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At least 1,009 records · Page 56

Materials Data on Y3(SiNi)2 by Materials Project

Y3(NiSi)2 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 7-coordinate geometry to two equivalent Ni and five equivalent Si atoms. Both Y–Ni bond lengths are 2.79 Å. There are four shorter (2.98 Å) and one longer (3.08 Å) Y–Si bond lengths. In the second Y site, Y is bonded to eight equivalent Ni and four equivalent Si atoms to form a mixture of edge and face-sharing YSi4Ni8 cuboctahedra. All Y–Ni bond lengths are 3.12 Å. All Y–Si bond lengths are 3.12 Å. Ni is bonded in a 9-coordinate geometry to six Y, one Ni, and two equivalent Si atoms. The Ni–Ni bond length is 2.36 Å. Both Ni–Si bond lengths are 2.34 Å. Si is bonded in a 9-coordinate geometry to seven Y and two equivalent Ni atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y3MnB7 by Materials Project

Y3MnB7 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 11-coordinate geometry to eleven B atoms. There are a spread of Y–B bond distances ranging from 2.61–2.73 Å. In the second Y site, Y is bonded in a 12-coordinate geometry to ten B atoms. There are a spread of Y–B bond distances ranging from 2.61–2.68 Å. Mn is bonded in a 10-coordinate geometry to ten B atoms. There are a spread of Mn–B bond distances ranging from 2.27–2.29 Å. There are four inequivalent B sites. In the first B site, B is bonded in a 9-coordinate geometry to six Y and three B atoms. There is one shorter (1.90 Å) and two longer (1.96 Å) B–B bond length. In the second B site, B is bonded in a 9-coordinate geometry to four Y, two equivalent Mn, and three B atoms. There is one shorter (1.78 Å) and one longer (1.81 Å) B–B bond length. In the third B site, B is bonded in a 9-coordinate geometry to four equivalent Y, two equivalent Mn, and three B atoms. There is one shorter (1.72 Å) and one longer (1.96 Å) B–B bond length. In the fourth B site, B is bonded in a 8-coordinate geometry to four equivalent Y, two equivalent Mn, and two equivalent B atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y3Pd2 by Materials Project

Y3Pd2 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. there are three inequivalent Y sites. In the first Y site, Y is bonded in an octahedral geometry to six equivalent Pd atoms. All Y–Pd bond lengths are 3.01 Å. In the second Y site, Y is bonded in a 6-coordinate geometry to six equivalent Pd atoms. There are three shorter (2.90 Å) and three longer (3.10 Å) Y–Pd bond lengths. In the third Y site, Y is bonded in a 5-coordinate geometry to five equivalent Pd atoms. There are a spread of Y–Pd bond distances ranging from 2.91–3.33 Å. Pd is bonded in a 9-coordinate geometry to eight Y and one Pd atom. The Pd–Pd bond length is 2.88 Å.

36 MATERIALS SCIENCE↗

Materials Data on Y3(CuGe)4 by Materials Project

Y3(CuGe)4 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded to six Ge atoms to form distorted edge-sharing YGe6 octahedra. There are four shorter (2.95 Å) and two longer (3.02 Å) Y–Ge bond lengths. In the second Y site, Y is bonded in a 12-coordinate geometry to six equivalent Cu and six Ge atoms. There are four shorter (3.01 Å) and two longer (3.08 Å) Y–Cu bond lengths. There are two shorter (3.02 Å) and four longer (3.06 Å) Y–Ge bond lengths. Cu is bonded in a 12-coordinate geometry to three equivalent Y, one Cu, and four Ge atoms. The Cu–Cu bond length is 2.53 Å. There are a spread of Cu–Ge bond distances ranging from 2.50–2.61 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to three Y and six equivalent Cu atoms. In the second Ge site, Ge is bonded in a 9-coordinate geometry to six Y, two equivalent Cu, and one Ge atom. The Ge–Ge bond length is 2.55 Å.

