cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1740561
title: Materials Data on LaCeSi2 by Materials Project

description: CeLaSi2 crystallizes in the orthorhombic Pmc2_1 space group. The structure is three-dimensional. Ce is bonded in a 7-coordinate geometry to seven Si atoms. There are a spread of Ce–Si bond distances ranging from 3.02–3.17 Å. La is bonded in a 7-coordinate geometry to seven Si atoms. There are a spread of La–Si bond distances ranging from 3.04–3.20 Å. There are two inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to three equivalent Ce, four equivalent La, and two equivalent Si atoms. Both Si–Si bond lengths are 2.44 Å. In the second Si site, Si is bonded in a 9-coordinate geometry to four equivalent Ce, three equivalent La, and two equivalent Si atoms.
DOI: 10.17188/1740562
title: Materials Data on Ho8In3Co by Materials Project

description: Ho8CoIn3 crystallizes in the hexagonal P6_3mc space group. The structure is three-dimensional. there are four inequivalent Ho sites. In the first Ho site, Ho is bonded in a 3-coordinate geometry to one Co and four equivalent In atoms. The Ho–Co bond length is 2.81 Å. There are two shorter (3.25 Å) and two longer (3.79 Å) Ho–In bond lengths. In the second Ho site, Ho is bonded in a 4-coordinate geometry to one Co and four equivalent In atoms. The Ho–Co bond length is 2.81 Å. There are a spread of Ho–In bond distances ranging from 3.07–3.73 Å. In the third Ho site, Ho is bonded to one Co and three equivalent In atoms to form distorted corner-sharing HoIn3Co tetrahedra. The corner-sharing octahedra tilt angles range from 13–49°. The Ho–Co bond length is 2.70 Å. All Ho–In bond lengths are 3.21 Å. In the fourth Ho site, Ho is bonded to six equivalent In atoms to form distorted HoIn6 octahedra that share corners with six equivalent HoIn3Co tetrahedra and faces with two equivalent HoIn6 octahedra. There are three shorter (3.37 Å) and three longer (3.40 Å) Ho–In bond lengths. Co is bonded in a 7-coordinate geometry to seven Ho atoms. In is bonded in a 11-coordinate geometry to eleven Ho atoms.
DOI: 10.17188/1740563
title: Materials Data on Yb(AlC)3 by Materials Project

description: YbAl3C3 crystallizes in the hexagonal P6_3mc space group. The structure is three-dimensional. Yb3+ is bonded to six C4- atoms to form YbC6 octahedra that share corners with six AlC4 tetrahedra, edges with six equivalent YbC6 octahedra, and edges with six AlC4 tetrahedra. There are three shorter (2.61 Å) and three longer (2.65 Å) Yb–C bond lengths. There are three inequivalent Al3+ sites. In the first Al3+ site, Al3+ is bonded to four C4- atoms to form AlC4 tetrahedra that share corners with three equivalent YbC6 octahedra, corners with seven AlC4 tetrahedra, and edges with three equivalent YbC6 octahedra. The corner-sharing octahedral tilt angles are 26°. There are one shorter (2.05 Å) and three longer (2.06 Å) Al–C bond lengths. In the second Al3+ site, Al3+ is bonded to four C4- atoms to form AlC4 tetrahedra that share corners with three equivalent YbC6 octahedra, corners with seven AlC4 tetrahedra, and edges with three equivalent YbC6 octahedra. The corner-sharing octahedral tilt angles are 23°. There are one shorter (2.03 Å) and three longer (2.08 Å) Al–C bond lengths. In the third Al3+ site, Al3+ is bonded in a distorted trigonal planar geometry to four C4- atoms. There are three shorter (1.98 Å) and one longer (2.54 Å) Al–C bond lengths. There are three inequivalent C4- sites. In the first C4- site, C4- is bonded to five Al3+ atoms to form corner-sharing CAl5 trigonal bipyramids. In the second C4- site, C4- is bonded in a 3-coordinate geometry to three equivalent Yb3+ and four Al3+ atoms. In the third C4- site, C4- is bonded in a 6-coordinate geometry to three equivalent Yb3+ and three equivalent Al3+ atoms.
DOI: 10.17188/1740564
title: Materials Data on FeOF 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: 10.17188/1740565
title: Materials Data on Li3TiV3O8 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: 10.17188/1740566
title: Materials Data on FeSe by Materials Project

