cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.6084/m9.figshare.13656395.v1
title: Supplementary Material for: Complement Component 3 Is Required for Tissue Damage, Neutrophil Infiltration, and Ensuring NET Formation in Acute Pancreatitis

description: <b><i>Background:</i></b> Neutrophil extracellular traps (NETs) are known to play an important role in the pathophysiology of acute pancreatitis (AP). Activation of the complement cascade has been shown to occur in AP. The aim of this study was to examine whether complement component 3 is involved in the generation of NETs in AP. <b><i>Methods:</i></b> AP was induced in wild-type and C3-deficient mice by retrograde infusion of taurocholate into the pancreatic duct. Blood, lung, and pancreas tissue were collected and MPO activity was determined in lung and pancreas tissue. Histological examination of the inflamed pancreas was performed. Plasma levels of CXCL2, MMP-9, IL-6, and DNA-histone complexes as well as pancreatic levels of CXCL1 and CXCL2 were determined by use of enzyme-linked immunosorbent assay. NETs were detected in the pancreas by electron microscopy. The amount of MPO and citrullinated histone 3 in neutrophils isolated from bone marrow was examined using flow cytometry. <b><i>Results:</i></b> In C3-deficient mice, challenge with taurocholate yielded much fewer NETs in the pancreatic tissue compared with wild-type controls. Taurocholate-induced blood levels of amylase, tissue injury, and neutrophil recruitment in the pancreas were markedly reduced in the mice lacking C3. Furthermore, MPO levels in the lung, and plasma levels of IL-6, MMP-9, and CXCL2 were significantly lower in the C3-deficient mice compared to wild-type mice after the induction of AP. In vitro studies revealed that neutrophils from C3-deficient mice had normal NET-forming ability and recombinant C3a was not capable of directly inducing NETs formation in the wild-type neutrophils. <b><i>Conclusion:</i></b> C3 plays an important role in the pathophysiology of AP as it is necessary for the recruitment of neutrophils into the pancreas and ensuring NETs formation. Targeting C3 could hence be a potential strategy to ameliorate local damage as well as remote organ dysfunction in AP.
DOI: 10.17188/1188492
title: Materials Data on YMgTl by Materials Project

description: MgYTl crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Mg is bonded in a 4-coordinate geometry to four Tl atoms. There are two shorter (2.93 Å) and two longer (2.98 Å) Mg–Tl bond lengths. Y is bonded in a 5-coordinate geometry to five Tl atoms. There are four shorter (3.25 Å) and one longer (3.26 Å) Y–Tl bond lengths. There are two inequivalent Tl sites. In the first Tl site, Tl is bonded in a 9-coordinate geometry to three equivalent Mg and six equivalent Y atoms. In the second Tl site, Tl is bonded in a 9-coordinate geometry to six equivalent Mg and three equivalent Y atoms.
DOI: 10.17188/1188493
title: Materials Data on LaMgTl by Materials Project

description: MgLaTl crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Mg is bonded in a 4-coordinate geometry to four Tl atoms. There are two shorter (3.05 Å) and two longer (3.09 Å) Mg–Tl bond lengths. La is bonded in a 5-coordinate geometry to five Tl atoms. There are one shorter (3.35 Å) and four longer (3.38 Å) La–Tl bond lengths. There are two inequivalent Tl sites. In the first Tl site, Tl is bonded in a 9-coordinate geometry to three equivalent Mg and six equivalent La atoms. In the second Tl site, Tl is bonded in a distorted q6 geometry to six equivalent Mg and three equivalent La atoms.
DOI: 10.17188/1188494
title: Materials Data on SmMgTl by Materials Project

