cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1732567
title: Materials Data on Ti6Al16Rh7 by Materials Project

description: Ti6Rh7Al16 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a 4-coordinate geometry to four equivalent Ti, four equivalent Rh, and eight Al atoms. All Ti–Ti bond lengths are 3.05 Å. All Ti–Rh bond lengths are 3.16 Å. There are four shorter (2.72 Å) and four longer (3.20 Å) Ti–Al bond lengths. There are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a 12-coordinate geometry to four equivalent Ti and eight Al atoms. There are four shorter (2.48 Å) and four longer (2.66 Å) Rh–Al bond lengths. In the second Rh site, Rh is bonded in a body-centered cubic geometry to eight equivalent Al atoms. All Rh–Al bond lengths are 2.53 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded in a distorted trigonal planar geometry to three equivalent Ti and three equivalent Rh atoms. In the second Al site, Al is bonded to three equivalent Ti and four Rh atoms to form a mixture of distorted face, edge, and corner-sharing AlTi3Rh4 tetrahedra.
DOI: 10.17188/1732568
title: Materials Data on SmGePd by Materials Project

description: SmPdGe is hexagonal omega structure-derived structured and crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Sm is bonded to six equivalent Pd and six equivalent Ge atoms to form a mixture of face and edge-sharing SmGe6Pd6 cuboctahedra. All Sm–Pd bond lengths are 3.16 Å. All Sm–Ge bond lengths are 3.16 Å. Pd is bonded in a 9-coordinate geometry to six equivalent Sm and three equivalent Ge atoms. All Pd–Ge bond lengths are 2.59 Å. Ge is bonded in a 9-coordinate geometry to six equivalent Sm and three equivalent Pd atoms.
DOI: 10.17188/1732569
title: Materials Data on AlH12C4NF4 by Materials Project

description: N(CH3)4AlF4 is Silicon tetrafluoride-derived structured and crystallizes in the triclinic P1 space group. The structure is zero-dimensional and consists of one tetramethylammonium molecule and one AlF4 cluster. In the AlF4 cluster, Al3+ is bonded in a tetrahedral geometry to four F1- atoms. All Al–F bond lengths are 1.70 Å. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a single-bond geometry to one Al3+ atom. In the second F1- site, F1- is bonded in a single-bond geometry to one Al3+ atom. In the third F1- site, F1- is bonded in a single-bond geometry to one Al3+ atom. In the fourth F1- site, F1- is bonded in a single-bond geometry to one Al3+ atom.
DOI: 10.5281/zenodo.4492861
title: Renaissance Benchmark Results for OpenJDK, HotSpot and GraalVM

description: The Renaissance Benchmark Suite is an open source collaborative benchmark project where the community can propose and improve benchmark workloads. This archive contains a collection of benchmark results collected on multiple JVM implementations. The measurements in this archive were collected using OpenJDK 1.8.0-252, OpenJDK 11.0.7, HotSpot 1.8.0-251, HotSpot 11.0.7, and GraalVM 20.1.0.
DOI: 10.17188/1732570
title: Materials Data on ZnSnO2 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: 10.5281/zenodo.4492860
title: Renaissance Benchmark Results for OpenJDK, HotSpot and GraalVM

description: The Renaissance Benchmark Suite is an open source collaborative benchmark project where the community can propose and improve benchmark workloads. This archive contains a collection of benchmark results collected on multiple JVM implementations. The measurements in this archive were collected using OpenJDK 1.8.0-252, OpenJDK 11.0.7, HotSpot 1.8.0-251, HotSpot 11.0.7, and GraalVM 20.1.0.
DOI: 10.17188/1732571
title: Materials Data on Hf2MnCo by Materials Project

description: Hf2MnCo crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Hf2MnCo ribbons oriented in the (1, 0, 0) direction. Hf is bonded in a linear geometry to one Mn and one Co atom. The Hf–Mn bond length is 2.38 Å. The Hf–Co bond length is 2.22 Å. Mn is bonded in a linear geometry to two equivalent Hf atoms. Co is bonded in a linear geometry to two equivalent Hf atoms.
DOI: 10.17188/1732572
title: Materials Data on LiMn3O4 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: 10.17188/1732573
title: Materials Data on LaBMoO6 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: 10.17188/1732574
title: Materials Data on SrCoO3 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: 10.17188/1732575
title: Materials Data on MnV2Tc by Materials Project