36 MATERIALS SCIENCE↗

Materials Data on AcY3 by Materials Project

AcY3 is beta Cu3Ti-like structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Ac is bonded to twelve Y atoms to form AcY12 cuboctahedra that share corners with four equivalent AcY12 cuboctahedra, corners with eight equivalent YAc4Y8 cuboctahedra, edges with eight equivalent AcY12 cuboctahedra, edges with sixteen equivalent YAc4Y8 cuboctahedra, faces with four equivalent AcY12 cuboctahedra, and faces with fourteen YAc4Y8 cuboctahedra. There are eight shorter (3.69 Å) and four longer (3.70 Å) Ac–Y bond lengths. There are two inequivalent Y sites. In the first Y site, Y is bonded to four equivalent Ac and eight Y atoms to form YAc4Y8 cuboctahedra that share corners with twelve equivalent YAc4Y8 cuboctahedra, edges with eight equivalent AcY12 cuboctahedra, edges with sixteen YAc4Y8 cuboctahedra, faces with four equivalent AcY12 cuboctahedra, and faces with fourteen YAc4Y8 cuboctahedra. There are four shorter (3.69 Å) and four longer (3.70 Å) Y–Y bond lengths. In the second Y site, Y is bonded to four equivalent Ac and eight equivalent Y atoms to form YAc4Y8 cuboctahedra that share corners with four equivalent YAc4Y8 cuboctahedra, corners with eight equivalent AcY12 cuboctahedra, edges with twenty-four YAc4Y8 cuboctahedra, faces with six equivalent AcY12 cuboctahedra, and faces with twelve YAc4Y8 cuboctahedra.

36 MATERIALS SCIENCE↗

Materials Data on Y3In5 by Materials Project

Y3In5 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 9-coordinate geometry to nine In atoms. There are a spread of Y–In bond distances ranging from 3.21–3.69 Å. In the second Y site, Y is bonded in a 10-coordinate geometry to ten In atoms. There are a spread of Y–In bond distances ranging from 3.30–3.69 Å. There are four inequivalent In sites. In the first In site, In is bonded in a 3-coordinate geometry to six Y and two equivalent In atoms. Both In–In bond lengths are 3.11 Å. In the second In site, In is bonded in a 5-coordinate geometry to five Y and three In atoms. There are one shorter (3.27 Å) and two longer (3.35 Å) In–In bond lengths. In the third In site, In is bonded in a 9-coordinate geometry to six Y and three In atoms. Both In–In bond lengths are 3.18 Å. In the fourth In site, In is bonded in a 10-coordinate geometry to six Y and four In atoms. The In–In bond length is 3.14 Å.

36 MATERIALS SCIENCE↗

Materials Data on Y3(CuSn)4 by Materials Project

Y3Cu4Sn4 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded to six Sn atoms to form distorted edge-sharing YSn6 octahedra. There are four shorter (3.05 Å) and two longer (3.18 Å) Y–Sn bond lengths. In the second Y site, Y is bonded in a 12-coordinate geometry to six equivalent Cu and six Sn atoms. All Y–Cu bond lengths are 3.19 Å. There are two shorter (3.19 Å) and four longer (3.28 Å) Y–Sn bond lengths. Cu is bonded in a 8-coordinate geometry to three equivalent Y, one Cu, and four Sn atoms. The Cu–Cu bond length is 2.62 Å. There are a spread of Cu–Sn bond distances ranging from 2.64–2.73 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 9-coordinate geometry to three Y and six equivalent Cu atoms. In the second Sn site, Sn is bonded in a 9-coordinate geometry to six Y, two equivalent Cu, and one Sn atom. The Sn–Sn bond length is 2.84 Å.

36 MATERIALS SCIENCE↗

ML-based Micro-CT SOFC Microstructure Models (from Kent 2026 Microstructural Augmentation paper)