description: MgSmTl crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Mg is bonded in a 4-coordinate geometry to four Tl atoms. There are two shorter (2.97 Å) and two longer (3.01 Å) Mg–Tl bond lengths. Sm is bonded in a 5-coordinate geometry to five Tl atoms. All Sm–Tl bond lengths are 3.29 Å. There are two inequivalent Tl sites. In the first Tl site, Tl is bonded in a 9-coordinate geometry to three equivalent Mg and six equivalent Sm atoms. In the second Tl site, Tl is bonded in a 9-coordinate geometry to six equivalent Mg and three equivalent Sm atoms.
DOI: 10.17188/1188495
title: Materials Data on HoMg by Materials Project

description: MgHo is Tetraauricupride structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight equivalent Ho atoms. All Mg–Ho bond lengths are 3.27 Å. Ho is bonded in a body-centered cubic geometry to eight equivalent Mg atoms.
DOI: 10.17188/1188496
title: Materials Data on Pr2CdNi2 by Materials Project

description: Pr2Ni2Cd crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. Pr is bonded in a 6-coordinate geometry to six equivalent Ni and four equivalent Cd atoms. There are two shorter (2.93 Å) and four longer (2.98 Å) Pr–Ni bond lengths. All Pr–Cd bond lengths are 3.39 Å. Ni is bonded in a 9-coordinate geometry to six equivalent Pr, one Ni, and two equivalent Cd atoms. The Ni–Ni bond length is 2.48 Å. Both Ni–Cd bond lengths are 3.03 Å. Cd is bonded to eight equivalent Pr and four equivalent Ni atoms to form a mixture of face and corner-sharing CdPr8Ni4 cuboctahedra.
DOI: 10.17188/1188497
title: Materials Data on Nd2CdNi2 by Materials Project

description: Nd2Ni2Cd crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. Nd is bonded in a 6-coordinate geometry to six equivalent Ni and four equivalent Cd atoms. There are two shorter (2.91 Å) and four longer (2.96 Å) Nd–Ni bond lengths. All Nd–Cd bond lengths are 3.37 Å. Ni is bonded in a 9-coordinate geometry to six equivalent Nd, one Ni, and two equivalent Cd atoms. The Ni–Ni bond length is 2.48 Å. Both Ni–Cd bond lengths are 3.01 Å. Cd is bonded to eight equivalent Nd and four equivalent Ni atoms to form a mixture of corner and face-sharing CdNd8Ni4 cuboctahedra.
DOI: 10.17188/1188498
title: Materials Data on LiLa2IrO6 by Materials Project

description: La2LiIrO6 is Orthorhombic Perovskite-derived structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six equivalent IrO6 octahedra. The corner-sharing octahedra tilt angles range from 29–31°. There are a spread of Li–O bond distances ranging from 2.08–2.17 Å. La3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of La–O bond distances ranging from 2.41–2.77 Å. Ir5+ is bonded to six O2- atoms to form IrO6 octahedra that share corners with six equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 29–31°. There are a spread of Ir–O bond distances ranging from 1.99–2.01 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to one Li1+, three equivalent La3+, and one Ir5+ atom. In the second O2- site, O2- is bonded to one Li1+, two equivalent La3+, and one Ir5+ atom to form distorted corner-sharing OLiLa2Ir tetrahedra. In the third O2- site, O2- is bonded in a 5-coordinate geometry to one Li1+, three equivalent La3+, and one Ir5+ atom.
DOI: 10.17188/1188499
title: Materials Data on TbCo5 by Materials Project

description: TbCo5 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Tb is bonded in a 6-coordinate geometry to eighteen Co atoms. There are six shorter (2.85 Å) and twelve longer (3.16 Å) Tb–Co bond lengths. There are two inequivalent Co sites. In the first Co site, Co is bonded to four equivalent Tb and eight Co atoms to form a mixture of corner, edge, and face-sharing CoTb4Co8 cuboctahedra. There are four shorter (2.43 Å) and four longer (2.47 Å) Co–Co bond lengths. In the second Co site, Co is bonded in a 12-coordinate geometry to three equivalent Tb and six equivalent Co atoms.
DOI: 10.17188/1188500
title: Materials Data on Al9Ir2 by Materials Project