description: V2TcMn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two V2TcMn ribbons oriented in the (0, 1, 0) direction. V is bonded in a linear geometry to one Tc and one Mn atom. The V–Tc bond length is 2.13 Å. The V–Mn bond length is 2.91 Å. Tc is bonded in a linear geometry to two equivalent V atoms. Mn is bonded in a linear geometry to two equivalent V atoms.
DOI: 10.17188/1732576
title: Materials Data on Ti2CuRe by Materials Project

description: Ti2ReCu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a body-centered cubic geometry to four equivalent Re and four equivalent Cu atoms. All Ti–Re bond lengths are 2.69 Å. All Ti–Cu bond lengths are 2.69 Å. Re is bonded in a body-centered cubic geometry to eight equivalent Ti atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Ti atoms.
DOI: 10.17188/1732577
title: Materials Data on Mn2(Ni7B2)3 by Materials Project

description: Mn2(Ni7B2)3 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mn is bonded in a distorted tetrahedral geometry to four equivalent Ni atoms. All Mn–Ni bond lengths are 2.36 Å. There are three inequivalent Ni sites. In the first Ni site, Ni is bonded in a cuboctahedral geometry to twelve equivalent Ni atoms. All Ni–Ni bond lengths are 2.50 Å. In the second Ni site, Ni is bonded to one Mn and three equivalent B atoms to form a mixture of edge and corner-sharing NiMnB3 tetrahedra. All Ni–B bond lengths are 2.10 Å. In the third Ni site, Ni is bonded in a distorted bent 150 degrees geometry to one Ni and two equivalent B atoms. Both Ni–B bond lengths are 2.05 Å. B is bonded in a 8-coordinate geometry to eight Ni atoms.
DOI: 10.17188/1732578
title: Materials Data on In3SbTe2 by Materials Project

description: In3Sb1Te2 is Caswellsilverite-like structured and crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. there are two inequivalent In+2.33+ sites. In the first In+2.33+ site, In+2.33+ is bonded to two equivalent Sb3- and four equivalent Te2- atoms to form a mixture of edge and corner-sharing InSb2Te4 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. Both In–Sb bond lengths are 3.13 Å. All In–Te bond lengths are 3.16 Å. In the second In+2.33+ site, In+2.33+ is bonded to two equivalent Sb3- and four equivalent Te2- atoms to form a mixture of edge and corner-sharing InSb2Te4 octahedra. The corner-sharing octahedra tilt angles range from 0–5°. Both In–Sb bond lengths are 3.07 Å. All In–Te bond lengths are 3.13 Å. Sb3- is bonded to six In+2.33+ atoms to form SbIn6 octahedra that share corners with two equivalent SbIn6 octahedra, corners with four equivalent TeIn6 octahedra, edges with two equivalent SbIn6 octahedra, and edges with ten equivalent TeIn6 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. Te2- is bonded to six In+2.33+ atoms to form TeIn6 octahedra that share corners with two equivalent SbIn6 octahedra, corners with four equivalent TeIn6 octahedra, edges with five equivalent SbIn6 octahedra, and edges with seven equivalent TeIn6 octahedra. The corner-sharing octahedra tilt angles range from 0–5°.
DOI: 10.17188/1732579
title: Materials Data on Li2Mn7O12 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: 10.17188/1732580
title: Materials Data on Fe5O3F7 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: 10.17188/1732581
title: Materials Data on Li3Co2(GeO4)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: 10.17188/1732583
title: Materials Data on FeTeO5 by Materials Project

