cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1733750
title: Materials Data on Al4As3O23 by Materials Project

description: (Al4As3O16)2(O2)7 crystallizes in the cubic P-43m space group. The structure is three-dimensional and consists of seven water molecules and one Al4As3O16 framework. In the Al4As3O16 framework, Al is bonded to six O atoms to form AlO6 octahedra that share corners with three equivalent AsO4 tetrahedra and edges with three equivalent AlO6 octahedra. There is three shorter (1.85 Å) and three longer (1.96 Å) Al–O bond length. As is bonded to four equivalent O atoms to form AsO4 tetrahedra that share corners with four equivalent AlO6 octahedra. The corner-sharing octahedral tilt angles are 56°. All As–O bond lengths are 1.71 Å. There are two inequivalent O sites. In the first O site, O is bonded in a trigonal non-coplanar geometry to three equivalent Al atoms. In the second O site, O is bonded in a bent 120 degrees geometry to one Al and one As atom.
DOI: 10.17188/1733751
title: Materials Data on Li4Mn3P4(HO8)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: 10.17188/1733752
title: Materials Data on Zr9Re4O3 by Materials Project

description: Zr9Re4O3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Zr sites. In the first Zr site, Zr is bonded in a distorted bent 150 degrees geometry to two equivalent Re and two equivalent O atoms. Both Zr–Re bond lengths are 2.90 Å. Both Zr–O bond lengths are 2.28 Å. In the second Zr site, Zr is bonded in a 2-coordinate geometry to four Re and two equivalent O atoms. There are two shorter (3.04 Å) and two longer (3.07 Å) Zr–Re bond lengths. Both Zr–O bond lengths are 2.32 Å. There are two inequivalent Re sites. In the first Re site, Re is bonded to eight Zr and four Re atoms to form distorted ReZr8Re4 cuboctahedra that share corners with four equivalent ReZr8Re4 cuboctahedra, corners with four equivalent OZr6 octahedra, faces with eight ReZr6Re6 cuboctahedra, and faces with four equivalent OZr6 octahedra. The corner-sharing octahedral tilt angles are 41°. There are two shorter (2.69 Å) and two longer (2.76 Å) Re–Re bond lengths. In the second Re site, Re is bonded to six equivalent Zr and six equivalent Re atoms to form ReZr6Re6 cuboctahedra that share edges with six equivalent OZr6 octahedra and faces with eight ReZr6Re6 cuboctahedra. O is bonded to six Zr atoms to form OZr6 octahedra that share corners with four equivalent ReZr8Re4 cuboctahedra, corners with six equivalent OZr6 octahedra, edges with two equivalent ReZr6Re6 cuboctahedra, and faces with four equivalent ReZr8Re4 cuboctahedra. The corner-sharing octahedra tilt angles range from 36–45°.
DOI: 10.17188/1733753
title: Materials Data on GdGa3Os by Materials Project

description: GdOsGa3 crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Gd is bonded in a 8-coordinate geometry to four equivalent Os and ten Ga atoms. All Gd–Os bond lengths are 3.23 Å. There are eight shorter (2.97 Å) and two longer (3.23 Å) Gd–Ga bond lengths. Os is bonded to four equivalent Gd and eight equivalent Ga atoms to form distorted OsGd4Ga8 cuboctahedra that share corners with four equivalent OsGd4Ga8 cuboctahedra, edges with four equivalent GaGd6 octahedra, and faces with eight equivalent OsGd4Ga8 cuboctahedra. All Os–Ga bond lengths are 2.68 Å. There are two inequivalent Ga sites. In the first Ga site, Ga is bonded to six equivalent Gd atoms to form GaGd6 octahedra that share corners with six equivalent GaGd6 octahedra and edges with twelve equivalent OsGd4Ga8 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. In the second Ga site, Ga is bonded in a 9-coordinate geometry to three equivalent Gd, three equivalent Os, and three equivalent Ga atoms. All Ga–Ga bond lengths are 2.72 Å.
DOI: 10.17188/1733755
title: Materials Data on Fe3(BrO2)8 by Materials Project

