cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1759777
title: Materials Data on Ni5P4(O8F)2 by Materials Project

description: Ni5P4(O8F)2 crystallizes in the orthorhombic Aea2 space group. The structure is three-dimensional. there are three inequivalent Ni+2.80+ sites. In the first Ni+2.80+ site, Ni+2.80+ is bonded to five O2- and one F1- atom to form NiO5F octahedra that share corners with two NiO4F2 octahedra, corners with three equivalent PO4 tetrahedra, and edges with two equivalent NiO5F octahedra. The corner-sharing octahedra tilt angles range from 56–69°. There are a spread of Ni–O bond distances ranging from 1.96–2.18 Å. The Ni–F bond length is 2.11 Å. In the second Ni+2.80+ site, Ni+2.80+ is bonded to four O2- and two equivalent F1- atoms to form corner-sharing NiO4F2 octahedra. The corner-sharing octahedra tilt angles range from 46–56°. There are two shorter (2.00 Å) and two longer (2.01 Å) Ni–O bond lengths. Both Ni–F bond lengths are 2.04 Å. In the third Ni+2.80+ site, Ni+2.80+ is bonded to five O2- and one F1- atom to form distorted NiO5F octahedra that share corners with two NiO5F octahedra, corners with two equivalent PO4 tetrahedra, edges with two equivalent NiO5F octahedra, and an edgeedge with one PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 46–69°. There are a spread of Ni–O bond distances ranging from 2.03–2.31 Å. The Ni–F bond length is 2.04 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded in a trigonal planar geometry to three O2- atoms. There is two shorter (1.48 Å) and one longer (1.50 Å) P–O bond length. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with five NiO5F octahedra and an edgeedge with one NiO5F octahedra. The corner-sharing octahedra tilt angles range from 53–67°. There are a spread of P–O bond distances ranging from 1.55–1.57 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to two Ni+2.80+ and one P5+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to one Ni+2.80+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to one Ni+2.80+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to two Ni+2.80+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one Ni+2.80+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Ni+2.80+ and one P5+ atom. In the seventh O2- site, O2- is bonded in a distorted trigonal planar geometry to two Ni+2.80+ and one P5+ atom. In the eighth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to two Ni+2.80+ and one P5+ atom. F1- is bonded in a distorted trigonal planar geometry to three Ni+2.80+ atoms.
DOI: 10.17188/1759778
title: Materials Data on RbPdC4Br by Materials Project

description: RbPdC4Br crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Rb1+ is bonded in a rectangular see-saw-like geometry to four equivalent Br1- atoms. All Rb–Br bond lengths are 3.72 Å. There are two inequivalent Pd2+ sites. In the first Pd2+ site, Pd2+ is bonded to four equivalent C+0.50- and two equivalent Br1- atoms to form corner-sharing PdC4Br2 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pd–C bond lengths are 2.00 Å. Both Pd–Br bond lengths are 2.77 Å. In the second Pd2+ site, Pd2+ is bonded to four equivalent C+0.50- and two Br1- atoms to form corner-sharing PdC4Br2 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pd–C bond lengths are 2.01 Å. Both Pd–Br bond lengths are 2.62 Å. There are two inequivalent C+0.50- sites. In the first C+0.50- site, C+0.50- is bonded in a linear geometry to one Pd2+ and one C+0.50- atom. The C–C bond length is 1.25 Å. In the second C+0.50- site, C+0.50- is bonded in a linear geometry to one Pd2+ and one C+0.50- atom. There are two inequivalent Br1- sites. In the first Br1- site, Br1- is bonded to four equivalent Rb1+ and two Pd2+ atoms to form a mixture of edge and corner-sharing BrRb4Pd2 octahedra. The corner-sharing octahedra tilt angles range from 0–2°. In the second Br1- site, Br1- is bonded to four equivalent Rb1+ and two Pd2+ atoms to form a mixture of edge and corner-sharing BrRb4Pd2 octahedra. The corner-sharing octahedra tilt angles range from 0–2°. All Br–Rb bond lengths are 3.72 Å. The Br–Pd bond length is 2.77 Å.
DOI: 10.17188/1759780
title: Materials Data on LiNiP2O7 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: 10.17188/1759781
title: Materials Data on ZnPd3 by Materials Project

