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MnSn 2 and MnSn 2 –TiO 2 nanostructured anode materials for lithium-ion batteries

The high theoretical lithium storage capacity of Sn makes it an enticing anode material for Li-ion batteries (LIBs); however, its large volumetric expansion during Li–Sn alloying must be addressed. Combining Sn with metals that are electrochemically inactive to lithium leads to intermetallics that can alleviate volumetric expansion issues and still enable high capacity. Here, we present the cycling behavior of a nanostructured MnSn 2 intermetallic used in LIBs. Nanostructured MnSn 2 is synthesized by reducing Sn and Mn salts using a hot injection method. The resulting MnSn 2 is characterized by x-ray diffraction and transmission electron microscopy and then is investigated as an anode for LIBs. The MnSn 2 electrode delivers a stable capacity of 514 mAh g -1 after 100 cycles at a C/10 current rate with a Coulombic efficiency >99%. Unlike other Sn-intermetallic anodes, an activation overpotential peak near 0.9 V versus Li is present from the second lithiation and in subsequent cycles. We hypothesize that this effect is likely due to electrolyte reactions with segregated Mn from MnSn 2 . To prevent these undesirable Mn reactions with the electrolyte, a 5 nm TiO 2 protection layer is applied onto the MnSn 2 electrode surface via atomic layer deposition. The TiO 2 -coated MnSn 2 electrodes do not exhibit the activation overpotential peak. The protection layer also increases the capacity to 612 mAh g -1 after 100 cycles at a C/10 current rate with a Coulombic efficiency >99%. This higher capacity is achieved by suppressing the parasitic reaction of Mn with the electrolyte, as is supported by x-ray photoelectron spectroscopy analysis.

77 NANOSCIENCE AND NANOTECHNOLOGY↗

Magnetism and topological Hall effect in antiferromagnetic Ru 2 MnSn-based Heusler compounds

Heusler compounds and alloys based on them are of great recent interest because they exhibit a wide variety of spin structures, magnetic properties, and electron-transport phenomena. Their properties are tunable by alloying and we have investigated L2 1 -orderd compound Ru 2 MnSn and its alloys by varying the atomic Mn:Sn composition. While antiferromagnetic ordering with a Néel temperature of 361 K was observed in Ru 2 MnSn, the Mn-poor Ru 2 Mn 0.8 Sn 1.2 alloy exhibits properties of a diluted antiferromagnet in which there are localized regions of uncompensated Mn spins. Furthermore, a noncoplanar spin structure, evident from a topological Hall-effect contribution to the room-temperature Hall resistivity, is realized in Ru 2 Mn 0.8 Sn 1.2 . Finally, our combined experimental and theoretical analysis shows that in the Ru 2 Mn 0.8 Sn 1.2 alloy, the magnetic properties can be explained in terms of a noncoplanar antiferromagnetic scissor mode, which creates a small net magnetization in a magnetic field and subsequently yields a Berry curvature with a strong topological Hall effect.

36 MATERIALS SCIENCE↗

Materials Data on Ba(MnSn)2 by Materials Project

Ba(MnSn)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Ba is bonded in a 8-coordinate geometry to eight equivalent Mn and eight equivalent Sn atoms. All Ba–Mn bond lengths are 3.82 Å. All Ba–Sn bond lengths are 3.70 Å. Mn is bonded to four equivalent Ba and four equivalent Sn atoms to form a mixture of distorted edge, corner, and face-sharing MnBa4Sn4 tetrahedra. All Mn–Sn bond lengths are 2.75 Å. Sn is bonded in a 9-coordinate geometry to four equivalent Ba, four equivalent Mn, and one Sn atom. The Sn–Sn bond length is 3.18 Å.

36 MATERIALS SCIENCE↗

Materials Data on Hf(MnSn)6 by Materials Project

Hf(MnSn)6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Hf is bonded to eight Sn atoms to form distorted edge-sharing HfSn8 hexagonal bipyramids. There are two shorter (2.93 Å) and six longer (3.12 Å) Hf–Sn bond lengths. Mn is bonded in a 12-coordinate geometry to six Sn atoms. There are a spread of Mn–Sn bond distances ranging from 2.71–2.79 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 12-coordinate geometry to three equivalent Hf and six equivalent Mn atoms. In the second Sn site, Sn is bonded in a 6-coordinate geometry to six equivalent Mn atoms. In the third Sn site, Sn is bonded in a 7-coordinate geometry to one Hf and six equivalent Mn atoms.

