cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.6084/m9.figshare.13295831.v5
title: Autism Spectrum Disorder and Asperger Syndrome Question Answering Dataset 1.0

description: A dataset for question-answering used for building an informational Russian language chatbot for the inclusion of people with autism spectrum disorder and Asperger syndrome in particular, based on data from the following website: https://aspergers.ru.
DOI: 10.17188/1683862
title: Materials Data on K2PdN2(ClO2)2 by Materials Project

description: K2PdN2(O2Cl)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. K1+ is bonded in a 10-coordinate geometry to six equivalent O2- and four equivalent Cl1- atoms. There are a spread of K–O bond distances ranging from 2.92–3.09 Å. There are two shorter (3.17 Å) and two longer (3.26 Å) K–Cl bond lengths. Pd2+ is bonded in a linear geometry to two equivalent Cl1- atoms. Both Pd–Cl bond lengths are 2.33 Å. N3+ is bonded in a bent 120 degrees geometry to two equivalent O2- atoms. Both N–O bond lengths are 1.25 Å. O2- is bonded in a distorted single-bond geometry to three equivalent K1+ and one N3+ atom. Cl1- is bonded in a 1-coordinate geometry to four equivalent K1+ and one Pd2+ atom.
DOI: 10.17188/1683865
title: Materials Data on GdPO4 by Materials Project

description: GdPO4 is Zircon structured and crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional. Gd3+ is bonded in a 8-coordinate geometry to eight equivalent O2- atoms. There are four shorter (2.38 Å) and four longer (2.43 Å) Gd–O bond lengths. P5+ is bonded in a tetrahedral geometry to four equivalent O2- atoms. All P–O bond lengths are 1.56 Å. O2- is bonded in a 1-coordinate geometry to two equivalent Gd3+ and one P5+ atom.
DOI: 10.17188/1683866
title: Materials Data on DyInO3 by Materials Project

description: DyInO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Dy3+ is bonded to twelve equivalent O2- atoms to form DyO12 cuboctahedra that share corners with twelve equivalent DyO12 cuboctahedra, faces with six equivalent DyO12 cuboctahedra, and faces with eight equivalent InO6 octahedra. All Dy–O bond lengths are 2.91 Å. In3+ is bonded to six equivalent O2- atoms to form InO6 octahedra that share corners with six equivalent InO6 octahedra and faces with eight equivalent DyO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All In–O bond lengths are 2.06 Å. O2- is bonded in a distorted linear geometry to four equivalent Dy3+ and two equivalent In3+ atoms.
DOI: 10.17188/1683867
title: Materials Data on DySiPd2 by Materials Project

description: DyPd2Si crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Dy is bonded in a 11-coordinate geometry to ten equivalent Pd and three equivalent Si atoms. There are a spread of Dy–Pd bond distances ranging from 2.97–3.52 Å. There are a spread of Dy–Si bond distances ranging from 2.98–3.02 Å. Pd is bonded in a 12-coordinate geometry to five equivalent Dy, four equivalent Pd, and three equivalent Si atoms. There are a spread of Pd–Pd bond distances ranging from 2.77–3.05 Å. There are a spread of Pd–Si bond distances ranging from 2.49–2.62 Å. Si is bonded in a 9-coordinate geometry to three equivalent Dy and six equivalent Pd atoms.
DOI: 10.17188/1683868
title: Materials Data on FeCoSi by Materials Project

description: FeCoSi crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Fe2+ is bonded in a 8-coordinate geometry to two equivalent Fe2+, one Co2+, and five equivalent Si4- atoms. Both Fe–Fe bond lengths are 2.47 Å. The Fe–Co bond length is 2.49 Å. There are a spread of Fe–Si bond distances ranging from 2.41–2.54 Å. Co2+ is bonded in a 6-coordinate geometry to one Fe2+ and five equivalent Si4- atoms. There are a spread of Co–Si bond distances ranging from 2.31–2.61 Å. Si4- is bonded in a 10-coordinate geometry to five equivalent Fe2+ and five equivalent Co2+ atoms.
DOI: 10.17188/1683869
title: Materials Data on CsNb2(SiO3)8 by Materials Project