description: Pd3Zn is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Pd is bonded to eight equivalent Pd and four equivalent Zn atoms to form distorted PdZn4Pd8 cuboctahedra that share corners with twelve equivalent PdZn4Pd8 cuboctahedra, edges with eight equivalent ZnPd12 cuboctahedra, edges with sixteen equivalent PdZn4Pd8 cuboctahedra, faces with four equivalent ZnPd12 cuboctahedra, and faces with fourteen equivalent PdZn4Pd8 cuboctahedra. All Pd–Pd bond lengths are 2.78 Å. All Pd–Zn bond lengths are 2.78 Å. Zn is bonded to twelve equivalent Pd atoms to form ZnPd12 cuboctahedra that share corners with twelve equivalent ZnPd12 cuboctahedra, edges with twenty-four equivalent PdZn4Pd8 cuboctahedra, faces with six equivalent ZnPd12 cuboctahedra, and faces with twelve equivalent PdZn4Pd8 cuboctahedra.
DOI: 10.17188/1759782
title: Materials Data on LiPrZn2 by Materials Project

description: LiPrZn2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Zn atoms. All Li–Zn bond lengths are 3.01 Å. Pr is bonded in a body-centered cubic geometry to eight equivalent Zn atoms. All Pr–Zn bond lengths are 3.01 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Pr atoms.
DOI: 10.17188/1759783
title: Materials Data on LaYPd2 by Materials Project

description: LaYPd2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two LaYPd2 ribbons oriented in the (1, 0, 0) direction. La is bonded in a linear geometry to two equivalent Pd atoms. Both La–Pd bond lengths are 2.43 Å. Y is bonded in a linear geometry to two equivalent Pd atoms. Both Y–Pd bond lengths are 2.77 Å. Pd is bonded in a linear geometry to one La and one Y atom.
DOI: 10.17188/1759784
title: Materials Data on H5PbC2SBrN6 by Materials Project

description: PbC2N6H5SBr crystallizes in the monoclinic P2_1/c space group. The structure is two-dimensional and consists of four hydrobromic acid molecules and one PbC2N6H5S sheet oriented in the (0, 0, 1) direction. In the PbC2N6H5S sheet, Pb2+ is bonded in a 4-coordinate geometry to three N3- and one S2- atom. There are a spread of Pb–N bond distances ranging from 2.51–2.78 Å. The Pb–S bond length is 2.94 Å. There are two inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a trigonal planar geometry to three N3- atoms. There are a spread of C–N bond distances ranging from 1.33–1.37 Å. In the second C4+ site, C4+ is bonded in a distorted trigonal planar geometry to two N3- and one S2- atom. There is one shorter (1.33 Å) and one longer (1.39 Å) C–N bond length. The C–S bond length is 1.71 Å. There are six inequivalent N3- sites. In the first N3- site, N3- is bonded in a distorted single-bond geometry to one Pb2+, one C4+, and one N3- atom. The N–N bond length is 1.38 Å. In the second N3- site, N3- is bonded in a distorted single-bond geometry to one Pb2+, one C4+, and one N3- atom. In the third N3- site, N3- is bonded in a distorted water-like geometry to one N3- and two H1+ atoms. The N–N bond length is 1.41 Å. There is one shorter (1.02 Å) and one longer (1.03 Å) N–H bond length. In the fourth N3- site, N3- is bonded in a 2-coordinate geometry to one C4+, one N3-, and one H1+ atom. The N–N bond length is 1.42 Å. The N–H bond length is 1.03 Å. In the fifth N3- site, N3- is bonded in a distorted trigonal planar geometry to two C4+ and one N3- atom. In the sixth N3- site, N3- is bonded in a distorted water-like geometry to one Pb2+, one N3-, and two H1+ atoms. There is one shorter (1.02 Å) and one longer (1.03 Å) N–H bond length. There are five inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. S2- is bonded in a distorted single-bond geometry to one Pb2+ and one C4+ atom.
DOI: 10.17188/1759785
title: Materials Data on Tl2Hg3S4 by Materials Project

description: Hg3Tl2S4 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are two inequivalent Hg2+ sites. In the first Hg2+ site, Hg2+ is bonded in a tetrahedral geometry to four S2- atoms. There are two shorter (2.62 Å) and two longer (2.65 Å) Hg–S bond lengths. In the second Hg2+ site, Hg2+ is bonded in a distorted rectangular see-saw-like geometry to four S2- atoms. There are a spread of Hg–S bond distances ranging from 2.38–3.31 Å. Tl1+ is bonded in a 4-coordinate geometry to five S2- atoms. There are a spread of Tl–S bond distances ranging from 2.98–3.82 Å. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a 5-coordinate geometry to three Hg2+ and two equivalent Tl1+ atoms. In the second S2- site, S2- is bonded in a 5-coordinate geometry to three Hg2+ and three equivalent Tl1+ atoms.
DOI: 10.17188/1759786
title: Materials Data on LiCo2OF5 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: 10.17188/1759787
title: Materials Data on K2GaAuBr6 by Materials Project