description: FeTeO5 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form distorted FeO6 octahedra that share corners with three equivalent TeO5 trigonal bipyramids and an edgeedge with one FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 1.99–2.21 Å. In the second Fe site, Fe is bonded in a distorted hexagonal planar geometry to six O atoms. There are a spread of Fe–O bond distances ranging from 1.91–2.22 Å. There are two inequivalent Te sites. In the first Te site, Te is bonded to five O atoms to form TeO5 trigonal bipyramids that share corners with three equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 42–57°. There are a spread of Te–O bond distances ranging from 1.86–2.01 Å. In the second Te site, Te is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Te–O bond distances ranging from 1.92–2.55 Å. There are ten inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to one Fe and two Te atoms. In the second O site, O is bonded in a water-like geometry to one Fe and one Te atom. In the third O site, O is bonded in a water-like geometry to one Te and one O atom. The O–O bond length is 1.41 Å. In the fourth O site, O is bonded in a distorted trigonal planar geometry to two equivalent Fe and one Te atom. In the fifth O site, O is bonded in a 3-coordinate geometry to two equivalent Fe and one O atom. The O–O bond length is 1.52 Å. In the sixth O site, O is bonded in a bent 150 degrees geometry to one Fe and one Te atom. In the seventh O site, O is bonded in a 3-coordinate geometry to one Fe and two O atoms. In the eighth O site, O is bonded in a 3-coordinate geometry to one Fe and two equivalent Te atoms. In the ninth O site, O is bonded in a bent 120 degrees geometry to one Fe and one Te atom. In the tenth O site, O is bonded in a distorted trigonal non-coplanar geometry to two Fe and one Te atom.
DOI: 10.17188/1732584
title: Materials Data on Ba2NiOsO6 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: 10.17188/1732585
title: Materials Data on Na2In2SiS6 by Materials Project

description: Na2In2SiS6 is Chalcostibite-derived structured and crystallizes in the monoclinic Cc space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded to four S2- atoms to form distorted NaS4 trigonal pyramids that share corners with three equivalent NaS5 square pyramids, corners with two equivalent SiS4 tetrahedra, and corners with six InS4 tetrahedra. There are a spread of Na–S bond distances ranging from 2.76–3.12 Å. In the second Na1+ site, Na1+ is bonded to five S2- atoms to form distorted NaS5 square pyramids that share a cornercorner with one SiS4 tetrahedra, corners with seven InS4 tetrahedra, corners with three equivalent NaS4 trigonal pyramids, and an edgeedge with one SiS4 tetrahedra. There are a spread of Na–S bond distances ranging from 2.79–3.13 Å. There are two inequivalent In3+ sites. In the first In3+ site, In3+ is bonded to four S2- atoms to form InS4 tetrahedra that share corners with four equivalent NaS5 square pyramids, corners with two equivalent InS4 tetrahedra, corners with two equivalent SiS4 tetrahedra, and corners with three equivalent NaS4 trigonal pyramids. There are a spread of In–S bond distances ranging from 2.47–2.54 Å. In the second In3+ site, In3+ is bonded to four S2- atoms to form InS4 tetrahedra that share corners with three equivalent NaS5 square pyramids, corners with two equivalent InS4 tetrahedra, corners with two equivalent SiS4 tetrahedra, and corners with three equivalent NaS4 trigonal pyramids. There are a spread of In–S bond distances ranging from 2.49–2.54 Å. Si4+ is bonded to four S2- atoms to form SiS4 tetrahedra that share a cornercorner with one NaS5 square pyramid, corners with four InS4 tetrahedra, corners with two equivalent NaS4 trigonal pyramids, and an edgeedge with one NaS5 square pyramid. There are three shorter (2.14 Å) and one longer (2.17 Å) Si–S bond lengths. There are six inequivalent S2- sites. In the first S2- site, S2- is bonded to two Na1+ and two In3+ atoms to form corner-sharing SNa2In2 tetrahedra. In the second S2- site, S2- is bonded to two Na1+ and two In3+ atoms to form corner-sharing SNa2In2 tetrahedra. In the third S2- site, S2- is bonded in a distorted trigonal non-coplanar geometry to one Na1+, one In3+, and one Si4+ atom. In the fourth S2- site, S2- is bonded in a distorted trigonal non-coplanar geometry to one Na1+, one In3+, and one Si4+ atom. In the fifth S2- site, S2- is bonded in a 4-coordinate geometry to two Na1+, one In3+, and one Si4+ atom. In the sixth S2- site, S2- is bonded in a distorted trigonal non-coplanar geometry to one Na1+, one In3+, and one Si4+ atom.
DOI: 10.17188/1732586
title: Materials Data on Hf10CuSn7 by Materials Project

