Engineering Papers⌕ Search

SEARCH · Engineering Papers

Results for “Mn3Ge”

Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

Materials Data on Mn3Ge by Materials Project

Mn3Ge is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Mn is bonded to eight equivalent Mn and four equivalent Ge atoms to form distorted MnMn8Ge4 cuboctahedra that share corners with twelve equivalent MnMn8Ge4 cuboctahedra, edges with eight equivalent GeMn12 cuboctahedra, edges with sixteen equivalent MnMn8Ge4 cuboctahedra, faces with four equivalent GeMn12 cuboctahedra, and faces with fourteen equivalent MnMn8Ge4 cuboctahedra. All Mn–Mn bond lengths are 2.58 Å. All Mn–Ge bond lengths are 2.58 Å. Ge is bonded to twelve equivalent Mn atoms to form GeMn12 cuboctahedra that share corners with twelve equivalent GeMn12 cuboctahedra, edges with twenty-four equivalent MnMn8Ge4 cuboctahedra, faces with six equivalent GeMn12 cuboctahedra, and faces with twelve equivalent MnMn8Ge4 cuboctahedra.

36 MATERIALS SCIENCE↗

Materials Data on Mn3Ge by Materials Project

Mn3Ge is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Mn sites. In the first Mn site, Mn is bonded to four equivalent Mn and four equivalent Ge atoms to form a mixture of distorted face, edge, and corner-sharing MnMn4Ge4 tetrahedra. All Mn–Mn bond lengths are 2.50 Å. All Mn–Ge bond lengths are 2.50 Å. In the second Mn site, Mn is bonded in a 8-coordinate geometry to eight equivalent Mn and six equivalent Ge atoms. All Mn–Ge bond lengths are 2.88 Å. Ge is bonded in a distorted body-centered cubic geometry to fourteen Mn atoms.

36 MATERIALS SCIENCE↗

Materials Data on Mn3Ge by Materials Project

Mn3Ge is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are three inequivalent Mn sites. In the first Mn site, Mn is bonded to eight Mn and four equivalent Ge atoms to form distorted MnMn8Ge4 cuboctahedra that share corners with four equivalent GeMn12 cuboctahedra, corners with fourteen MnMn8Ge4 cuboctahedra, edges with six equivalent GeMn12 cuboctahedra, edges with twelve MnMn8Ge4 cuboctahedra, faces with four equivalent GeMn12 cuboctahedra, and faces with sixteen MnMn8Ge4 cuboctahedra. There are a spread of Mn–Mn bond distances ranging from 2.51–2.67 Å. There are two shorter (2.59 Å) and two longer (2.60 Å) Mn–Ge bond lengths. In the second Mn site, Mn is bonded to eight equivalent Mn and four equivalent Ge atoms to form distorted MnMn8Ge4 cuboctahedra that share corners with four equivalent GeMn12 cuboctahedra, corners with fourteen MnMn8Ge4 cuboctahedra, edges with six equivalent GeMn12 cuboctahedra, edges with twelve equivalent MnMn8Ge4 cuboctahedra, faces with four equivalent GeMn12 cuboctahedra, and faces with sixteen MnMn8Ge4 cuboctahedra. There are two shorter (2.59 Å) and two longer (2.60 Å) Mn–Ge bond lengths. In the third Mn site, Mn is bonded to eight equivalent Mn and four equivalent Ge atoms to form distorted MnMn8Ge4 cuboctahedra that share corners with four equivalent GeMn12 cuboctahedra, corners with fourteen MnMn8Ge4 cuboctahedra, edges with six equivalent GeMn12 cuboctahedra, edges with twelve equivalent MnMn8Ge4 cuboctahedra, faces with four equivalent GeMn12 cuboctahedra, and faces with sixteen MnMn8Ge4 cuboctahedra. There are two shorter (2.59 Å) and two longer (2.60 Å) Mn–Ge bond lengths. Ge is bonded to twelve Mn atoms to form GeMn12 cuboctahedra that share corners with six equivalent GeMn12 cuboctahedra, corners with twelve MnMn8Ge4 cuboctahedra, edges with eighteen MnMn8Ge4 cuboctahedra, faces with eight equivalent GeMn12 cuboctahedra, and faces with twelve MnMn8Ge4 cuboctahedra.

36 MATERIALS SCIENCE↗

Temperature-induced anomalous magnetotransport in the Weyl semimetal Mn 3 Ge

The magnetic Weyl semimetallic state can lead to intriguing magnetotransport, such as chiral anomaly and the layered quantum Hall effect. Mn3X (X = Sn, Ge) is a noncollinear antiferromagnetic semimetal where a Weyl semimetallic state is stabilized by time-reversal symmetry breaking. Compared to the well-studied Mn3Sn, the Weyl fermion-induced magnetotransport in Mn3Ge has been merely studied. Here, we report an in-depth study on the magnetotransport in a microfabricated Mn3Ge single crystal from room temperature to 10 K. We reveal an anomalous anisotropic magnetoresistance with fourfold symmetry and a positive high-field longitudinal magnetoresistance below the critical temperature (160–170 K). The possible origin is the temperature-induced tilting of the Weyl nodes. Our study helps to understand the magnetotransport properties in the Weyl fermion system.

36 MATERIALS SCIENCE↗

Magnetism and magnetotransport in the kagome antiferromagnet Mn 3 Ge

We perform classical Monte Carlo and stochastic Landau-Lifshitz-Gilbert simulations to study the temperature-dependent magnetism of the kagome antiferromagnet Weyl metal Mn3Ge, and we find that a long-range chiral order sets in at a transition temperature well below the Neel temperature (T N ). Based on the crystalline symmetries imposed by the chiral magnetic order, we argue for the presence of multiple isoenergetic Weyl nodes (nodes that are at the same energy and with a congruent Fermi surface around them) near the chemical potential. Using the semiclassical Boltzmann equations, we show that the combined contribution to the net longitudinal magnetoconductance (LMC) and the planar Hall conductance (PHC) from tilted Weyl nodes can lead to signatures that are qualitatively distinct from that of a single pair of Weyl nodes. In particular, we show that magnetic orders with different chiralities can give rise to different periods in LMC and PHC as a function of the in-plane magnetic field direction. As a result, this is ultimately related to differences in the symmetry-imposed constraints on the Weyl nodes.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