36 MATERIALS SCIENCE↗

Materials Data on MnSn by Materials Project

MnSn is Tetraauricupride structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Mn is bonded in a body-centered cubic geometry to eight equivalent Sn atoms. All Mn–Sn bond lengths are 2.88 Å. Sn is bonded in a body-centered cubic geometry to eight equivalent Mn atoms.

36 MATERIALS SCIENCE↗

Materials Data on MnSn by Materials Project

MnSn is Zincblende, Sphalerite structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Mn is bonded to four equivalent Sn atoms to form corner-sharing MnSn4 tetrahedra. All Mn–Sn bond lengths are 2.66 Å. Sn is bonded to four equivalent Mn atoms to form corner-sharing SnMn4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on MnSn by Materials Project

MnSn is Halite, Rock Salt structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mn is bonded to six equivalent Sn atoms to form a mixture of edge and corner-sharing MnSn6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Mn–Sn bond lengths are 2.75 Å. Sn is bonded to six equivalent Mn atoms to form a mixture of edge and corner-sharing SnMn6 octahedra. The corner-sharing octahedral tilt angles are 0°.

36 MATERIALS SCIENCE↗

Materials Data on Sc(MnSn)6 by Materials Project

ScMn6Sn6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Sc is bonded to eight Sn atoms to form distorted edge-sharing ScSn8 hexagonal bipyramids. There are two shorter (2.93 Å) and six longer (3.12 Å) Sc–Sn bond lengths. Mn is bonded in a 12-coordinate geometry to six Sn atoms. There are a spread of Mn–Sn bond distances ranging from 2.72–2.80 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 7-coordinate geometry to one Sc and six equivalent Mn atoms. In the second Sn site, Sn is bonded in a 6-coordinate geometry to six equivalent Mn atoms. In the third Sn site, Sn is bonded in a 12-coordinate geometry to three equivalent Sc and six equivalent Mn atoms.

36 MATERIALS SCIENCE↗

Materials Data on Ho(MnSn)6 by Materials Project

HoMn6Sn6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Ho is bonded to eight Sn atoms to form distorted edge-sharing HoSn8 hexagonal bipyramids. There are two shorter (3.00 Å) and six longer (3.15 Å) Ho–Sn bond lengths. Mn is bonded in a 12-coordinate geometry to six Sn atoms. There are a spread of Mn–Sn bond distances ranging from 2.73–2.83 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 8-coordinate geometry to one Ho, six equivalent Mn, and one Sn atom. The Sn–Sn bond length is 3.00 Å. In the second Sn site, Sn is bonded in a 6-coordinate geometry to six equivalent Mn atoms. In the third Sn site, Sn is bonded in a 12-coordinate geometry to three equivalent Ho and six equivalent Mn atoms.

36 MATERIALS SCIENCE↗

Materials Data on Tb(MnSn)6 by Materials Project

TbMn6Sn6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Tb is bonded to eight Sn atoms to form distorted edge-sharing TbSn8 hexagonal bipyramids. There are two shorter (3.00 Å) and six longer (3.15 Å) Tb–Sn bond lengths. Mn is bonded in a 12-coordinate geometry to six Sn atoms. There are a spread of Mn–Sn bond distances ranging from 2.74–2.83 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 8-coordinate geometry to one Tb, six equivalent Mn, and one Sn atom. The Sn–Sn bond length is 3.00 Å. In the second Sn site, Sn is bonded in a 12-coordinate geometry to three equivalent Tb and six equivalent Mn atoms. In the third Sn site, Sn is bonded in a 6-coordinate geometry to six equivalent Mn atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y(MnSn)6 by Materials Project

YMn6Sn6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Y is bonded to eight Sn atoms to form distorted edge-sharing YSn8 hexagonal bipyramids. There are two shorter (3.00 Å) and six longer (3.15 Å) Y–Sn bond lengths. Mn is bonded in a 12-coordinate geometry to six Sn atoms. There are a spread of Mn–Sn bond distances ranging from 2.74–2.84 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 6-coordinate geometry to six equivalent Mn atoms. In the second Sn site, Sn is bonded in a 12-coordinate geometry to three equivalent Y and six equivalent Mn atoms. In the third Sn site, Sn is bonded in a 8-coordinate geometry to one Y, six equivalent Mn, and one Sn atom. The Sn–Sn bond length is 3.00 Å.