description: Hf10CuSn7 crystallizes in the trigonal P-31m space group. The structure is three-dimensional. there are three inequivalent Hf sites. In the first Hf site, Hf is bonded in a 6-coordinate geometry to two equivalent Hf and six equivalent Sn atoms. Both Hf–Hf bond lengths are 2.93 Å. All Hf–Sn bond lengths are 3.07 Å. In the second Hf site, Hf is bonded in a 6-coordinate geometry to two equivalent Hf and six equivalent Sn atoms. All Hf–Sn bond lengths are 3.06 Å. In the third Hf site, Hf is bonded to one Cu and six Sn atoms to form distorted HfCuSn6 pentagonal bipyramids that share corners with two equivalent CuHf6Sn2 octahedra, corners with two equivalent SnHf6Cu2 octahedra, corners with eight equivalent HfCuSn6 pentagonal bipyramids, edges with two equivalent HfCuSn6 pentagonal bipyramids, and faces with six equivalent HfCuSn6 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 57–123°. The Hf–Cu bond length is 2.75 Å. There are a spread of Hf–Sn bond distances ranging from 2.82–3.13 Å. Cu is bonded to six equivalent Hf and two equivalent Sn atoms to form distorted CuHf6Sn2 octahedra that share corners with two equivalent CuHf6Sn2 octahedra, corners with twelve equivalent HfCuSn6 pentagonal bipyramids, and faces with two equivalent SnHf6Cu2 octahedra. The corner-sharing octahedral tilt angles are 0°. Both Cu–Sn bond lengths are 2.93 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 9-coordinate geometry to nine Hf atoms. In the second Sn site, Sn is bonded to six equivalent Hf and two equivalent Cu atoms to form distorted SnHf6Cu2 octahedra that share corners with two equivalent SnHf6Cu2 octahedra, corners with twelve equivalent HfCuSn6 pentagonal bipyramids, and faces with two equivalent CuHf6Sn2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1732587
title: Materials Data on Rb2VCuF6 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: 10.17188/1732588
title: Materials Data on Sr(H2O3)2 by Materials Project

description: Sr(H2O3)2 crystallizes in the monoclinic Cc space group. The structure is three-dimensional. Sr is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Sr–O bond distances ranging from 2.57–2.87 Å. There are four inequivalent H sites. In the first H site, H is bonded in a single-bond geometry to two O atoms. There is one shorter (1.00 Å) and one longer (1.74 Å) H–O bond length. In the second H site, H is bonded in a single-bond geometry to one O atom. The H–O bond length is 0.98 Å. In the third H site, H is bonded in a single-bond geometry to two O atoms. There is one shorter (0.99 Å) and one longer (1.73 Å) H–O bond length. In the fourth H site, H is bonded in a distorted single-bond geometry to two O atoms. There is one shorter (1.01 Å) and one longer (1.67 Å) H–O bond length. There are six inequivalent O sites. In the first O site, O is bonded in a water-like geometry to two equivalent Sr and two H atoms. In the second O site, O is bonded in a 3-coordinate geometry to one Sr, one H, and one O atom. The O–O bond length is 1.36 Å. In the third O site, O is bonded in a water-like geometry to two equivalent Sr and two H atoms. In the fourth O site, O is bonded in a 3-coordinate geometry to two equivalent Sr and one O atom. In the fifth O site, O is bonded in a 3-coordinate geometry to one Sr, one H, and one O atom. The O–O bond length is 1.35 Å. In the sixth O site, O is bonded in a distorted trigonal planar geometry to one Sr, one H, and one O atom.
DOI: 10.17188/1732590
title: Materials Data on V2NiSb2 by Materials Project

description: V2NiSb2 crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. V2+ is bonded to six Sb3- atoms to form distorted VSb6 octahedra that share corners with twelve equivalent VSb6 octahedra, corners with six equivalent NiSb5 trigonal bipyramids, edges with six equivalent VSb6 octahedra, faces with two equivalent VSb6 octahedra, and faces with three equivalent NiSb5 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 51–53°. There are three shorter (2.80 Å) and three longer (2.86 Å) V–Sb bond lengths. Ni2+ is bonded to five Sb3- atoms to form NiSb5 trigonal bipyramids that share corners with twelve equivalent VSb6 octahedra, corners with eight equivalent NiSb5 trigonal bipyramids, and faces with six equivalent VSb6 octahedra. The corner-sharing octahedra tilt angles range from 30–62°. There are three shorter (2.48 Å) and two longer (2.73 Å) Ni–Sb bond lengths. There are two inequivalent Sb3- sites. In the first Sb3- site, Sb3- is bonded in a 8-coordinate geometry to six equivalent V2+ and two equivalent Ni2+ atoms. In the second Sb3- site, Sb3- is bonded in a 9-coordinate geometry to six equivalent V2+ and three equivalent Ni2+ atoms.
DOI: 10.17188/1732591
title: Materials Data on LaTaBi2O7 by Materials Project