description: Al9Ir2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Ir is bonded in a 9-coordinate geometry to nine Al atoms. There are a spread of Ir–Al bond distances ranging from 2.47–2.61 Å. There are five inequivalent Al sites. In the first Al site, Al is bonded in a linear geometry to two equivalent Ir atoms. In the second Al site, Al is bonded in a 2-coordinate geometry to two equivalent Ir atoms. In the third Al site, Al is bonded in a 2-coordinate geometry to two equivalent Ir atoms. In the fourth Al site, Al is bonded in a distorted bent 120 degrees geometry to two equivalent Ir atoms. In the fifth Al site, Al is bonded in a distorted bent 150 degrees geometry to two equivalent Ir atoms.
DOI: 10.5281/zenodo.3755072
title: IODP Expedition 362 Color reflectance

description: Color reflectance data were measured on section halves using an integration sphere and a UV-VIS spectrophotometer mounted on the Section Half Multisensor Logger (SHMSL). Spectral counts are recorded in the range of 380 to 700 nm, covering the visible spectrum, and binned in ~2 nm bins. Spectral data are reduced from spectra and recorded in tristimulus XYZ values, CieLAB L*a*b* values, and other units.
DOI: 10.17188/1188501
title: Materials Data on Er2Al3Si2 by Materials Project

description: Er2Al3Si2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Er is bonded in a 12-coordinate geometry to six Al and five equivalent Si atoms. There are a spread of Er–Al bond distances ranging from 3.01–3.23 Å. There are a spread of Er–Si bond distances ranging from 2.86–2.99 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded in a distorted water-like geometry to four equivalent Er and two equivalent Si atoms. Both Al–Si bond lengths are 2.60 Å. In the second Al site, Al is bonded in a 12-coordinate geometry to four equivalent Er and two equivalent Si atoms. Both Al–Si bond lengths are 2.72 Å. Si is bonded in a 9-coordinate geometry to five equivalent Er, three Al, and one Si atom. The Si–Si bond length is 2.38 Å.
DOI: 10.17188/1188502
title: Materials Data on Tm2Al3Si2 by Materials Project

description: Tm2Al3Si2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Tm is bonded in a 12-coordinate geometry to six Al and five equivalent Si atoms. There are a spread of Tm–Al bond distances ranging from 3.00–3.22 Å. There are a spread of Tm–Si bond distances ranging from 2.85–2.98 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded in a distorted water-like geometry to four equivalent Tm and two equivalent Si atoms. Both Al–Si bond lengths are 2.60 Å. In the second Al site, Al is bonded in a 12-coordinate geometry to four equivalent Tm and two equivalent Si atoms. Both Al–Si bond lengths are 2.71 Å. Si is bonded in a 9-coordinate geometry to five equivalent Tm, three Al, and one Si atom. The Si–Si bond length is 2.38 Å.
DOI: 10.5281/zenodo.3755071
title: IODP Expedition 362 Color reflectance

description: Color reflectance data were measured on section halves using an integration sphere and a UV-VIS spectrophotometer mounted on the Section Half Multisensor Logger (SHMSL). Spectral counts are recorded in the range of 380 to 700 nm, covering the visible spectrum, and binned in ~2 nm bins. Spectral data are reduced from spectra and recorded in tristimulus XYZ values, CieLAB L*a*b* values, and other units.
DOI: 10.17188/1188503
title: Materials Data on CeCdNi4 by Materials Project

description: CeNi4Cd is Hexagonal Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Ce is bonded in a 12-coordinate geometry to twelve equivalent Ni and four equivalent Cd atoms. All Ce–Ni bond lengths are 2.93 Å. All Ce–Cd bond lengths are 3.06 Å. Ni is bonded to three equivalent Ce, six equivalent Ni, and three equivalent Cd atoms to form a mixture of face, edge, and corner-sharing NiCe3Cd3Ni6 cuboctahedra. There are three shorter (2.48 Å) and three longer (2.52 Å) Ni–Ni bond lengths. All Ni–Cd bond lengths are 2.93 Å. Cd is bonded in a 4-coordinate geometry to four equivalent Ce and twelve equivalent Ni atoms.
DOI: 10.17188/1188504
title: Materials Data on HoCdCu4 by Materials Project