description: Fe3(O2Br)8 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are three inequivalent Fe sites. In the first Fe site, Fe is bonded in a square co-planar geometry to four O atoms. There is two shorter (1.92 Å) and two longer (2.01 Å) Fe–O bond length. In the second Fe site, Fe is bonded in a square co-planar geometry to four O atoms. There is two shorter (1.93 Å) and two longer (1.98 Å) Fe–O bond length. In the third Fe site, Fe is bonded in a square co-planar geometry to four O and two equivalent Br atoms. There is two shorter (1.86 Å) and two longer (1.99 Å) Fe–O bond length. Both Fe–Br bond lengths are 3.01 Å. There are eight inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to one Fe and one Br atom. The O–Br bond length is 1.77 Å. In the second O site, O is bonded in a distorted bent 120 degrees geometry to one Fe and one Br atom. The O–Br bond length is 1.77 Å. In the third O site, O is bonded in a bent 150 degrees geometry to one Fe and one Br atom. The O–Br bond length is 1.92 Å. In the fourth O site, O is bonded in a bent 120 degrees geometry to one Fe and one Br atom. The O–Br bond length is 1.84 Å. In the fifth O site, O is bonded in a 3-coordinate geometry to one Fe and two Br atoms. There are one shorter (2.15 Å) and one longer (2.33 Å) O–Br bond lengths. In the sixth O site, O is bonded in a single-bond geometry to one Br atom. The O–Br bond length is 1.69 Å. In the seventh O site, O is bonded in a distorted single-bond geometry to one Br atom. The O–Br bond length is 1.70 Å. In the eighth O site, O is bonded in a bent 120 degrees geometry to one Fe and one Br atom. The O–Br bond length is 1.74 Å. There are four inequivalent Br sites. In the first Br site, Br is bonded in a water-like geometry to two O atoms. In the second Br site, Br is bonded in a distorted water-like geometry to two O atoms. In the third Br site, Br is bonded in a 4-coordinate geometry to one Fe and three O atoms. In the fourth Br site, Br is bonded in a linear geometry to two O atoms.
DOI: 10.17188/1733756
title: Materials Data on Nd(MnCo2)4 by Materials Project

description: Nd(MnCo2)4 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Nd is bonded in a 12-coordinate geometry to eight equivalent Mn and twelve Co atoms. All Nd–Mn bond lengths are 3.20 Å. There are eight shorter (3.00 Å) and four longer (3.05 Å) Nd–Co bond lengths. Mn is bonded in a 12-coordinate geometry to two equivalent Nd, two equivalent Mn, and eight Co atoms. Both Mn–Mn bond lengths are 2.27 Å. There are four shorter (2.40 Å) and four longer (2.58 Å) Mn–Co bond lengths. There are two inequivalent Co sites. In the first Co site, Co is bonded in a 10-coordinate geometry to one Nd, four equivalent Mn, and nine Co atoms. There are a spread of Co–Co bond distances ranging from 2.35–2.81 Å. In the second Co site, Co is bonded in a 12-coordinate geometry to two equivalent Nd, four equivalent Mn, and six Co atoms. Both Co–Co bond lengths are 2.77 Å.
DOI: 10.17188/1733757
title: Materials Data on Sr6Pr3Cu6O17 by Materials Project

description: Sr6Pr3Cu6O17 crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Sr–O bond distances ranging from 2.46–2.84 Å. In the second Sr2+ site, Sr2+ is bonded to seven O2- atoms to form distorted SrO7 pentagonal bipyramids that share edges with two equivalent SrO7 pentagonal bipyramids and edges with four equivalent CuO5 square pyramids. There are a spread of Sr–O bond distances ranging from 2.49–2.68 Å. There are two inequivalent Pr+3.33+ sites. In the first Pr+3.33+ site, Pr+3.33+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Pr–O bond distances ranging from 2.47–2.50 Å. In the second Pr+3.33+ site, Pr+3.33+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Pr–O bond distances ranging from 2.48–2.70 Å. There are two inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded to five O2- atoms to form CuO5 square pyramids that share corners with three equivalent CuO5 square pyramids and edges with two equivalent SrO7 pentagonal bipyramids. There are a spread of Cu–O bond distances ranging from 1.91–2.26 Å. In the second Cu2+ site, Cu2+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.88–1.96 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded to two Sr2+, two Pr+3.33+, and two equivalent Cu2+ atoms to form distorted OSr2Pr2Cu2 octahedra that share corners with eleven OSr2Pr2Cu2 octahedra, edges with two equivalent OSr2Pr2Cu2 octahedra, and faces with four OSr5Cu octahedra. The corner-sharing octahedra tilt angles range from 1–65°. In the second O2- site, O2- is bonded in a 6-coordinate geometry to two equivalent Sr2+, two equivalent Pr+3.33+, and two Cu2+ atoms. In the third O2- site, O2- is bonded to five Sr2+ and one Cu2+ atom to form distorted OSr5Cu octahedra that share corners with ten OSr2Pr2Cu2 octahedra and edges with eight OSr5Cu octahedra. The corner-sharing octahedra tilt angles range from 10–56°. In the fourth O2- site, O2- is bonded to five Sr2+ and one Cu2+ atom to form distorted OSr5Cu octahedra that share corners with eight OSr2Pr2Cu2 octahedra, edges with eight OSr5Cu octahedra, and faces with two equivalent OSr2Pr2Cu2 octahedra. The corner-sharing octahedra tilt angles range from 1–64°. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Pr+3.33+ and two equivalent Cu2+ atoms. In the sixth O2- site, O2- is bonded to four Pr+3.33+ and two equivalent Cu2+ atoms to form distorted OPr4Cu2 octahedra that share corners with eight OSr2Pr2Cu2 octahedra, edges with three equivalent OPr4Cu2 octahedra, and faces with four equivalent OSr2Pr2Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–65°.
DOI: 10.17188/1733758
title: Materials Data on LiFe(PO3)4 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: 10.17188/1733759
title: Materials Data on Rb5(Pb3Cl8)2 by Materials Project