description: FeSe crystallizes in the orthorhombic Cmme space group. The structure is one-dimensional and consists of two FeSe ribbons oriented in the (0, 1, 0) direction. Fe2+ is bonded in a distorted linear geometry to two equivalent Se2- atoms. Both Fe–Se bond lengths are 2.28 Å. Se2- is bonded in a 2-coordinate geometry to two equivalent Fe2+ atoms.
DOI: 10.17188/1740567
title: Materials Data on Ba6Nd2Y(MoO6)3 by Materials Project

description: Ba6Nd2Y(MoO6)3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form distorted BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six BaO12 cuboctahedra, a faceface with one YO6 octahedra, faces with three equivalent NdO6 octahedra, and faces with four MoO6 octahedra. There are a spread of Ba–O bond distances ranging from 2.83–3.29 Å. In the second Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form distorted BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six BaO12 cuboctahedra, faces with two equivalent NdO6 octahedra, faces with two equivalent YO6 octahedra, and faces with four MoO6 octahedra. There are a spread of Ba–O bond distances ranging from 2.87–3.27 Å. Nd3+ is bonded to six O2- atoms to form NdO6 octahedra that share corners with six MoO6 octahedra and faces with eight BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–16°. There are a spread of Nd–O bond distances ranging from 2.30–2.37 Å. Y3+ is bonded to six O2- atoms to form YO6 octahedra that share corners with six MoO6 octahedra and faces with eight BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–14°. There are a spread of Y–O bond distances ranging from 2.26–2.33 Å. There are two inequivalent Mo5+ sites. In the first Mo5+ site, Mo5+ is bonded to six O2- atoms to form MoO6 octahedra that share corners with two equivalent YO6 octahedra, corners with four equivalent NdO6 octahedra, and faces with eight BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–16°. There are a spread of Mo–O bond distances ranging from 2.00–2.03 Å. In the second Mo5+ site, Mo5+ is bonded to six O2- atoms to form MoO6 octahedra that share corners with two equivalent YO6 octahedra, corners with four equivalent NdO6 octahedra, and faces with eight BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–16°. There are a spread of Mo–O bond distances ranging from 1.98–2.04 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to four Ba2+, one Nd3+, and one Mo5+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to four Ba2+, one Nd3+, and one Mo5+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to four equivalent Ba2+, one Nd3+, and one Mo5+ atom. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to four Ba2+, one Y3+, and one Mo5+ atom. In the fifth O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Nd3+, and one Mo5+ atom. In the sixth O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Y3+, and one Mo5+ atom. In the seventh O2- site, O2- is bonded in a 2-coordinate geometry to four equivalent Ba2+, one Nd3+, and one Mo5+ atom. In the eighth O2- site, O2- is bonded in a 2-coordinate geometry to four Ba2+, one Y3+, and one Mo5+ atom.
DOI: 10.17188/1740568
title: Materials Data on La2CuSi3 by Materials Project

description: La2CuSi3 is hexagonal omega structure-derived structured and crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. La is bonded to three equivalent Cu and nine Si atoms to form a mixture of edge and face-sharing LaCu3Si9 cuboctahedra. All La–Cu bond lengths are 3.21 Å. There are three shorter (3.21 Å) and six longer (3.24 Å) La–Si bond lengths. Cu is bonded in a 9-coordinate geometry to six equivalent La and three equivalent Si atoms. All Cu–Si bond lengths are 2.40 Å. There are three inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to six equivalent La and three equivalent Si atoms. All Si–Si bond lengths are 2.40 Å. In the second Si site, Si is bonded in a 9-coordinate geometry to six equivalent La and three equivalent Cu atoms. In the third Si site, Si is bonded in a 9-coordinate geometry to six equivalent La and three equivalent Si atoms.
DOI: 10.17188/1740569
title: Materials Data on Li2Mn(CoO3)2 by Materials Project

description: Li2Mn(CoO3)2 crystallizes in the orthorhombic Cmce space group. The structure is three-dimensional. Li1+ is bonded in a distorted rectangular see-saw-like geometry to four equivalent O2- atoms. There are two shorter (2.06 Å) and two longer (2.08 Å) Li–O bond lengths. Mn2+ is bonded to six O2- atoms to form MnO6 octahedra that share edges with six equivalent CoO6 octahedra. There is two shorter (1.93 Å) and four longer (1.97 Å) Mn–O bond length. Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share edges with three equivalent MnO6 octahedra and edges with three equivalent CoO6 octahedra. There are a spread of Co–O bond distances ranging from 1.96–2.10 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one Mn2+ and two equivalent Co4+ atoms. In the second O2- site, O2- is bonded to two equivalent Li1+, one Mn2+, and two equivalent Co4+ atoms to form a mixture of distorted edge and corner-sharing OLi2MnCo2 square pyramids.
DOI: 10.17188/1740570
title: Materials Data on Y3Ge13Rh4 by Materials Project