Overview -------------------------- This repository contains datasets from the manuscript **"Enhanced Generalizability to Deep-Learning Quantification of 3D Microstructural Characteristics through Microstructurally Aware Augmentation of Scarce Data"** (*William F. Kent, Rochan Bajpai, Rachel C. Kurchin, William K. Epting, Harry W. Abernathy, Paul A. Salvador. Submitted 2026*). The methods are also described in the dissertation **Data Intensive Analysis of Solid Oxide Cell Microstructures** (*Doctoral dissertation, Carnegie Mellon University, 2025*). The datasets here are trained convolutional neural network (CNN) models for predicting key microstructural properties of solid oxide cell (SOC) electrodes from low-res, 2-channel 3D images, as well as some helpful code. The parameters for input images are provided in the paper. Sample data is provided in the file `Combined_anode_aug_dual_1k_examples` - that particular data was used to train `anode_all_aug.pth` and will work most accurately with that model. Please familiarize yourself with all caveats on accuracy and applicability, as detailed in the associated paper. Usage -------------------------- The basic usage is as follows, assuming `model_fn` is the path to the .pth file, and `X` is 2-channel input image(s) of the proper dimensions (either one image of shape `[2,12,24,24]`, or a batch of N input images of shape `[N,2,12,24,24]`): from CNN_inferencer import load_model_for_inference model = load_model_for_inference(model_fn) y_predicted = model(X) The model object automatically handles input scaling and output de-scaling based on the way the models were trained - in other words, pass in a 2-channel micro-CT image, and it will output microstructural property values in real units. ## Other model object attributes Note that model has useful attributes other than its forward pass model(X). * `model.output_descaler` - returns the output descaler object. Model does the de-scaling when generating inferences, but you may want to re-use this de-scaler on other values to e.g. compare predictions to ground truth from already-scaled training data. * `model.prop_names` - Gives the property names of the predicted y values, in order. Only exists if there's an output scaler as part of the model object, which there will be in the models provided here. ## Usage with sample data Here is a short script to use with the included sample data. from CNN_inferencer import display_predictions, load_model_for_inference, calculate_mape, parity_plot import h5py import numpy as np model_fn = 'anode_all_aug.pth' data_fn = 'Combined_anode_aug_dual_1k_examples.h5' N_samples = 200 figure_outdir = '.' model = load_model_for_inference(model_fn) with h5py.File(data_fn,'r') as f: XX = f['X'] #These are the 2-channel 3D images yy = f['y'] #These are the ground-truth microstructural properties, but they have been scaled for training - need to de-scale below N = XX.shape[0] #How many images total in the input data file #Run inferences on N_samples random samples from XX. #Run in a batch, much more efficient than one at a time. ii = np.random.choice(N,N_samples,replace=False) ii.sort() y_pred = model(XX[ii]) #Get the original/true (but normalized/scaled) values from the training dataset... #Because they were normalized, they are not in real units yet. So let's also de-scale them using model.output_scaler. y_true = model.output_scaler.transform(yy[ii]) #Let's display actual values for just 5 random ones for i in np.random.choice(N_samples,5,replace=False): display_predictions(y_true[i], y_pred[i], model.prop_names) #Make parity plots for each property (ground truth vs predicted values) #Also label each plot with the mean abs. percent error (MAPE) of the predicted values for i,key in enumerate(model.prop_names): mape = calculate_mape(y_true[:,i], y_pred[:,i]) parity_plot(y_true[:,i], y_pred[:,i], figure_outdir, key, extra_title=f' ({mape:.2f}% MAPE)')

3D microstructure↗

Antifoam Development for Eliminating Flammability Hazards and Decreasing Cycle Time in the Defense Waste Processing Facility