description: HoCu4Cd is Hexagonal Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Ho is bonded in a 12-coordinate geometry to twelve equivalent Cu and four equivalent Cd atoms. All Ho–Cu bond lengths are 2.99 Å. All Ho–Cd bond lengths are 3.12 Å. Cu is bonded to three equivalent Ho, six equivalent Cu, and three equivalent Cd atoms to form a mixture of edge, corner, and face-sharing CuHo3Cd3Cu6 cuboctahedra. There are three shorter (2.53 Å) and three longer (2.56 Å) Cu–Cu bond lengths. All Cu–Cd bond lengths are 2.98 Å. Cd is bonded in a 4-coordinate geometry to four equivalent Ho and twelve equivalent Cu atoms.
DOI: 10.17188/1188505
title: Materials Data on ErCdCu4 by Materials Project

description: ErCu4Cd is Hexagonal Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Er is bonded in a 12-coordinate geometry to twelve equivalent Cu and four equivalent Cd atoms. All Er–Cu bond lengths are 2.98 Å. All Er–Cd bond lengths are 3.11 Å. Cu is bonded to three equivalent Er, six equivalent Cu, and three equivalent Cd atoms to form a mixture of corner, edge, and face-sharing CuEr3Cd3Cu6 cuboctahedra. There are three shorter (2.53 Å) and three longer (2.55 Å) Cu–Cu bond lengths. All Cu–Cd bond lengths are 2.98 Å. Cd is bonded in a 4-coordinate geometry to four equivalent Er and twelve equivalent Cu atoms.
DOI: 10.17188/1188506
title: Materials Data on YbCdCu4 by Materials Project

description: YbCdCu4 is Hexagonal Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Yb is bonded in a 12-coordinate geometry to twelve equivalent Cu and four equivalent Cd atoms. All Yb–Cu bond lengths are 2.97 Å. All Yb–Cd bond lengths are 3.10 Å. Cu is bonded to three equivalent Yb, six equivalent Cu, and three equivalent Cd atoms to form a mixture of face, edge, and corner-sharing CuYb3Cd3Cu6 cuboctahedra. There are three shorter (2.52 Å) and three longer (2.54 Å) Cu–Cu bond lengths. All Cu–Cd bond lengths are 2.97 Å. Cd is bonded in a 4-coordinate geometry to four equivalent Yb and twelve equivalent Cu atoms.
DOI: 10.17188/1188507
title: Materials Data on Sb2Te3 by Materials Project

description: Sb2Te3 is MAX Phase-derived structured and crystallizes in the trigonal R-3m space group. The structure is two-dimensional and consists of three Sb2Te3 sheets oriented in the (0, 0, 1) direction. Sb3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing SbTe6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are three shorter (3.03 Å) and three longer (3.19 Å) Sb–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to six equivalent Sb3+ atoms to form edge-sharing TeSb6 octahedra. In the second Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Sb3+ atoms.
DOI: 10.17188/1188508
title: Materials Data on BaSeO4 by Materials Project

description: BaSeO4 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Ba2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Ba–O bond distances ranging from 2.72–3.24 Å. Se6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of Se–O bond distances ranging from 1.66–1.68 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to three equivalent Ba2+ and one Se6+ atom. In the second O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Ba2+ and one Se6+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to three equivalent Ba2+ and one Se6+ atom.
DOI: 10.17188/1188509
title: Materials Data on KTbGeS4 by Materials Project