description: CsNb2(SiO3)8 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. Cs is bonded in a 10-coordinate geometry to ten O atoms. There are a spread of Cs–O bond distances ranging from 3.29–3.67 Å. Nb is bonded to six O atoms to form distorted NbO6 octahedra that share corners with five SiO4 tetrahedra. There are a spread of Nb–O bond distances ranging from 1.92–2.09 Å. There are four inequivalent Si sites. In the first Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one NbO6 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 19°. There are a spread of Si–O bond distances ranging from 1.62–1.64 Å. In the second Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with two equivalent NbO6 octahedra and corners with two SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 26–29°. There are a spread of Si–O bond distances ranging from 1.62–1.64 Å. In the third Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with two equivalent NbO6 octahedra and corners with two SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 27–34°. There is two shorter (1.63 Å) and two longer (1.64 Å) Si–O bond length. In the fourth Si site, Si is bonded to four O atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.62–1.65 Å. There are twelve inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one Cs and one Si atom. In the second O site, O is bonded in a single-bond geometry to one Nb atom. In the third O site, O is bonded in a bent 150 degrees geometry to one Nb and one Si atom. In the fourth O site, O is bonded in a distorted bent 150 degrees geometry to one Cs, one Nb, and one Si atom. In the fifth O site, O is bonded in a distorted bent 150 degrees geometry to one Cs, one Nb, and one Si atom. In the sixth O site, O is bonded in a bent 150 degrees geometry to one Cs and two Si atoms. In the seventh O site, O is bonded in a bent 150 degrees geometry to two Si atoms. In the eighth O site, O is bonded in a bent 150 degrees geometry to one Cs and two Si atoms. In the ninth O site, O is bonded in a bent 150 degrees geometry to two Si atoms. In the tenth O site, O is bonded in a bent 150 degrees geometry to two Si atoms. In the eleventh O site, O is bonded in a bent 150 degrees geometry to one Nb and one Si atom. In the twelfth O site, O is bonded in a bent 150 degrees geometry to one Nb and one Si atom.
DOI: 10.17188/1683870
title: Materials Data on In12Ga4Ir2O15 by Materials Project

description: (Ir)2InIn11Ga4O15 crystallizes in the orthorhombic Pnn2 space group. The structure is three-dimensional and consists of two indium, elemental molecules; four iridium atom molecules; and one In11Ga4O15 framework. In the In11Ga4O15 framework, there are six inequivalent In1+ sites. In the first In1+ site, In1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of In–O bond distances ranging from 2.23–2.45 Å. In the second In1+ site, In1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of In–O bond distances ranging from 2.18–2.40 Å. In the third In1+ site, In1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of In–O bond distances ranging from 2.12–2.42 Å. In the fourth In1+ site, In1+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of In–O bond distances ranging from 2.13–2.31 Å. In the fifth In1+ site, In1+ is bonded in a 3-coordinate geometry to three O2- atoms. There are one shorter (2.14 Å) and two longer (2.23 Å) In–O bond lengths. In the sixth In1+ site, In1+ is bonded in a distorted L-shaped geometry to two equivalent O2- atoms. Both In–O bond lengths are 2.97 Å. There are two inequivalent Ga3+ sites. In the first Ga3+ site, Ga3+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of Ga–O bond distances ranging from 1.86–1.94 Å. In the second Ga3+ site, Ga3+ is bonded to four O2- atoms to form distorted corner-sharing GaO4 tetrahedra. There are a spread of Ga–O bond distances ranging from 1.83–1.90 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to two equivalent Ga3+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to three In1+ and one Ga3+ atom. In the third O2- site, O2- is bonded to three In1+ and one Ga3+ atom to form corner-sharing OIn3Ga tetrahedra. In the fourth O2- site, O2- is bonded to three In1+ and one Ga3+ atom to form corner-sharing OIn3Ga tetrahedra. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to two In1+ and one Ga3+ atom. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to three In1+ and one Ga3+ atom. In the seventh O2- site, O2- is bonded in a trigonal non-coplanar geometry to three In1+ and one Ga3+ atom. In the eighth O2- site, O2- is bonded in a trigonal non-coplanar geometry to two In1+ and one Ga3+ atom.
DOI: 10.17188/1683871
title: Materials Data on LiMn3(O2F)2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1683872
title: Materials Data on ZrCdPt2 by Materials Project