description: Y3Rh4Ge13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Y is bonded in a 8-coordinate geometry to four equivalent Rh and twelve equivalent Ge atoms. All Y–Rh bond lengths are 3.19 Å. There are eight shorter (3.13 Å) and four longer (3.24 Å) Y–Ge bond lengths. Rh is bonded in a 6-coordinate geometry to three equivalent Y and six equivalent Ge atoms. All Rh–Ge bond lengths are 2.50 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 2-coordinate geometry to three equivalent Y, two equivalent Rh, and one Ge atom. The Ge–Ge bond length is 3.10 Å. In the second Ge site, Ge is bonded in a cuboctahedral geometry to twelve equivalent Ge atoms.
DOI: 10.17188/1740571
title: Materials Data on Li5Mn2CoO8 by Materials Project

description: Li5Mn2CoO8 is Caswellsilverite-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share a cornercorner with one CoO6 octahedra, corners with two equivalent LiO6 octahedra, corners with three equivalent MnO6 octahedra, edges with three equivalent MnO6 octahedra, and edges with nine LiO6 octahedra. The corner-sharing octahedra tilt angles range from 0–12°. There are a spread of Li–O bond distances ranging from 2.01–2.26 Å. In the second Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share a cornercorner with one LiO6 octahedra, corners with two equivalent CoO6 octahedra, corners with three equivalent MnO6 octahedra, edges with three equivalent MnO6 octahedra, edges with three equivalent CoO6 octahedra, and edges with six LiO6 octahedra. The corner-sharing octahedra tilt angles range from 6–13°. There are a spread of Li–O bond distances ranging from 2.02–2.25 Å. In the third Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six LiO6 octahedra, edges with four equivalent MnO6 octahedra, and edges with eight LiO6 octahedra. The corner-sharing octahedra tilt angles range from 11–13°. There are four shorter (2.09 Å) and two longer (2.10 Å) Li–O bond lengths. Mn+4.50+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six LiO6 octahedra, edges with two equivalent MnO6 octahedra, edges with two equivalent CoO6 octahedra, and edges with eight LiO6 octahedra. The corner-sharing octahedra tilt angles range from 0–12°. There are a spread of Mn–O bond distances ranging from 1.81–2.13 Å. Co2+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with six LiO6 octahedra, edges with two equivalent CoO6 octahedra, edges with four equivalent MnO6 octahedra, and edges with six equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 4–8°. There are four shorter (1.94 Å) and two longer (2.11 Å) Co–O bond lengths. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to five Li1+ and one Mn+4.50+ atom to form a mixture of edge and corner-sharing OLi5Mn octahedra. The corner-sharing octahedra tilt angles range from 0–13°. In the second O2- site, O2- is bonded to four Li1+ and two equivalent Mn+4.50+ atoms to form a mixture of edge and corner-sharing OLi4Mn2 octahedra. The corner-sharing octahedra tilt angles range from 0–13°. In the third O2- site, O2- is bonded to three equivalent Li1+, one Mn+4.50+, and two equivalent Co2+ atoms to form OLi3MnCo2 octahedra that share corners with six OLi5Mn octahedra and edges with twelve OLi4Mn2 octahedra. The corner-sharing octahedra tilt angles range from 0–4°. In the fourth O2- site, O2- is bonded to three Li1+, two equivalent Mn+4.50+, and one Co2+ atom to form a mixture of edge and corner-sharing OLi3Mn2Co octahedra. The corner-sharing octahedra tilt angles range from 0–8°.
DOI: 10.17188/1740572
title: Materials Data on InPb by Materials Project