description: K2AuGaBr6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. K1+ is bonded to twelve equivalent Br1- atoms to form KBr12 cuboctahedra that share corners with twelve equivalent KBr12 cuboctahedra, faces with six equivalent KBr12 cuboctahedra, faces with four equivalent AuBr6 octahedra, and faces with four equivalent GaBr6 octahedra. All K–Br bond lengths are 3.82 Å. Au1+ is bonded to six equivalent Br1- atoms to form AuBr6 octahedra that share corners with six equivalent GaBr6 octahedra and faces with eight equivalent KBr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Au–Br bond lengths are 2.78 Å. Ga3+ is bonded to six equivalent Br1- atoms to form GaBr6 octahedra that share corners with six equivalent AuBr6 octahedra and faces with eight equivalent KBr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Ga–Br bond lengths are 2.62 Å. Br1- is bonded to four equivalent K1+, one Au1+, and one Ga3+ atom to form a mixture of distorted face, edge, and corner-sharing BrK4GaAu octahedra. The corner-sharing octahedra tilt angles range from 0–60°.
DOI: 10.17188/1759789
title: Materials Data on V2AgN3 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: 10.17188/1759790
title: Materials Data on ErC3O8 by Materials Project

description: ErC3O8 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. Er is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Er–O bond distances ranging from 2.09–2.69 Å. There are three inequivalent C sites. In the first C site, C is bonded in a linear geometry to two O atoms. There is one shorter (1.17 Å) and one longer (1.18 Å) C–O bond length. In the second C site, C is bonded in a linear geometry to two O atoms. There is one shorter (1.17 Å) and one longer (1.18 Å) C–O bond length. In the third C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.28–1.31 Å. There are eight inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to one Er and one C atom. In the second O site, O is bonded in an L-shaped geometry to one Er and one C atom. In the third O site, O is bonded in a single-bond geometry to one Er atom. In the fourth O site, O is bonded in an L-shaped geometry to one Er and one C atom. In the fifth O site, O is bonded in a distorted single-bond geometry to one Er and one C atom. In the sixth O site, O is bonded in a distorted linear geometry to one Er and one C atom. In the seventh O site, O is bonded in a single-bond geometry to one C atom. In the eighth O site, O is bonded in a distorted linear geometry to one Er and one C atom.
DOI: 10.17188/1759791
title: Materials Data on SnSb by Materials Project

description: SnSb is SC16 CuCl, stable at 5GPa-like structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. Sn2+ is bonded to four equivalent Sb2- atoms to form corner-sharing SnSb4 trigonal pyramids. There are one shorter (2.90 Å) and three longer (2.98 Å) Sn–Sb bond lengths. Sb2- is bonded to four equivalent Sn2+ atoms to form corner-sharing SbSn4 trigonal pyramids.
DOI: 10.17188/1759792
title: Materials Data on HfCdPd2 by Materials Project

description: HfPd2Cd crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two HfPd2Cd ribbons oriented in the (1, 0, 0) direction. Hf is bonded in a linear geometry to two equivalent Pd atoms. Both Hf–Pd bond lengths are 2.32 Å. Pd is bonded in a linear geometry to one Hf and one Cd atom. The Pd–Cd bond length is 2.74 Å. Cd is bonded in a linear geometry to two equivalent Pd atoms.
DOI: 10.17188/1759793
title: Materials Data on K2TaCuI6 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: 10.17188/1759794
title: Materials Data on V6O7F5 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: 10.17188/1759795
title: Materials Data on Li4MnCo2O7 by Materials Project

description: Li4MnCo2O7 crystallizes in the triclinic P-1 space group. The structure is one-dimensional and consists of one Li4MnCo2O7 ribbon oriented in the (4, 5, 3) direction. there are five inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a linear geometry to two O2- atoms. There is one shorter (1.21 Å) and one longer (1.29 Å) Li–O bond length. In the second Li1+ site, Li1+ is bonded in a linear geometry to two O2- atoms. There is one shorter (1.24 Å) and one longer (1.34 Å) Li–O bond length. In the third Li1+ site, Li1+ is bonded in a linear geometry to two O2- atoms. There is one shorter (1.20 Å) and one longer (1.21 Å) Li–O bond length. In the fourth Li1+ site, Li1+ is bonded in a linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.30 Å. In the fifth Li1+ site, Li1+ is bonded in a linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.20 Å. Mn2+ is bonded in a linear geometry to two O2- atoms. There is one shorter (1.15 Å) and one longer (1.25 Å) Mn–O bond length. There are two inequivalent Co4+ sites. In the first Co4+ site, Co4+ is bonded in a bent 150 degrees geometry to two O2- atoms. There is one shorter (1.05 Å) and one longer (1.37 Å) Co–O bond length. In the second Co4+ site, Co4+ is bonded in a linear geometry to two O2- atoms. There is one shorter (1.23 Å) and one longer (1.26 Å) Co–O bond length. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to one Li1+ and one Mn2+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Li1+ and one Co4+ atom. In the third O2- site, O2- is bonded in a linear geometry to one Li1+ and one Co4+ atom. In the fourth O2- site, O2- is bonded in a bent 150 degrees geometry to two Li1+ atoms. In the fifth O2- site, O2- is bonded in a linear geometry to one Li1+ and one Co4+ atom. In the sixth O2- site, O2- is bonded in a linear geometry to one Li1+ and one Co4+ atom. In the seventh O2- site, O2- is bonded in a linear geometry to one Li1+ and one Mn2+ atom.
DOI: 10.17188/1759796
title: Materials Data on NiPdO3 by Materials Project