description: KTbGeS4 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. K1+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of K–S bond distances ranging from 3.25–3.68 Å. Tb3+ is bonded to seven S2- atoms to form distorted TbS7 pentagonal bipyramids that share corners with two equivalent TbS7 pentagonal bipyramids, a cornercorner with one GeS4 tetrahedra, edges with two equivalent TbS7 pentagonal bipyramids, and edges with three equivalent GeS4 tetrahedra. There are a spread of Tb–S bond distances ranging from 2.81–2.95 Å. Ge4+ is bonded to four S2- atoms to form GeS4 tetrahedra that share a cornercorner with one TbS7 pentagonal bipyramid and edges with three equivalent TbS7 pentagonal bipyramids. There are a spread of Ge–S bond distances ranging from 2.20–2.24 Å. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent K1+, two equivalent Tb3+, and one Ge4+ atom. In the second S2- site, S2- is bonded in a 5-coordinate geometry to three equivalent K1+, one Tb3+, and one Ge4+ atom. In the third S2- site, S2- is bonded in a distorted see-saw-like geometry to one K1+, two equivalent Tb3+, and one Ge4+ atom. In the fourth S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent K1+, two equivalent Tb3+, and one Ge4+ atom.
DOI: 10.17188/1188510
title: Materials Data on KPrGeSe4 by Materials Project

description: KPrGeSe4 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. K1+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of K–Se bond distances ranging from 3.45–4.00 Å. Pr3+ is bonded to seven Se2- atoms to form distorted PrSe7 pentagonal bipyramids that share corners with two equivalent PrSe7 pentagonal bipyramids, a cornercorner with one GeSe4 tetrahedra, edges with two equivalent PrSe7 pentagonal bipyramids, and edges with three equivalent GeSe4 tetrahedra. There are a spread of Pr–Se bond distances ranging from 3.03–3.17 Å. Ge4+ is bonded to four Se2- atoms to form GeSe4 tetrahedra that share a cornercorner with one PrSe7 pentagonal bipyramid and edges with three equivalent PrSe7 pentagonal bipyramids. There are a spread of Ge–Se bond distances ranging from 2.35–2.39 Å. There are four inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 5-coordinate geometry to two equivalent K1+, two equivalent Pr3+, and one Ge4+ atom. In the second Se2- site, Se2- is bonded to two equivalent K1+, two equivalent Pr3+, and one Ge4+ atom to form distorted corner-sharing SeK2Pr2Ge square pyramids. In the third Se2- site, Se2- is bonded in a 4-coordinate geometry to three equivalent K1+, one Pr3+, and one Ge4+ atom. In the fourth Se2- site, Se2- is bonded in a distorted see-saw-like geometry to one K1+, two equivalent Pr3+, and one Ge4+ atom.
DOI: 10.17188/1188520
title: Materials Data on Rb2SiS3 by Materials Project

description: Rb2SiS3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Rb–S bond distances ranging from 3.37–3.91 Å. In the second Rb1+ site, Rb1+ is bonded to seven S2- atoms to form distorted RbS7 pentagonal bipyramids that share corners with two equivalent RbS7 pentagonal bipyramids, corners with three equivalent SiS4 tetrahedra, edges with four equivalent RbS7 pentagonal bipyramids, and edges with three equivalent SiS4 tetrahedra. There are a spread of Rb–S bond distances ranging from 3.34–3.59 Å. Si4+ is bonded to four S2- atoms to form SiS4 tetrahedra that share corners with three equivalent RbS7 pentagonal bipyramids, edges with three equivalent RbS7 pentagonal bipyramids, and an edgeedge with one SiS4 tetrahedra. There are a spread of Si–S bond distances ranging from 2.09–2.22 Å. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded in a distorted L-shaped geometry to four Rb1+ and two equivalent Si4+ atoms. In the second S2- site, S2- is bonded to five Rb1+ and one Si4+ atom to form a mixture of distorted edge and corner-sharing SRb5Si octahedra. The corner-sharing octahedra tilt angles range from 4–80°. In the third S2- site, S2- is bonded to five Rb1+ and one Si4+ atom to form a mixture of distorted edge and corner-sharing SRb5Si octahedra. The corner-sharing octahedra tilt angles range from 4–80°.
DOI: 10.17188/1188521
title: Materials Data on CeAl4Ge2Au by Materials Project