description: Rb5(Pb3Cl8)2 crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. there are three inequivalent Rb sites. In the first Rb site, Rb is bonded in a 10-coordinate geometry to ten Cl atoms. There are a spread of Rb–Cl bond distances ranging from 3.31–3.69 Å. In the second Rb site, Rb is bonded in a 9-coordinate geometry to nine Cl atoms. There are a spread of Rb–Cl bond distances ranging from 3.28–3.82 Å. In the third Rb site, Rb is bonded in a distorted body-centered cubic geometry to eight equivalent Cl atoms. All Rb–Cl bond lengths are 3.58 Å. There are two inequivalent Pb sites. In the first Pb site, Pb is bonded in a 4-coordinate geometry to four equivalent Cl atoms. All Pb–Cl bond lengths are 3.00 Å. In the second Pb site, Pb is bonded to six Cl atoms to form a mixture of distorted edge and corner-sharing PbCl6 pentagonal pyramids. There are a spread of Pb–Cl bond distances ranging from 2.92–3.07 Å. There are four inequivalent Cl sites. In the first Cl site, Cl is bonded to four Rb and two equivalent Pb atoms to form edge-sharing ClRb4Pb2 octahedra. In the second Cl site, Cl is bonded in a distorted see-saw-like geometry to two equivalent Rb and two equivalent Pb atoms. In the third Cl site, Cl is bonded in a 5-coordinate geometry to three equivalent Rb and two equivalent Pb atoms. In the fourth Cl site, Cl is bonded in a 5-coordinate geometry to three Rb and two Pb atoms.
DOI: 10.17188/1733760
title: Materials Data on LiCr(CoO3)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: 10.17188/1733761
title: Materials Data on La2CoSiO2 by Materials Project

description: La2CoSiO2 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. La3+ is bonded in a 8-coordinate geometry to four equivalent Si4- and four equivalent O2- atoms. All La–Si bond lengths are 3.31 Å. All La–O bond lengths are 2.58 Å. Co2+ is bonded in a square co-planar geometry to four equivalent O2- atoms. All Co–O bond lengths are 1.96 Å. Si4- is bonded in a body-centered cubic geometry to eight equivalent La3+ atoms. O2- is bonded to four equivalent La3+ and two equivalent Co2+ atoms to form a mixture of face, edge, and corner-sharing OLa4Co2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1733762
title: Materials Data on CdPbS2 by Materials Project

description: CdPbS2 is Caswellsilverite structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Cd2+ is bonded to six equivalent S2- atoms to form CdS6 octahedra that share corners with six equivalent PbS6 octahedra, edges with six equivalent CdS6 octahedra, and edges with six equivalent PbS6 octahedra. The corner-sharing octahedral tilt angles are 6°. All Cd–S bond lengths are 2.78 Å. Pb2+ is bonded to six equivalent S2- atoms to form PbS6 octahedra that share corners with six equivalent CdS6 octahedra, edges with six equivalent CdS6 octahedra, and edges with six equivalent PbS6 octahedra. The corner-sharing octahedral tilt angles are 6°. All Pb–S bond lengths are 2.98 Å. S2- is bonded to three equivalent Cd2+ and three equivalent Pb2+ atoms to form a mixture of corner and edge-sharing SCd3Pb3 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1733764
title: Materials Data on MgZn(FeO2)4 by Materials Project