description: PdNiO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Pd4+ is bonded to twelve equivalent O2- atoms to form PdO12 cuboctahedra that share corners with twelve equivalent PdO12 cuboctahedra, faces with six equivalent PdO12 cuboctahedra, and faces with eight equivalent NiO6 octahedra. All Pd–O bond lengths are 2.61 Å. Ni2+ is bonded to six equivalent O2- atoms to form NiO6 octahedra that share corners with six equivalent NiO6 octahedra and faces with eight equivalent PdO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Ni–O bond lengths are 1.85 Å. O2- is bonded in a linear geometry to four equivalent Pd4+ and two equivalent Ni2+ atoms.
DOI: 10.17188/1759797
title: Materials Data on Na2LaCeTi4O12 by Materials Project

description: Na2CeLaTi4O12 is Orthorhombic Perovskite-derived structured and crystallizes in the monoclinic C2 space group. The structure is three-dimensional. Na1+ is bonded in a 3-coordinate geometry to nine O2- atoms. There are a spread of Na–O bond distances ranging from 2.42–2.78 Å. Ce3+ is bonded in a 3-coordinate geometry to nine O2- atoms. There are a spread of Ce–O bond distances ranging from 2.34–2.76 Å. La3+ is bonded in a 3-coordinate geometry to nine O2- atoms. There are a spread of La–O bond distances ranging from 2.40–2.77 Å. There are two inequivalent Ti4+ sites. In the first Ti4+ site, Ti4+ is bonded to six O2- atoms to form corner-sharing TiO6 octahedra. The corner-sharing octahedra tilt angles range from 18–22°. There are a spread of Ti–O bond distances ranging from 1.96–1.99 Å. In the second Ti4+ site, Ti4+ is bonded to six O2- atoms to form corner-sharing TiO6 octahedra. The corner-sharing octahedra tilt angles range from 19–23°. There are a spread of Ti–O bond distances ranging from 1.95–2.00 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to one Na1+, one Ce3+, one La3+, and two Ti4+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, two equivalent La3+, and two equivalent Ti4+ atoms. In the third O2- site, O2- is bonded in a 5-coordinate geometry to one Na1+, two equivalent Ce3+, and two equivalent Ti4+ atoms. In the fourth O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Na1+, one Ce3+, and two Ti4+ atoms. In the fifth O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Na1+, one La3+, and two Ti4+ atoms. In the sixth O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Na1+, one La3+, and two equivalent Ti4+ atoms. In the seventh O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Na1+, one Ce3+, and two equivalent Ti4+ atoms.
DOI: 10.17188/1759798
title: Materials Data on Li2Mn5Si5O16 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: 10.13145/bacdive135944.20201210.5
title: Pseudomonas aeruginosa

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135945.20201210.5
title: Lactobacillus sakei

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135946.20201210.5
title: Escherichia coli

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135947.20201210.5
title: Rhodobacter blasticus

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135948.20201210.5
title: Bacillus acidovorans

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135949.20201210.5
title: Bacillus acidovorans

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135950.20201210.5
title: Streptococcus suis

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135951.20201210.5
title: Paracoccus thiocyanatus

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135952.20201210.5
title: Salmonella enterica

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135953.20201210.5
title: Serratia proteamaculans

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135954.20201210.5
title: Pseudomonas lundensis

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135955.20201210.5
title: Staphylococcus aureus

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135956.20201210.5
title: Corynebacterium diphtheriae

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135957.20201210.5
title: Carnobacterium maltaromaticum

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135958.20201210.5
title: Moraxella osloensis

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.
DOI: 10.13145/bacdive135959.20201210.5
title: Escherichia coli

description: The range of data encompasses taxonomy, morphology, physiology, sampling and concomitant environmental conditions as well as molecular biology.