description: Bi2LaTaO7 crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. La3+ is bonded to six O2- atoms to form distorted LaO6 octahedra that share corners with two equivalent LaO6 octahedra, corners with four equivalent TaO6 octahedra, and edges with two equivalent BiO6 octahedra. The corner-sharing octahedra tilt angles range from 60–69°. There are two shorter (2.36 Å) and four longer (2.50 Å) La–O bond lengths. Ta5+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with two equivalent TaO6 octahedra, corners with four equivalent LaO6 octahedra, and corners with four equivalent BiO6 octahedra. The corner-sharing octahedra tilt angles range from 11–60°. There is two shorter (1.97 Å) and four longer (2.02 Å) Ta–O bond length. There are two inequivalent Bi3+ sites. In the first Bi3+ site, Bi3+ is bonded to six O2- atoms to form BiO6 octahedra that share corners with two equivalent BiO6 octahedra, corners with four equivalent TaO6 octahedra, and edges with two equivalent LaO6 octahedra. The corner-sharing octahedra tilt angles range from 56–68°. There are two shorter (2.35 Å) and four longer (2.41 Å) Bi–O bond lengths. In the second Bi3+ site, Bi3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Bi–O bond distances ranging from 2.44–2.78 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent Ta5+ atoms. In the second O2- site, O2- is bonded to two equivalent La3+ and two equivalent Bi3+ atoms to form OLa2Bi2 tetrahedra that share corners with six OLa2Bi2 tetrahedra and an edgeedge with one OBi4 tetrahedra. In the third O2- site, O2- is bonded in a 4-coordinate geometry to one La3+, one Ta5+, and two Bi3+ atoms. In the fourth O2- site, O2- is bonded to four Bi3+ atoms to form a mixture of edge and corner-sharing OBi4 tetrahedra.
DOI: 10.17188/1732592
title: Materials Data on Sr2TaVO6 by Materials Project

description: Sr2TaVO6 crystallizes in the tetragonal I4/m space group. The structure is three-dimensional. Sr2+ is bonded to twelve O2- atoms to form SrO12 cuboctahedra that share corners with twelve equivalent SrO12 cuboctahedra, faces with six equivalent SrO12 cuboctahedra, faces with four equivalent TaO6 octahedra, and faces with four equivalent VO6 octahedra. There are a spread of Sr–O bond distances ranging from 2.66–3.02 Å. Ta5+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with six equivalent VO6 octahedra and faces with eight equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–15°. All Ta–O bond lengths are 2.00 Å. V3+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six equivalent TaO6 octahedra and faces with eight equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–15°. There are two shorter (2.00 Å) and four longer (2.05 Å) V–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to four equivalent Sr2+, one Ta5+, and one V3+ atom. In the second O2- site, O2- is bonded in a distorted linear geometry to four equivalent Sr2+, one Ta5+, and one V3+ atom.
DOI: 10.5281/zenodo.4492879
title: mHealth Mapping

description: Review of study characteristics and clinical evidence of experimental studies on mHealth apps for the management of major chronic conditions
DOI: 10.17188/1732593
title: Materials Data on HgS2(IN2)2 by Materials Project

description: HgI2N2(NS)2 crystallizes in the tetragonal P4_2/nmc space group. The structure is zero-dimensional and consists of two 1,3,5,7,2,4,6,8-tetrathiatetrazocane molecules; eight ammonia molecules; and four mercury diiodide molecules.
DOI: 10.5281/zenodo.4492878
title: mHealth Mapping

description: Review of study characteristics and clinical evidence of experimental studies on mHealth apps for the management of major chronic conditions