36 MATERIALS SCIENCE↗

Materials Data on Tm(MnSn)6 by Materials Project

TmMn6Sn6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Tm is bonded to eight Sn atoms to form distorted edge-sharing TmSn8 hexagonal bipyramids. There are two shorter (2.99 Å) and six longer (3.14 Å) Tm–Sn bond lengths. Mn is bonded in a 12-coordinate geometry to six Sn atoms. There are a spread of Mn–Sn bond distances ranging from 2.73–2.82 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 6-coordinate geometry to six equivalent Mn atoms. In the second Sn site, Sn is bonded in a 8-coordinate geometry to one Tm, six equivalent Mn, and one Sn atom. The Sn–Sn bond length is 3.01 Å. In the third Sn site, Sn is bonded in a 12-coordinate geometry to three equivalent Tm and six equivalent Mn atoms.

36 MATERIALS SCIENCE↗

Materials Data on Zr(MnSn)6 by Materials Project

ZrMn6Sn6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Zr is bonded to eight Sn atoms to form distorted edge-sharing ZrSn8 hexagonal bipyramids. There are two shorter (2.94 Å) and six longer (3.12 Å) Zr–Sn bond lengths. Mn is bonded in a 12-coordinate geometry to six Sn atoms. There are a spread of Mn–Sn bond distances ranging from 2.72–2.80 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 12-coordinate geometry to three equivalent Zr and six equivalent Mn atoms. In the second Sn site, Sn is bonded in a 6-coordinate geometry to six equivalent Mn atoms. In the third Sn site, Sn is bonded in a 7-coordinate geometry to one Zr and six equivalent Mn atoms.

36 MATERIALS SCIENCE↗

Materials Data on Dy(MnSn)6 by Materials Project

DyMn6Sn6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Dy is bonded to eight Sn atoms to form distorted edge-sharing DySn8 hexagonal bipyramids. There are two shorter (3.00 Å) and six longer (3.15 Å) Dy–Sn bond lengths. Mn is bonded in a 12-coordinate geometry to six Sn atoms. There are a spread of Mn–Sn bond distances ranging from 2.74–2.83 Å. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a 12-coordinate geometry to three equivalent Dy and six equivalent Mn atoms. In the second Sn site, Sn is bonded in a 6-coordinate geometry to six equivalent Mn atoms. In the third Sn site, Sn is bonded in a 8-coordinate geometry to one Dy, six equivalent Mn, and one Sn atom. The Sn–Sn bond length is 3.01 Å.

36 MATERIALS SCIENCE↗

Understanding magnetic phase coexistence in Ru 2 Mn 1-x Fe x Sn Heusler alloys: A neutron scattering, thermodynamic, and phenomenological analysis

The random substitutional solid solution between the antiferromagnetic (AFM) full-Heusler alloy Ru 2 MnSn and the ferromagnetic (FM) full-Heusler alloy Ru 2 FeSn provides a rare opportunity to study FM-AFM phase competition in a near-lattice-matched, cubic system, with full solubility. At intermediate x in Ru 2 Mn 1-x Fe x Sn this system displays suppressed magnetic ordering temperatures, spatially coexisting FM and AFM order, and strong coercivity enhancement, despite rigorous chemical homogeneity. Here, we construct the most detailed temperature- and x-dependent understanding of the magnetic phase competition and coexistence in this system to date, combining wide-temperature-range neutron diffraction and small-angle neutron scattering with magnetometry and specific heat measurements on thoroughly characterized polycrystals. A complete magnetic phase diagram is generated, showing FM-AFM coexistence between x ≈ 0.30 and x ≈ 0.70. Furthermore, important insight is gained from the extracted length scales for magnetic phase coexistence (25–100 nm), the relative magnetic volume fractions and ordering temperatures, and remarkable x-dependent trends in magnetic and electronic contributions to specific heat. An unusual feature in the magnetic phase diagram (an intermediate FM phase) is also shown to arise from an extrinsic effect related to a minor Ru-rich secondary phase. The established magnetic phase diagram is then discussed with the aid of phenomenological modeling, clarifying the nature of the mesoscale phase coexistence with respect to the understanding of disordered Heisenberg models.

36 MATERIALS SCIENCE↗