description: PbIn1 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are three inequivalent In sites. In the first In site, In is bonded to six equivalent Pb atoms to form distorted InPb6 cuboctahedra that share corners with six InPb6 cuboctahedra, corners with twelve equivalent PbIn6Pb6 cuboctahedra, edges with twelve InPb6 cuboctahedra, and edges with twelve equivalent PbIn6Pb6 cuboctahedra. All In–Pb bond lengths are 3.49 Å. In the second In site, In is bonded to six Pb atoms to form distorted InPb6 cuboctahedra that share corners with six InPb6 cuboctahedra, corners with fourteen PbIn6Pb6 cuboctahedra, edges with twelve InPb6 cuboctahedra, edges with fourteen PbIn6Pb6 cuboctahedra, and faces with two equivalent PbIn6Pb10 cuboctahedra. All In–Pb bond lengths are 3.49 Å. In the third In site, In is bonded to six Pb atoms to form distorted InPb6 cuboctahedra that share corners with six InPb6 cuboctahedra, corners with fourteen PbIn6Pb6 cuboctahedra, edges with twelve InPb6 cuboctahedra, edges with fourteen PbIn6Pb6 cuboctahedra, and faces with two equivalent PbIn6Pb10 cuboctahedra. All In–Pb bond lengths are 3.49 Å. There are two inequivalent Pb sites. In the first Pb site, Pb is bonded to six In and six equivalent Pb atoms to form distorted PbIn6Pb6 cuboctahedra that share corners with twelve InPb6 cuboctahedra, corners with twelve PbIn6Pb6 cuboctahedra, edges with twelve InPb6 cuboctahedra, edges with twelve PbIn6Pb6 cuboctahedra, and faces with six equivalent PbIn6Pb6 cuboctahedra. All Pb–Pb bond lengths are 3.51 Å. In the second Pb site, Pb is bonded to six In and ten equivalent Pb atoms to form distorted PbIn6Pb10 cuboctahedra that share corners with twelve PbIn6Pb6 cuboctahedra, corners with sixteen InPb6 cuboctahedra, edges with sixteen InPb6 cuboctahedra, edges with sixteen PbIn6Pb6 cuboctahedra, faces with four InPb6 cuboctahedra, and faces with sixteen equivalent PbIn6Pb10 cuboctahedra. There are a spread of Pb–Pb bond distances ranging from 3.51–7.02 Å.
DOI: 10.6084/m9.figshare.13335746
title: PS B (Chapter II, Evans Dissertation)

description: This is drone product set B from Chapter II of Alexandra's dissertation.<br>The orthomosaic and DSM show East Branch Piscataqua River in Falmouth, ME, USA. The imagery was collected on October 16, 2017 using a DJI Phantom 3 Professional drone. Note that the elevation values are only reliable for examining relative topography across the site. The built-in drone GPS was used for georeferencing during SfM processing, and the EXIF data provided inaccurate altitude measurements. The XY locations are more reliable based on checks against alignment with base maps in ArcGIS. The drone PS' relative accuracy was deemed acceptable for the purposes in Chapter II. Automated drone flight paths were used to collect nadir and angled aerial images with sufficient image overlap for SfM processing in Agisoft PhotoScan Professional. The PhotoScan-generated report includes additional details on the SfM processing workflow and on the drone products.<br>Please see Alexandra's dissertation (University of New Hampshire) for more information on the drone products and project.<br>These materials were made using resources from an NSF EPSCoR funded project “RII Track-2 FEC: Strengthening the scientific basis for decision-making about dams: Multi-scale, coupled-systems research on ecological, social, and economic trade-offs” (a.k.a. "Future of Dams"). Support for this project is provided by the National Science Foundation’s Research Infrastructure Improvement NSF #IIA-1539071. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation.
DOI: 10.6084/m9.figshare.13335746.v1
title: PS B (Chapter II, Evans Dissertation)

description: This is drone product set B from Chapter II of Alexandra's dissertation.<br>The orthomosaic and DSM show East Branch Piscataqua River in Falmouth, ME, USA. The imagery was collected on October 16, 2017 using a DJI Phantom 3 Professional drone. Note that the elevation values are only reliable for examining relative topography across the site. The built-in drone GPS was used for georeferencing during SfM processing, and the EXIF data provided inaccurate altitude measurements. The XY locations are more reliable based on checks against alignment with base maps in ArcGIS. The drone PS' relative accuracy was deemed acceptable for the purposes in Chapter II. Automated drone flight paths were used to collect nadir and angled aerial images with sufficient image overlap for SfM processing in Agisoft PhotoScan Professional. The PhotoScan-generated report includes additional details on the SfM processing workflow and on the drone products.<br>Please see Alexandra's dissertation (University of New Hampshire) for more information on the drone products and project.<br>These materials were made using resources from an NSF EPSCoR funded project “RII Track-2 FEC: Strengthening the scientific basis for decision-making about dams: Multi-scale, coupled-systems research on ecological, social, and economic trade-offs” (a.k.a. "Future of Dams"). Support for this project is provided by the National Science Foundation’s Research Infrastructure Improvement NSF #IIA-1539071. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation.
DOI: 10.17188/1740573
title: Materials Data on P7Pb by Materials Project