The Savannah River National Laboratory (SRNL) was requested to develop a new antifoam control method for the Defense Waste Processing Facility’s (DWPF) Chemical Process Cell (CPC). SRNL completed testing of both chemical and nonchemical foam controls. The nonchemical foam controls were either ineffective (or worse, created more foam) or impractical (a water spray can control foam, but excessive water is needed). As a result, the focus of this study was on finding a superwetter or commercial antifoam for controlling foam. Thirty potential antifoams were tested as part of this study. A series of tests were developed to help screen out ineffective alternatives including: 1. Spreading testing of superspreaders, 2. Foam column testing with physical simulants, 3. Boiling testing with physical and chemical simulants, 4. Days-only Sludge Receipt and Adjustment Tank (SRAT) process simulations with sludge (containing noble metals and mercury), Precipitate Reactor Feed Tank (PRFT), and Slurry Mix Evaporator Feed Tank (SEFT) simulants in the RC1 Reaction Calorimeter (purchased for antifoam testing), and 5. Around-the-clock SRAT and Slurry Mix Evaporator (SME) process simulations with sludge(containing noble metals and mercury), PRFT, and SEFT simulants in the RC1 Reaction Calorimeter. Evonik Surfynol® MD20, a commercially available defoamer, was relatively effective in controlling foam, while remaining chemically stable in SRAT and SME processing across the pH range of 4 to 13. No degradation products were detected in the offgas, in the condensate or in the SRAT and SME products. In nitric-glycolic acid flowsheet testing, 250 mg/kg Evonik Surfynol® MD20 was needed for foam control compared to 1,625 mg/kg for Antifoam 747, DWPF’s current antifoam. In nitric-formic acid flowsheet testing, 1,125 mg/kg of Evonik Surfynol® MD20 was needed to control foam throughout the SRAT and SME cycles. The commercially available superspreader Momentive™ Y-17112 was even more effective than Evonik Surfynol® MD20 as both a defoamer and an antifoam. Not only was the foam destroyed upon addition but also was less persistent between additions. It was the most effective antifoam in testing using both the nitric-glycolic acid flowsheet and the nitric-formic acid flowsheet. In nitric-glycolic acid flowsheet testing, only 100 mg/kg Momentive™ Y-17112 was needed to control foam throughout the SRAT and SME cycles. In nitric-formic acid flowsheet testing, 300 mg/kg Momentive™ Y-17112 was needed to control foam throughout the SRAT and SME cycles. Momentive™ Y-17112 is also resistant to hydrolysis as demonstrated by its chemical stability in SRAT and SME processing across the pH range of 4 to 13 and lack of degradation products in offgas or condensate. Both candidates were effective as potential replacements for Antifoam 747, with Y-17112 demonstrating superior foam control. During nitric-glycolic flowsheet testing 50% less antifoam was needed when using Momentive™ Y-17112 compared to MD20. During nitric-formic flowsheet testing 75% less antifoam was needed when using Momentive™ Y-17112 compared to MD20. Foam remediated with Momentive™ Y-17112 was less persistent throughout testing. In addition, no degradation products were detected in the offgas, in the condensate or in the SRAT and SME products. Based on this testing, Momentive™ Y-17112 is clearly superior to Evonik Surfynol® MD20 and Antifoam 747, especially for the nitric-formic acid flowsheet processing; it is recommended that Momentive™ Y-17112 replace Antifoam 747 in DWPF. An antifoam addition strategy is recommended for both the nitric-glycolic acid flowsheet and the nitric-formic acid flowsheet. Implementation of Momentive™ Y-17112 is expected to decrease SRAT and SME boiling times by up to 50%, eliminate the issues resulting from Antifoam 747 degradation products, and minimize foamovers. To validate the effectiveness of these defoaming agents, SRNL recommends irradiation of a SRAT or SME product simulant containing fresh antifoam. The goal of this testing is to determine whether the irradiation causes decomposition of the antifoam that would make it less effective or produce new species in the offgas or slurry. This testing began in April 2020. An evaluation should be completed to determine the thermolytic hydrogen and methane generation rate in downstream equipment, including the High-Level Waste evaporators.

12 MANAGEMENT OF RADIOACTIVE AND NON-RADIOACTIVE W↗

Estrategias de agua caliente para edificios comerciales: Una guia breve

Las calderas comerciales utilizan gas combustible o petroleo, y a veces electricidad, para producir agua caliente o vapor que se distribuye en un edificio para calefaccion de espacios y/o agua caliente sanitaria. Las calderas se encuentran en edificios de todos los tamanos, desde viviendas residenciales hasta grandes complejos comerciales y, en general, las calderas se vuelven menos eficientes y confiables con el tiempo. La vida util media de una caldera de gas es de 24 a 35 anos1 y, aunque la caldera continue funcionando, se debe planificar su reemplazo alrededor de los 15 a 20 anos de antiguedad o cuando aumentan las necesidades de mantenimiento. La lista de opciones de equipo para reemplazar calderas a gas esta creciendo, especialmente en lo que respecta a bombas de calor. Es fundamental evaluar las opciones para identificar la mejor solucion antes de su instalacion, antes de que sea necesario un reemplazo urgente. En muchos edificios existentes, el equipo se reemplaza con poca planificacion, lo que puede resultar en una operacion ineficiente, mayores costos y mantener al edificio en un ciclo de 25 anos de alto consumo energetico y emisiones. Al planificar un nuevo sistema de agua caliente, se deben considerar las emisiones de carbono, el consumo de energia, los costos y los cambios en las demandas del edificio para lograr un sistema optimo. Un enfoque colaborativo, integral e innovador puede resultar en un sistema mas limpio, energeticamente eficiente y rentable que cumpla con las necesidades de su instalacion y favorezca la disminucion de emisiones en el lugar. Este documento informativo asiste a propietarios y administradores de edificios en la planificacion del reemplazo de calderas, comprendiendo las opciones y encontrando las soluciones mas adecuadas para su situacion.