description: ZrPt2Cd crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two ZrPt2Cd ribbons oriented in the (1, 0, 0) direction. Zr2+ is bonded in a linear geometry to two equivalent Pt2- atoms. Both Zr–Pt bond lengths are 2.36 Å. Pt2- is bonded in a linear geometry to one Zr2+ and one Cd2+ atom. The Pt–Cd bond length is 2.77 Å. Cd2+ is bonded in a linear geometry to two equivalent Pt2- atoms.
DOI: 10.17632/vf3wcdsrds.1
title: Supplementary Material for JAAD-D-20-03692

description: Supplementary material for JAAD-D-20-03692 Topical Timolol 0.5% Gel-Forming Solution for Erythema in Rosacea: A Quantitative, Split-Face, Randomized, and Rater-Masked Pilot Clinical Trial
DOI: 10.17188/1683873
title: Materials Data on Y3Cd by Materials Project

description: Y3Cd is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Y is bonded to eight equivalent Y and four equivalent Cd atoms to form distorted YY8Cd4 cuboctahedra that share corners with twelve equivalent YY8Cd4 cuboctahedra, edges with eight equivalent CdY12 cuboctahedra, edges with sixteen equivalent YY8Cd4 cuboctahedra, faces with four equivalent CdY12 cuboctahedra, and faces with fourteen equivalent YY8Cd4 cuboctahedra. All Y–Y bond lengths are 3.45 Å. All Y–Cd bond lengths are 3.45 Å. Cd is bonded to twelve equivalent Y atoms to form CdY12 cuboctahedra that share corners with twelve equivalent CdY12 cuboctahedra, edges with twenty-four equivalent YY8Cd4 cuboctahedra, faces with six equivalent CdY12 cuboctahedra, and faces with twelve equivalent YY8Cd4 cuboctahedra.
DOI: 10.17188/1683874
title: Materials Data on MgSi by Materials Project

description: MgSi is Magnesium tetraboride-like structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are three inequivalent Mg sites. In the first Mg site, Mg is bonded in a 7-coordinate geometry to seven Si atoms. There are a spread of Mg–Si bond distances ranging from 2.69–3.01 Å. In the second Mg site, Mg is bonded in a 6-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.71–3.17 Å. In the third Mg site, Mg is bonded in a 6-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.73–3.11 Å. There are three inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to six Mg and three equivalent Si atoms. There are a spread of Si–Si bond distances ranging from 2.49–2.67 Å. In the second Si site, Si is bonded in a 8-coordinate geometry to seven Mg and one Si atom. The Si–Si bond length is 2.40 Å. In the third Si site, Si is bonded in a 9-coordinate geometry to six Mg and three equivalent Si atoms.
DOI: 10.17632/x2nz352ffm.2
title: Code and data for 'consideration of culture is vital if we are to achieve the sustainable development goals'

description: This dataset provides the data, code, and Table S4-S6 for the manuscript titled 'consideration of culture is vital if we are to achieve the sustainable development goals'.
DOI: 10.17188/1683875
title: Materials Data on Fe3(OF3)2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1683876
title: Materials Data on SrCaI4 by Materials Project

description: SrCaI4 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Sr2+ is bonded in a 8-coordinate geometry to eight I1- atoms. There are a spread of Sr–I bond distances ranging from 3.39–3.53 Å. Ca2+ is bonded in a 8-coordinate geometry to eight I1- atoms. There are a spread of Ca–I bond distances ranging from 3.28–3.45 Å. There are two inequivalent I1- sites. In the first I1- site, I1- is bonded in a 4-coordinate geometry to two equivalent Sr2+ and two equivalent Ca2+ atoms. In the second I1- site, I1- is bonded in a 4-coordinate geometry to two equivalent Sr2+ and two equivalent Ca2+ atoms.
DOI: 10.17188/1683877
title: Materials Data on MnIrN2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1683878
title: Materials Data on DyAlNi4 by Materials Project

