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At least 397 records · Page 22

Materials Data on HoPaRu2 by Materials Project

PaHoRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Pa–Ru bond lengths are 2.96 Å. Ho is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Ho–Ru bond lengths are 2.96 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Ho atoms.

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Materials Data on Ac3Pa by Materials Project

PaAc3 is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pa is bonded to twelve equivalent Ac atoms to form PaAc12 cuboctahedra that share corners with six equivalent PaAc12 cuboctahedra, corners with twelve equivalent AcAc8Pa4 cuboctahedra, edges with eighteen equivalent AcAc8Pa4 cuboctahedra, faces with eight equivalent PaAc12 cuboctahedra, and faces with twelve equivalent AcAc8Pa4 cuboctahedra. There are six shorter (3.77 Å) and six longer (3.82 Å) Pa–Ac bond lengths. Ac is bonded to four equivalent Pa and eight equivalent Ac atoms to form distorted AcAc8Pa4 cuboctahedra that share corners with four equivalent PaAc12 cuboctahedra, corners with fourteen equivalent AcAc8Pa4 cuboctahedra, edges with six equivalent PaAc12 cuboctahedra, edges with twelve equivalent AcAc8Pa4 cuboctahedra, faces with four equivalent PaAc12 cuboctahedra, and faces with sixteen equivalent AcAc8Pa4 cuboctahedra. There are a spread of Ac–Ac bond distances ranging from 3.70–3.95 Å.

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Materials Data on Sr3Pa by Materials Project

Sr3Pa is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Sr is bonded to eight equivalent Sr and four equivalent Pa atoms to form distorted SrSr8Pa4 cuboctahedra that share corners with twelve equivalent SrSr8Pa4 cuboctahedra, edges with eight equivalent PaSr12 cuboctahedra, edges with sixteen equivalent SrSr8Pa4 cuboctahedra, faces with four equivalent PaSr12 cuboctahedra, and faces with fourteen equivalent SrSr8Pa4 cuboctahedra. All Sr–Sr bond lengths are 3.99 Å. All Sr–Pa bond lengths are 3.99 Å. Pa is bonded to twelve equivalent Sr atoms to form PaSr12 cuboctahedra that share corners with twelve equivalent PaSr12 cuboctahedra, edges with twenty-four equivalent SrSr8Pa4 cuboctahedra, faces with six equivalent PaSr12 cuboctahedra, and faces with twelve equivalent SrSr8Pa4 cuboctahedra.

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Materials Data on PaGa3 by Materials Project

PaGa3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pa is bonded to twelve equivalent Ga atoms to form a mixture of distorted face and corner-sharing PaGa12 cuboctahedra. There are six shorter (3.03 Å) and six longer (3.14 Å) Pa–Ga bond lengths. Ga is bonded in a 10-coordinate geometry to four equivalent Pa and six equivalent Ga atoms. There are four shorter (2.80 Å) and two longer (2.82 Å) Ga–Ga bond lengths.

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Materials Data on ThPaTc2 by Materials Project

PaThTc2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Tc atoms. All Pa–Tc bond lengths are 3.04 Å. Th is bonded in a body-centered cubic geometry to eight equivalent Tc atoms. All Th–Tc bond lengths are 3.04 Å. Tc is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Th atoms.

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Materials Data on PaInNi2 by Materials Project

PaNi2In is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Ni atoms. All Pa–Ni bond lengths are 2.84 Å. Ni is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent In atoms. All Ni–In bond lengths are 2.84 Å. In is bonded in a distorted body-centered cubic geometry to eight equivalent Ni atoms.

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Materials Data on MgPaPt2 by Materials Project

MgPaPt2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight equivalent Pt atoms. All Mg–Pt bond lengths are 2.95 Å. Pa is bonded in a body-centered cubic geometry to eight equivalent Pt atoms. All Pa–Pt bond lengths are 2.95 Å. Pt is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Pa atoms.

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Materials Data on PaBiAu2 by Materials Project

PaAu2Bi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Pa–Au bond lengths are 3.13 Å. Au is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Bi atoms. All Au–Bi bond lengths are 3.13 Å. Bi is bonded in a distorted body-centered cubic geometry to eight equivalent Au atoms.

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Materials Data on PaInPd2 by Materials Project

PaPd2In is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Pd atoms. All Pa–Pd bond lengths are 2.98 Å. Pd is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent In atoms. All Pd–In bond lengths are 2.98 Å. In is bonded in a body-centered cubic geometry to eight equivalent Pd atoms.

36 MATERIALS SCIENCE↗

Materials Data on MgPaAu2 by Materials Project

MgPaAu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Mg–Au bond lengths are 3.03 Å. Pa is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Pa–Au bond lengths are 3.03 Å. Au is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Pa atoms.

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Materials Data on Nd3Pa by Materials Project

PaNd3 is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pa is bonded to twelve equivalent Nd atoms to form PaNd12 cuboctahedra that share corners with six equivalent PaNd12 cuboctahedra, corners with twelve equivalent NdNd8Pa4 cuboctahedra, edges with eighteen equivalent NdNd8Pa4 cuboctahedra, faces with eight equivalent PaNd12 cuboctahedra, and faces with twelve equivalent NdNd8Pa4 cuboctahedra. All Pa–Nd bond lengths are 3.56 Å. Nd is bonded to four equivalent Pa and eight equivalent Nd atoms to form distorted NdNd8Pa4 cuboctahedra that share corners with four equivalent PaNd12 cuboctahedra, corners with fourteen equivalent NdNd8Pa4 cuboctahedra, edges with six equivalent PaNd12 cuboctahedra, edges with twelve equivalent NdNd8Pa4 cuboctahedra, faces with four equivalent PaNd12 cuboctahedra, and faces with sixteen equivalent NdNd8Pa4 cuboctahedra. There are a spread of Nd–Nd bond distances ranging from 3.50–3.63 Å.

