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Interplay between Local Moment and Itinerant Magnetism in the Layered Metallic Antiferromagnet TaFe 1.14 Te 3

Two-dimensional antiferromagnets have garnered considerable interest for the next generation of functional spintronics. However, many bulk materials from which two-dimensional antiferromagnets are isolated are limited by their air sensitivity, low ordering temperatures, and insulating transport properties. TaFe 1+y Te 3 aims to address these challenges with increased air stability, metallic transport, and robust antiferromagnetism. Here, we synthesize TaFe 1+y Te 3 (y = 0.14), identify its structural, magnetic, and electronic properties, and elucidate the relationships between them. Axial-dependent high-field magnetization measurements on TaFe 1.14 Te 3 reveal saturation magnetic fields ranging between 27-30 T with saturation magnetic moments of 2.05- 2.12 μ B . Magnetotransport measurements confirm TaFe 1.14 Te 3 is metallic with strong coupling between magnetic order and electronic transport. Angle-resolved photoemission spectroscopy measurements across the magnetic transition uncover a complex interplay between itinerant electrons and local magnetic moments that drives the magnetic transition. In conclusion, we demonstrate the ability to isolate few-layer sheets of TaFe 1.14 Te 3 , establishing TaFe 1.14 Te 3 as a potential platform for two-dimensional spintronics.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Materials Data on TaFe(PbO3)2 by Materials Project

TaFe(PbO3)2 is (Cubic) Perovskite-derived structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Ta5+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with six equivalent FeO6 octahedra and faces with eight equivalent PbO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Ta–O bond lengths are 2.00 Å. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent TaO6 octahedra and faces with eight equivalent PbO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. There is four shorter (1.95 Å) and two longer (2.02 Å) Fe–O bond length. Pb2+ is bonded to twelve O2- atoms to form PbO12 cuboctahedra that share corners with twelve equivalent PbO12 cuboctahedra, faces with six equivalent PbO12 cuboctahedra, faces with four equivalent TaO6 octahedra, and faces with four equivalent FeO6 octahedra. There are four shorter (2.80 Å) and eight longer (2.82 Å) Pb–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to one Ta5+, one Fe3+, and four equivalent Pb2+ atoms. In the second O2- site, O2- is bonded in a distorted linear geometry to one Ta5+, one Fe3+, and four equivalent Pb2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on TaFe by Materials Project

FeTa is Frank-Kasper $\mu$ Phase-like structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are seven inequivalent Ta sites. In the first Ta site, Ta is bonded in a 6-coordinate geometry to eight Ta and six equivalent Fe atoms. There are a spread of Ta–Ta bond distances ranging from 2.66–3.12 Å. All Ta–Fe bond lengths are 2.66 Å. In the second Ta site, Ta is bonded in a 8-coordinate geometry to eight Ta and six equivalent Fe atoms. There are a spread of Ta–Ta bond distances ranging from 2.76–3.11 Å. All Ta–Fe bond lengths are 2.68 Å. In the third Ta site, Ta is bonded in a 9-coordinate geometry to seven Ta and nine equivalent Fe atoms. There are three shorter (2.84 Å) and three longer (2.91 Å) Ta–Ta bond lengths. There are three shorter (2.83 Å) and six longer (2.99 Å) Ta–Fe bond lengths. In the fourth Ta site, Ta is bonded in a 12-coordinate geometry to four Ta and twelve Fe atoms. All Ta–Ta bond lengths are 2.91 Å. There are a spread of Ta–Fe bond distances ranging from 2.77–2.93 Å. In the fifth Ta site, Ta is bonded in a 6-coordinate geometry to nine Ta and six Fe atoms. All Ta–Ta bond lengths are 2.81 Å. There are three shorter (2.79 Å) and three longer (2.83 Å) Ta–Fe bond lengths. In the sixth Ta site, Ta is bonded in a 6-coordinate geometry to nine Ta and six Fe atoms. There are three shorter (2.78 Å) and three longer (2.82 Å) Ta–Fe bond lengths. In the seventh Ta site, Ta is bonded to six equivalent Ta and six equivalent Fe atoms to form distorted TaTa6Fe6 cuboctahedra that share corners with twelve equivalent FeTa8Fe4 cuboctahedra, edges with six equivalent TaTa6Fe6 cuboctahedra, and faces with eighteen equivalent FeTa8Fe4 cuboctahedra. All Ta–Fe bond lengths are 2.55 Å. There are three inequivalent Fe sites. In the first Fe site, Fe is bonded to seven Ta and five Fe atoms to form FeTa7Fe5 cuboctahedra that share corners with fifteen FeTa7Fe5 cuboctahedra, edges with five FeTa8Fe4 cuboctahedra, and faces with thirteen FeTa7Fe5 cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.42–2.46 Å. In the second Fe site, Fe is bonded to eight Ta and four equivalent Fe atoms to form distorted FeTa8Fe4 cuboctahedra that share corners with two equivalent TaTa6Fe6 cuboctahedra, corners with thirteen FeTa7Fe5 cuboctahedra, edges with five FeTa8Fe4 cuboctahedra, faces with three equivalent TaTa6Fe6 cuboctahedra, and faces with ten equivalent FeTa8Fe4 cuboctahedra. There are two shorter (2.38 Å) and two longer (2.49 Å) Fe–Fe bond lengths. In the third Fe site, Fe is bonded to six equivalent Ta and six equivalent Fe atoms to form FeTa6Fe6 cuboctahedra that share corners with twelve equivalent FeTa7Fe5 cuboctahedra, edges with six equivalent FeTa6Fe6 cuboctahedra, and faces with eighteen equivalent FeTa7Fe5 cuboctahedra.

36 MATERIALS SCIENCE↗

Dose-Rate Effects of Protons and Light Ions for DNA Damage Induction, Survival and Transformation in Apparently Normal Primary Human Fibroblasts

In this work, we report on effects of low-dose exposures of accelerated protons delivered at high-dose rate (HDR) or a simulated solar-particle event (SPE) like low-dose rate (LDR) on immediate DNA damage induction and processing, survival and in vitro transformation of low passage NFF28 apparently normal primary human fibroblasts. Cultures were exposed to 50, 100 and 1,000 MeV monoenergetic protons in the Bragg entrance/plateau region and cesium-137 γ rays at 20 Gy/h (HDR) or 1 Gy/h (LDR). DNA double-strand breaks (DSB) and clustered DNA damages (containing oxypurines and abasic sites) were measured using transverse alternating gel electrophoresis (TAFE) and immunocytochemical detection/scoring of colocalized γ-H2AX pS139/53BP1 foci, with their induction being linear energy transfer (LET) dependent and dose-rate sparing observed for the different damage classes. Relative biological effectiveness (RBE) values for cell survival after proton irradiation at both dose-rates ranged from 0.61–0.73. Transformation RBE values were dose-rate dependent, ranging from ~1.8–3.1 and ~0.6–1.0 at low doses (≤30 cGy) for HDR and LDR irradiations, respectively. However peak transformation frequencies were significantly higher (1.3–7.3-fold) for higher doses of 0.5–1 Gy delivered at SPE-like LDR. Cell survival and transformation frequencies measured after low-dose 500 MeV/n He-4, 290 MeV/n C-12 and 600 MeV/n Si-28 ion irradiations also showed an inverse dose-rate effect for transformation at SPE-like LDR. This work demonstrates the existence of inverse dose-rate effects for proton and light-ion-induced postirradiation cell survival and in vitro transformation for space mission-relevant doses and dose rates.

59 BASIC BIOLOGICAL SCIENCES↗