after the arrival of SNν. The characteristic TOF spectra of the BDM events can lead to large background suppression and unique determination of m_{χ}. New cross section constraints on sqrt[σ_{χe}σ_{χν}] are derived from SN1987a in the Large Magellanic Cloud with data from the Kamiokande and Super-Kamiokande experiments. Potential sensitivities for the next galactic SN with Hyper-Kamiokande are projected. This analysis extends the existing bounds on sqrt[σ_{χe}σ_{χν}] over a broad range of r_{χ}=σ_{χν}/σ_{χe}. In particular, the improvement is by 1-3 orders of magnitude for m_{χ}

E-Z Isomerization Mechanism of the Green Fluorescent Protein Chromophore: Remote Regulation by Proton Dissociation of the Phenol Group.

Dronpa, a GFP (green fluorescent protein)-like fluorescent protein, allows its fluorescent and nonfluorescent states to be switched to each other reversibly by light or heat through E-Z isomerization of the GFP chromophore. In this article, a GFP chromophore (p-HBDI) in water is used as a model to explore this E-Z isomerization mechanism. Based on the experimental solvent isotope effect (kH2O/kD2O = 2.30), the E-Z isomerization of p-HBDI in water is suggested to go through the remote-proton-dissociation-regulated direct mechanism with a proton transfer in the rate-determining step. The fractionation factor (ϕ) of the water-associated phenol proton of p-HBDI in the transition state is found to be 0.43, which is exactly in the range of 0.1-0.6 for the fractionation factor (ϕ) of the transferring proton in the transition state of R2O···H···O+H2 in water. This means that the phenol proton of E-p-HBDI in the transition state is on the way to the associated water oxygen during the E-Z isomerization. The proton dissociation from the phenol group of p-HBDI remotely regulates its E-Z isomerization. Less proton dissociation from the phenol group (pKa = 8.0) at pH = 1-4 results in a modest reduction in the E-Z isomerization rate of p-HBDI, while complete proton dissociation from the phenol group at pH = 11-12 also reduces its E-Z isomerization rate by one order of magnitude because of the larger charge separation in the transition state of the p-HBDI anion. All of these results are consistent with the remote-proton-dissociation-regulated direct mechanism but against the water-assisted addition/elimination mechanism.

Enormous Berry-Curvature-Based Anomalous Hall Effect in Topological Insulator (Bi,Sb)2Te3 on Ferrimagnetic Europium Iron Garnet beyond 400 K.

To realize the quantum anomalous Hall effect (QAHE) at elevated temperatures, the approach of magnetic proximity effect (MPE) was adopted to break the time-reversal symmetry in the topological insulator (Bi0.3Sb0.7)2Te3 (BST) based heterostructures with a ferrimagnetic insulator europium iron garnet (EuIG) of perpendicular magnetic anisotropy. Here we demonstrate large anomalous Hall resistance (RAHE) exceeding 8 Ω (ρAHE of 3.2 µΩ·cm) at 300 K and sustaining to 400 K in 35 BST/EuIG samples, surpassing the past record of 0.28 Ω (ρAHE of 0.14 µΩ·cm) at 300 K. The large RAHE is attributed to an atomically abrupt, Fe-rich interface between BST and EuIG. Importantly, the gate dependence of the AHE loops shows no sign change with varying chemical potential. This observation is supported by our first-principles calculations via applying a gradient Zeeman field plus a contact potential on BST. Our calculations further demonstrate that the AHE in this heterostructure is attributed to the intrinsic Berry curvature. Furthermore, for gate-biased 4 nm BST on EuIG, a pronounced topological Hall effect-like (THE-like) feature coexisting with AHE is observed at the negative top-gate voltage up to 15 K. Interface tuning with theoretical calculations has realized topologically distinct phenomena in tailored magnetic TI-based heterostructures.

Epitaxy from a Periodic Y-O Monolayer: Growth of Single-Crystal Hexagonal YAlO3 Perovskite.

The role of an atomic-layer thick periodic Y-O array in inducing the epitaxial growth of single-crystal hexagonal YAlO3 perovskite (H-YAP) films was studied using high-angle annular dark-field and annular bright-field scanning transmission electron microscopy in conjunction with a spherical aberration-corrected probe and in situ reflection high-energy electron diffraction. We observed the Y-O array at the interface of amorphous atomic layer deposition (ALD) sub-nano-laminated (snl) Al2O3/Y2O3 multilayers and GaAs(111)A, with the first film deposition being three cycles of ALD-Y2O3. This thin array was a seed layer for growing the H-YAP from the ALD snl multilayers with 900 °C rapid thermal annealing (RTA). The annealed film only contained H-YAP with an excellent crystallinity and an atomically sharp interface with the substrate. The initial Y-O array became the bottom layer of H-YAP, bonding with Ga, the top layer of GaAs. Using a similar ALD snl multilayer, but with the first film deposition of three ALD-Al2O3 cycles, there was no observation of a periodic atomic array at the interface. RTA of the sample to 900 °C resulted in a non-uniform film, mixing amorphous regions and island-like H-YAP domains. The results indicate that the epitaxial H-YAP was induced from the atomic-layer thick periodic Y-O array, rather than from GaAs(111)A.