caldera↗

Materials Data on YCo3H2 by Materials Project

YCo3H2 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 9-coordinate geometry to nine equivalent H atoms. There are three shorter (2.42 Å) and six longer (2.48 Å) Y–H bond lengths. In the second Y site, Y is bonded in a 6-coordinate geometry to eighteen Co atoms. There are six shorter (2.85 Å) and twelve longer (3.16 Å) Y–Co bond lengths. There are three inequivalent Co sites. In the first Co site, Co is bonded in a single-bond geometry to two equivalent Y, two equivalent Co, and one H atom. There are one shorter (2.40 Å) and one longer (2.45 Å) Co–Co bond lengths. The Co–H bond length is 1.72 Å. In the second Co site, Co is bonded in a 12-coordinate geometry to three equivalent Y and six equivalent Co atoms. In the third Co site, Co is bonded in an octahedral geometry to six equivalent H atoms. All Co–H bond lengths are 1.65 Å. H is bonded to three equivalent Y and two Co atoms to form a mixture of distorted corner, edge, and face-sharing HY3Co2 trigonal bipyramids.

36 MATERIALS SCIENCE↗

Materials Data on YZnGe by Materials Project

YZnGe crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 12-coordinate geometry to six equivalent Zn and six equivalent Ge atoms. All Y–Zn bond lengths are 2.94 Å. All Y–Ge bond lengths are 3.26 Å. In the second Y site, Y is bonded to six equivalent Ge atoms to form distorted edge-sharing YGe6 octahedra. All Y–Ge bond lengths are 3.04 Å. Zn is bonded in a 3-coordinate geometry to three equivalent Y and three equivalent Ge atoms. All Zn–Ge bond lengths are 2.51 Å. Ge is bonded in a 6-coordinate geometry to six Y and three equivalent Zn atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y3Ge5 by Materials Project

Y3Ge5 crystallizes in the orthorhombic Fdd2 space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 8-coordinate geometry to eight Ge atoms. There are a spread of Y–Ge bond distances ranging from 2.98–3.09 Å. In the second Y site, Y is bonded in a 10-coordinate geometry to ten Ge atoms. There are a spread of Y–Ge bond distances ranging from 2.95–3.50 Å. There are three inequivalent Ge sites. In the first Ge site, Ge is bonded in a 4-coordinate geometry to five Y and two equivalent Ge atoms. There are one shorter (2.59 Å) and one longer (2.66 Å) Ge–Ge bond lengths. In the second Ge site, Ge is bonded in a 9-coordinate geometry to six Y and three Ge atoms. The Ge–Ge bond length is 2.60 Å. In the third Ge site, Ge is bonded in a 8-coordinate geometry to six Y and two equivalent Ge atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y3Ge4 by Materials Project

Y3Ge4 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 5-coordinate geometry to seven Ge atoms. There are a spread of Y–Ge bond distances ranging from 2.92–3.19 Å. In the second Y site, Y is bonded in a 8-coordinate geometry to eight Ge atoms. There are a spread of Y–Ge bond distances ranging from 3.00–3.11 Å. There are three inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to seven Y and two equivalent Ge atoms. Both Ge–Ge bond lengths are 2.62 Å. In the second Ge site, Ge is bonded in a 4-coordinate geometry to four equivalent Y and four equivalent Ge atoms. All Ge–Ge bond lengths are 2.87 Å. In the third Ge site, Ge is bonded in a 9-coordinate geometry to six Y and three Ge atoms.