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Materials Data on GdPaRu2 by Materials Project

PaGdRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Pa–Ru bond lengths are 2.97 Å. Gd is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Gd–Ru bond lengths are 2.97 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Gd atoms.

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Materials Data on LuPaRe2 by Materials Project

PaLuRe2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Re atoms. All Pa–Re bond lengths are 2.96 Å. Lu is bonded in a body-centered cubic geometry to eight equivalent Re atoms. All Lu–Re bond lengths are 2.96 Å. Re is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Lu atoms.

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Materials Data on PaSnRu2 by Materials Project

PaRu2Sn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Pa–Ru bond lengths are 2.91 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Sn atoms. All Ru–Sn bond lengths are 2.91 Å. Sn is bonded in a distorted body-centered cubic geometry to eight equivalent Ru atoms.

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Materials Data on PaSiO3 by Materials Project

PaSiO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Pa is bonded to twelve equivalent O atoms to form PaO12 cuboctahedra that share corners with twelve equivalent PaO12 cuboctahedra, faces with six equivalent PaO12 cuboctahedra, and faces with eight equivalent SiO6 octahedra. All Pa–O bond lengths are 2.70 Å. Si is bonded to six equivalent O atoms to form SiO6 octahedra that share corners with six equivalent SiO6 octahedra and faces with eight equivalent PaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Si–O bond lengths are 1.91 Å. O is bonded in a distorted linear geometry to four equivalent Pa and two equivalent Si atoms.

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Materials Data on PaBe13 by Materials Project

Be13Pa crystallizes in the cubic Fm-3c space group. The structure is three-dimensional. there are two inequivalent Be sites. In the first Be site, Be is bonded in a cuboctahedral geometry to twelve equivalent Be atoms. All Be–Be bond lengths are 2.15 Å. In the second Be site, Be is bonded in a 12-coordinate geometry to ten Be and two equivalent Pa atoms. There are a spread of Be–Be bond distances ranging from 2.22–2.36 Å. Both Be–Pa bond lengths are 3.00 Å. Pa is bonded in a 1-coordinate geometry to twenty-four equivalent Be atoms.

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Investigation of the Effect of Framework Flexibility on CO 2 Adsorption in SIFSIX-3-Cu Using a Machine-Learned Force Field

Metal–organic frameworks (MOFs) offer promise as selective CO 2 sorbents, but successful MOF sorbent materials need high CO 2 binding affinity and selectivity for CO 2 over water. This work focuses on the use of machine-learned force fields (MLFFs) to model CO 2 adsorption in flexible MOFs, with a focus on SIFSIX-3-Cu, an anion-pillared MOF known for its high CO 2 affinity. A preliminary high-throughput screening of over 900 anion-pillared MOFs was performed using rigid UFF+DDEC6 force fields to predict zero-loading heats of adsorption for CO 2 and H 2 O. SIFSIX-3-Cu was selected for further computational study due to its predicted CO 2 heat of adsorption and experimental relevance. A DeePMD-based MLFF was trained to reproduce DFT (PBE+D3) energies and forces, with an iterative sampling scheme combining molecular dynamics, geometry optimization, random geometric insertion, and NVT Monte Carlo-based configuration generation to capture both attractive and repulsive regions of the potential energy surface. Flexibility of the MOF was explicitly included, contrasting with previous models that approximated the MOF as rigid. Hybrid Monte Carlo/molecular dynamics (MC/MD) simulations with the MLFF produced CO 2 adsorption isotherms in good agreement with experimental data at direct air capture (DAC) pressures (e.g., 40 Pa), in contrast to previous overestimations of CO 2 sorption by models with rigid structures. Bond and angle histogram analysis showed that MOF flexibility increased the variance of fluorine–fluorine diagonal distances at adsorption sites, resulting in a lower predicted sorption for flexible, asymmetric SIFSIX-3-Cu pore geometries compared to the rigid, symmetric DFT-optimized SIFSIX-3-Cu pore geometry. A detailed description of flexibility afforded by the MLFF resulted in an accurately predicted CO 2 uptake (0.88 mmol/g) at low pressure (40 Pa) compared to the experimentally measured value (1.24 mmol/g). In conclusion, these results underscore the importance of including framework flexibility when modeling adsorption phenomena in MOFs, particularly for low-pressure applications.

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Low-temperature selective laser sintering 3D printing of PEEK-Nylon blends: Impact of thermal post-processing on mechanical properties and thermal stability

Herein, a high-performance polymer (HPP) (polyether ether ketone, PEEK) blended with a commercial low-temperature polymer (polyamide 12, PA-12) was fabricated using a low-temperature selective laser sintering (SLS) 3D printer. Different post-processing heat treatments were implemented after fabrication to tune the thermal and mechanical properties of printed blends. The specific mechanical modulus of the blend was increased up to 79% in comparison to printed PA-12 samples with heat treatment. Additionally, the thermal resistance of the treated blends greatly exceeded the properties observed using PA-12 alone. This research proposes a methodology to fabricate and engineer HPP using desktop SLS printers through a secondary lower melting temperature material and heat treatments.

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