description: DyNi4Al crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Dy is bonded in a 6-coordinate geometry to fifteen Ni and three equivalent Al atoms. There are three shorter (2.91 Å) and twelve longer (3.17 Å) Dy–Ni bond lengths. All Dy–Al bond lengths are 2.91 Å. There are two inequivalent Ni sites. In the first Ni site, Ni is bonded to three equivalent Dy, six equivalent Ni, and three equivalent Al atoms to form NiDy3Al3Ni6 cuboctahedra that share corners with nine equivalent AlDy3Ni9 cuboctahedra, corners with twelve equivalent NiDy4Al2Ni6 cuboctahedra, edges with six equivalent NiDy3Al3Ni6 cuboctahedra, faces with three equivalent AlDy3Ni9 cuboctahedra, and faces with twenty NiDy3Al3Ni6 cuboctahedra. All Ni–Ni bond lengths are 2.40 Å. All Ni–Al bond lengths are 2.91 Å. In the second Ni site, Ni is bonded to four equivalent Dy, six Ni, and two equivalent Al atoms to form distorted NiDy4Al2Ni6 cuboctahedra that share corners with four equivalent AlDy3Ni9 cuboctahedra, corners with twenty NiDy3Al3Ni6 cuboctahedra, edges with ten equivalent NiDy4Al2Ni6 cuboctahedra, faces with six equivalent AlDy3Ni9 cuboctahedra, and faces with sixteen NiDy3Al3Ni6 cuboctahedra. There are two shorter (2.48 Å) and two longer (2.55 Å) Ni–Ni bond lengths. Both Ni–Al bond lengths are 2.43 Å. Al is bonded to three equivalent Dy and nine Ni atoms to form distorted AlDy3Ni9 cuboctahedra that share corners with twenty-one NiDy3Al3Ni6 cuboctahedra, edges with six equivalent AlDy3Ni9 cuboctahedra, faces with two equivalent AlDy3Ni9 cuboctahedra, and faces with twenty-one NiDy3Al3Ni6 cuboctahedra.
DOI: 10.17632/vrpb5xrf83.1
title: Diagnostic utility of CT for abdominal injury in the military setting: a systematic review and meta-analysis

description: PubMed, EMBASE, and Cochrane Library databases were searched. Included studies should explore the diagnostic accuracy of CT for abdominal injury in the military setting.
DOI: 10.17188/1683879
title: Materials Data on MnFe3Sb2(PO4)6 by Materials Project

description: MnFe3Sb2(PO4)6 crystallizes in the trigonal R3 space group. The structure is three-dimensional. Mn2+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.98 Å) and three longer (2.14 Å) Mn–O bond lengths. There are three inequivalent Fe+2.67+ sites. In the first Fe+2.67+ site, Fe+2.67+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.93 Å) and three longer (2.14 Å) Fe–O bond lengths. In the second Fe+2.67+ site, Fe+2.67+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.93 Å) and three longer (2.11 Å) Fe–O bond lengths. In the third Fe+2.67+ site, Fe+2.67+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.93 Å) and three longer (2.13 Å) Fe–O bond lengths. There are two inequivalent Sb4+ sites. In the first Sb4+ site, Sb4+ is bonded in a 6-coordinate geometry to six O2- atoms. There are three shorter (2.33 Å) and three longer (2.36 Å) Sb–O bond lengths. In the second Sb4+ site, Sb4+ is bonded in a distorted hexagonal planar geometry to six O2- atoms. There are three shorter (2.35 Å) and three longer (2.36 Å) Sb–O bond lengths. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one MnO6 octahedra and corners with three FeO6 octahedra. The corner-sharing octahedra tilt angles range from 28–46°. There is two shorter (1.53 Å) and two longer (1.57 Å) P–O bond length. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one MnO6 octahedra and corners with three FeO6 octahedra. The corner-sharing octahedra tilt angles range from 28–46°. There are a spread of P–O bond distances ranging from 1.52–1.58 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one Fe+2.67+ and one P5+ atom. In the second O2- site, O2- is bonded in a 1-coordinate geometry to one Fe+2.67+, one Sb4+, and one P5+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Mn2+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to one Fe+2.67+, one Sb4+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one Fe+2.67+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a 1-coordinate geometry to one Mn2+, one Sb4+, and one P5+ atom. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to one Fe+2.67+, one Sb4+, and one P5+ atom. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to one Fe+2.67+ and one P5+ atom.
DOI: 10.17188/1683880
title: Materials Data on Cd2InAgTe4 by Materials Project