description: PbP7 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Pb2+ is bonded in a 3-coordinate geometry to three P+0.29- atoms. There are a spread of Pb–P bond distances ranging from 2.87–3.03 Å. There are seven inequivalent P+0.29- sites. In the first P+0.29- site, P+0.29- is bonded in a trigonal non-coplanar geometry to one Pb2+ and two P+0.29- atoms. There are one shorter (2.21 Å) and one longer (2.24 Å) P–P bond lengths. In the second P+0.29- site, P+0.29- is bonded in a distorted trigonal non-coplanar geometry to three P+0.29- atoms. There are a spread of P–P bond distances ranging from 2.24–2.26 Å. In the third P+0.29- site, P+0.29- is bonded in a trigonal non-coplanar geometry to three P+0.29- atoms. The P–P bond length is 2.23 Å. In the fourth P+0.29- site, P+0.29- is bonded in a 3-coordinate geometry to three P+0.29- atoms. The P–P bond length is 2.21 Å. In the fifth P+0.29- site, P+0.29- is bonded in a distorted T-shaped geometry to three P+0.29- atoms. There are two shorter (2.22 Å) and one longer (2.23 Å) P–P bond lengths. In the sixth P+0.29- site, P+0.29- is bonded to two equivalent Pb2+ and two P+0.29- atoms to form distorted corner-sharing PP2Pb2 trigonal pyramids. In the seventh P+0.29- site, P+0.29- is bonded in a distorted trigonal non-coplanar geometry to three P+0.29- atoms.
DOI: 10.17188/1740574
title: Materials Data on MnSiOs2 by Materials Project

description: MnOs2Si is Cyanogen Chloride-like structured and crystallizes in the orthorhombic Immm space group. The structure is zero-dimensional and consists of two manganese molecules and two Os2Si clusters. In each Os2Si cluster, Os1+ is bonded in a single-bond geometry to one Si4- atom. The Os–Si bond length is 2.19 Å. Si4- is bonded in a linear geometry to two equivalent Os1+ atoms.
DOI: 10.17188/1740575
title: Materials Data on TiVCN by Materials Project

description: TiVCN is alpha Po-derived structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. Ti4+ is bonded to three equivalent C4- and three equivalent N3- atoms to form TiC3N3 octahedra that share corners with six equivalent VC3N3 octahedra, edges with six equivalent TiC3N3 octahedra, and edges with six equivalent VC3N3 octahedra. The corner-sharing octahedra tilt angles range from 1–2°. All Ti–C bond lengths are 2.12 Å. All Ti–N bond lengths are 2.14 Å. V3+ is bonded to three equivalent C4- and three equivalent N3- atoms to form VC3N3 octahedra that share corners with six equivalent TiC3N3 octahedra, edges with six equivalent TiC3N3 octahedra, and edges with six equivalent VC3N3 octahedra. The corner-sharing octahedra tilt angles range from 1–2°. All V–C bond lengths are 2.07 Å. All V–N bond lengths are 2.12 Å. C4- is bonded to three equivalent Ti4+ and three equivalent V3+ atoms to form CTi3V3 octahedra that share corners with six equivalent NTi3V3 octahedra, edges with six equivalent CTi3V3 octahedra, and edges with six equivalent NTi3V3 octahedra. The corner-sharing octahedra tilt angles range from 1–2°. N3- is bonded to three equivalent Ti4+ and three equivalent V3+ atoms to form NTi3V3 octahedra that share corners with six equivalent CTi3V3 octahedra, edges with six equivalent CTi3V3 octahedra, and edges with six equivalent NTi3V3 octahedra. The corner-sharing octahedra tilt angles range from 1–2°.
DOI: 10.6084/m9.figshare.13670530
title: Diversity ant interactions of vascular epiphytes recorded in Ant-gardens in southeastern Mexico

description: File names and description.<br>Morales_Linares_etal_Epiphytes_of_AGs.csv:<br>Records of ant-gardens and vascular epiphytes at 21 sites in southeastern Mexico.<br><br>Morales_Linares_etal_Regional_network.zip:<br>Matrix of interactions (nodes and borders) of vascular epiphytes on a regional scale.<br><br>Morales_Linares_etal_Site_networks.zip:<br>Matrices of interactions (nodes and edges) of vascular epiphytes at the local scale.<br><br>