description: CeAuAl4Ge2 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Ce is bonded to six equivalent Ge atoms to form CeGe6 octahedra that share corners with twelve AlGe3Au tetrahedra, edges with six equivalent CeGe6 octahedra, and edges with six equivalent AlGe3Au tetrahedra. All Ce–Ge bond lengths are 3.05 Å. Au is bonded in a body-centered cubic geometry to eight Al atoms. There are six shorter (2.59 Å) and two longer (2.63 Å) Au–Al bond lengths. There are two inequivalent Al sites. In the first Al site, Al is bonded to one Au and three equivalent Ge atoms to form AlGe3Au tetrahedra that share corners with three equivalent CeGe6 octahedra, corners with ten AlGe3Au tetrahedra, edges with three equivalent CeGe6 octahedra, and edges with three equivalent AlGeAu3 tetrahedra. The corner-sharing octahedral tilt angles are 18°. All Al–Ge bond lengths are 2.60 Å. In the second Al site, Al is bonded to three equivalent Au and one Ge atom to form distorted AlGeAu3 tetrahedra that share corners with three equivalent CeGe6 octahedra, corners with twelve AlGe3Au tetrahedra, and edges with six AlGe3Au tetrahedra. The corner-sharing octahedral tilt angles are 54°. The Al–Ge bond length is 2.64 Å. Ge is bonded to three equivalent Ce and four Al atoms to form a mixture of distorted corner and edge-sharing GeCe3Al4 pentagonal bipyramids.
DOI: 10.5281/zenodo.3755097
title: IODP Expedition 362 Thermal conductivity

description: Thermal conductivity was measured using the heated needle method in either full-space needle configuration (soft/saturated sediments) or half-space needle configuration (harder materials) of a TeKa Berlin TK-04 thermal conductivity meter. Heat is applied to the sample and then thermal equilibrium is sought. The heating and equilibration curve is reduced to derive the thermal conductivity value. Raw data are stored if a user wishes to do off-line or postexpedition reduction.
DOI: 10.17188/1188522
title: Materials Data on NdAl4Ge2Au by Materials Project

description: NdAuAl4Ge2 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Nd is bonded to six equivalent Ge atoms to form NdGe6 octahedra that share corners with twelve AlGe3Au tetrahedra, edges with six equivalent NdGe6 octahedra, and edges with six equivalent AlGe3Au tetrahedra. All Nd–Ge bond lengths are 3.07 Å. Au is bonded in a body-centered cubic geometry to eight Al atoms. There are six shorter (2.59 Å) and two longer (2.61 Å) Au–Al bond lengths. There are two inequivalent Al sites. In the first Al site, Al is bonded to one Au and three equivalent Ge atoms to form AlGe3Au tetrahedra that share corners with three equivalent NdGe6 octahedra, corners with ten AlGe3Au tetrahedra, edges with three equivalent NdGe6 octahedra, and edges with three equivalent AlGeAu3 tetrahedra. The corner-sharing octahedral tilt angles are 18°. All Al–Ge bond lengths are 2.60 Å. In the second Al site, Al is bonded to three equivalent Au and one Ge atom to form distorted AlGeAu3 tetrahedra that share corners with three equivalent NdGe6 octahedra, corners with twelve AlGe3Au tetrahedra, and edges with six AlGe3Au tetrahedra. The corner-sharing octahedral tilt angles are 54°. The Al–Ge bond length is 2.64 Å. Ge is bonded to three equivalent Nd and four Al atoms to form a mixture of distorted edge and corner-sharing GeNd3Al4 pentagonal bipyramids.