description: AgCd2InTe4 is Stannite structured and crystallizes in the tetragonal I-42m space group. The structure is three-dimensional. Ag1+ is bonded to four equivalent Te2- atoms to form AgTe4 tetrahedra that share corners with four equivalent InTe4 tetrahedra and corners with eight equivalent CdTe4 tetrahedra. All Ag–Te bond lengths are 2.83 Å. Cd2+ is bonded to four equivalent Te2- atoms to form CdTe4 tetrahedra that share corners with four equivalent AgTe4 tetrahedra, corners with four equivalent CdTe4 tetrahedra, and corners with four equivalent InTe4 tetrahedra. All Cd–Te bond lengths are 2.87 Å. In3+ is bonded to four equivalent Te2- atoms to form InTe4 tetrahedra that share corners with four equivalent AgTe4 tetrahedra and corners with eight equivalent CdTe4 tetrahedra. All In–Te bond lengths are 2.85 Å. Te2- is bonded to one Ag1+, two equivalent Cd2+, and one In3+ atom to form corner-sharing TeCd2InAg tetrahedra.
DOI: 10.6084/m9.figshare.13674136
title: Supplementary Material for: Detection of Major Cardioembolic Sources in Real-World Patients with Ischemic Stroke or Transient Ischemic Attack of Undetermined Cause

description: <b><i>Background/Aim:</i></b> Current guidelines recommend transthoracic echocardiography (TTE) and ambulatory rhythm monitoring following ischemic stroke or transient ischemic attack (TIA) of undetermined cause for identifying cardioembolic sources (CES). Due to ongoing controversies about this routine strategy, we evaluated its yield in a real-world setting. <b><i>Methods:</i></b> In a tertiary medical center, we retrospectively evaluated consecutive patients with ischemic stroke or TIA of undetermined cause, who (after standard work-up) underwent TTE, ambulatory rhythm monitoring, or both. CES were classified as major if probably related to ischemic events and warranting a change of therapy. <b><i>Results:</i></b> Between January 2014 and December 2017, 674 patients had ischemic stroke or TIA of undetermined cause. Of all 484 patients (71.8%) who underwent TTE, 9 (1.9%) had a major CES. However, 7 of them had already been identified for cardiac evaluation due to new major electrocardiographic abnormalities or cardiac symptoms. Thus, only 2 patients (0.4%) truly benefitted from unselected TTE screening. Ambulatory rhythm monitoring was performed in 411 patients (61.0%) and revealed AF in 10 patients (2.4%). <b><i>Conclusion:</i></b> Detecting a major CES is essential because appropriate treatment lowers the risk of recurrent stroke. Nonetheless, in this real-world study that aimed at routine use of TTE and ambulatory rhythm monitoring in patients with ischemic stroke or TIA of undetermined cause, the prevalence of major CES was low. Most patients with major CES on TTE already had an indication for referral to a cardiologist, suggesting that major CES might also have been identified with a much more selective use of TTE.
DOI: 10.17188/1683881
title: Materials Data on CeMnSbO by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17632/6674fwhhtg.1
title: Observational and Parcel and 1D model simulation data illustrated in Silber et al. (2021)

description: Long-term observational analysis results based on NSA measurements providing P(L|T), and parcel and 1D model ensembles' output for spherical and habit-evolving ice microphysics (Figures 1-3 in Silber et al., 2021). Reference: Silber et al. (2021): Crystal-Clear Evidence of Ice Crystal Habit Modulation of Arctic Supercooled Water Occurrence.
DOI: 10.17188/1683882
title: Materials Data on AgPd3Se by Materials Project

description: AgPd3Se crystallizes in the cubic Pa-3 space group. The structure is three-dimensional. Pd is bonded in a 2-coordinate geometry to four equivalent Ag and two equivalent Se atoms. There are a spread of Pd–Ag bond distances ranging from 3.04–3.28 Å. There are one shorter (2.47 Å) and one longer (2.52 Å) Pd–Se bond lengths. Ag is bonded in a 9-coordinate geometry to twelve equivalent Pd, one Ag, and three equivalent Se atoms. The Ag–Ag bond length is 2.85 Å. All Ag–Se bond lengths are 3.14 Å. Se is bonded in a 9-coordinate geometry to six equivalent Pd and three equivalent Ag atoms.