36 MATERIALS SCIENCE↗

Materials Data on YZnSn by Materials Project

YZnSn crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded to six equivalent Sn atoms to form edge-sharing YSn6 octahedra. All Y–Sn bond lengths are 3.19 Å. In the second Y site, Y is bonded in a 12-coordinate geometry to six equivalent Zn and six equivalent Sn atoms. All Y–Zn bond lengths are 2.97 Å. All Y–Sn bond lengths are 3.41 Å. Zn is bonded in a 6-coordinate geometry to three equivalent Y and three equivalent Sn atoms. All Zn–Sn bond lengths are 2.71 Å. Sn is bonded in a 6-coordinate geometry to six Y and three equivalent Zn atoms.

36 MATERIALS SCIENCE↗

Materials Data on YCo3 by Materials Project

YCo3 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 12-coordinate geometry to twelve Co atoms. There are a spread of Y–Co bond distances ranging from 2.88–3.10 Å. In the second Y site, Y is bonded in a 6-coordinate geometry to eighteen Co atoms. There are six shorter (2.88 Å) and twelve longer (3.18 Å) Y–Co bond lengths. There are three inequivalent Co sites. In the first Co site, Co is bonded to five Y and seven Co atoms to form a mixture of edge, face, and corner-sharing CoY5Co7 cuboctahedra. There are a spread of Co–Co bond distances ranging from 2.42–2.54 Å. In the second Co site, Co is bonded to six equivalent Y and six equivalent Co atoms to form CoY6Co6 cuboctahedra that share corners with twelve equivalent CoY5Co7 cuboctahedra, edges with six equivalent CoY6Co6 cuboctahedra, and faces with eighteen equivalent CoY5Co7 cuboctahedra. In the third Co site, Co is bonded in a 12-coordinate geometry to three equivalent Y and six equivalent Co atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y2Cl3 by Materials Project

Y2Cl3 crystallizes in the monoclinic C2/m space group. The structure is two-dimensional and consists of one Y2Cl3 sheet oriented in the (2, 0, -1) direction. there are two inequivalent Y sites. In the first Y site, Y is bonded in a pentagonal planar geometry to five Cl atoms. There are a spread of Y–Cl bond distances ranging from 2.72–2.84 Å. In the second Y site, Y is bonded in a 4-coordinate geometry to four Cl atoms. There are two shorter (2.76 Å) and two longer (2.79 Å) Y–Cl bond lengths. There are three inequivalent Cl sites. In the first Cl site, Cl is bonded in a distorted T-shaped geometry to three Y atoms. In the second Cl site, Cl is bonded in a distorted rectangular see-saw-like geometry to three Y atoms. In the third Cl site, Cl is bonded in a trigonal non-coplanar geometry to three equivalent Y atoms.

36 MATERIALS SCIENCE↗

Materials Data on YAl3Ni by Materials Project

YNiAl3 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Y is bonded in a 10-coordinate geometry to two equivalent Y, two equivalent Ni, and eleven Al atoms. Both Y–Y bond lengths are 3.65 Å. Both Y–Ni bond lengths are 3.10 Å. There are a spread of Y–Al bond distances ranging from 3.03–3.64 Å. Ni is bonded in a 9-coordinate geometry to two equivalent Y and seven Al atoms. There are a spread of Ni–Al bond distances ranging from 2.36–2.50 Å. There are three inequivalent Al sites. In the first Al site, Al is bonded in a 3-coordinate geometry to three equivalent Y, three equivalent Ni, and two equivalent Al atoms. There are one shorter (2.63 Å) and one longer (2.86 Å) Al–Al bond lengths. In the second Al site, Al is bonded in a 2-coordinate geometry to four equivalent Y, two equivalent Ni, and four equivalent Al atoms. There are two shorter (2.90 Å) and two longer (2.93 Å) Al–Al bond lengths. In the third Al site, Al is bonded in a 2-coordinate geometry to four equivalent Y, two equivalent Ni, and six Al atoms.

36 MATERIALS SCIENCE↗