description: MgZn(FeO2)4 is Spinel-derived structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. Mg2+ is bonded to six O2- atoms to form MgO6 octahedra that share corners with three equivalent FeO4 tetrahedra, corners with three equivalent ZnO4 tetrahedra, and edges with six equivalent FeO6 octahedra. There are three shorter (2.06 Å) and three longer (2.12 Å) Mg–O bond lengths. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with three equivalent FeO4 tetrahedra, corners with three equivalent ZnO4 tetrahedra, edges with two equivalent MgO6 octahedra, and edges with four equivalent FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 2.01–2.09 Å. In the second Fe3+ site, Fe3+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with three equivalent MgO6 octahedra and corners with nine equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 57–58°. There is three shorter (1.90 Å) and one longer (2.02 Å) Fe–O bond length. Zn2+ is bonded to four O2- atoms to form ZnO4 tetrahedra that share corners with three equivalent MgO6 octahedra and corners with nine equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 57–59°. There are three shorter (1.98 Å) and one longer (2.02 Å) Zn–O bond lengths. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to three equivalent Fe3+ and one Zn2+ atom. In the second O2- site, O2- is bonded to one Mg2+, two equivalent Fe3+, and one Zn2+ atom to form a mixture of distorted edge and corner-sharing OMgZnFe2 trigonal pyramids. In the third O2- site, O2- is bonded to four Fe3+ atoms to form distorted corner-sharing OFe4 trigonal pyramids. In the fourth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Mg2+ and three Fe3+ atoms.
DOI: 10.17188/1733765
title: Materials Data on MnH4(ClO)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: 10.17188/1733766
title: Materials Data on Cs3SbH2S4O by Materials Project

description: Cs3SbH2S4O crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 1-coordinate geometry to three H1+, seven S2-, and one O2- atom. There are a spread of Cs–H bond distances ranging from 3.35–3.50 Å. There are a spread of Cs–S bond distances ranging from 3.60–3.85 Å. The Cs–O bond length is 3.53 Å. In the second Cs1+ site, Cs1+ is bonded in a 9-coordinate geometry to one H1+, seven S2-, and one O2- atom. The Cs–H bond length is 3.29 Å. There are a spread of Cs–S bond distances ranging from 3.68–4.00 Å. The Cs–O bond length is 3.45 Å. In the third Cs1+ site, Cs1+ is bonded in a 7-coordinate geometry to one H1+, four S2-, and two equivalent O2- atoms. The Cs–H bond length is 3.33 Å. There are a spread of Cs–S bond distances ranging from 3.47–3.76 Å. There are one shorter (3.32 Å) and one longer (3.43 Å) Cs–O bond lengths. Sb5+ is bonded in a tetrahedral geometry to four S2- atoms. There are one shorter (2.35 Å) and three longer (2.37 Å) Sb–S bond lengths. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to two Cs1+ and one O2- atom. The H–O bond length is 1.00 Å. In the second H1+ site, H1+ is bonded in a single-bond geometry to three Cs1+ and one O2- atom. The H–O bond length is 0.99 Å. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded to five Cs1+ and one Sb5+ atom to form distorted edge-sharing SCs5Sb octahedra. In the second S2- site, S2- is bonded in a 1-coordinate geometry to five Cs1+ and one Sb5+ atom. In the third S2- site, S2- is bonded in a 1-coordinate geometry to four Cs1+ and one Sb5+ atom. In the fourth S2- site, S2- is bonded in a distorted single-bond geometry to four Cs1+ and one Sb5+ atom. O2- is bonded in a water-like geometry to four Cs1+ and two H1+ atoms.
DOI: 10.17188/1733767
title: Materials Data on MnFeO2 by Materials Project

description: MnFeO2 is Caswellsilverite-like structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Mn2+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six equivalent MnO6 octahedra, edges with four equivalent MnO6 octahedra, and edges with eight equivalent FeO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (2.20 Å) and two longer (2.21 Å) Mn–O bond lengths. Fe2+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent FeO6 octahedra, edges with four equivalent FeO6 octahedra, and edges with eight equivalent MnO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (2.20 Å) and two longer (2.21 Å) Fe–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Mn2+ and two equivalent Fe2+ atoms to form a mixture of corner and edge-sharing OMn4Fe2 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second O2- site, O2- is bonded to two equivalent Mn2+ and four equivalent Fe2+ atoms to form OMn2Fe4 octahedra that share corners with six equivalent OMn2Fe4 octahedra and edges with twelve OMn4Fe2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.14457/tu.the.2019.1112
title: การเปิดรับ ทัศนคติต่อส่วนประสมทางการตลาดและแนวโน้มพฤติกรรมการซื้อสินค้าทาง e-commerce ของ generation X

description: การวิจัยนี้มีวัตถุประสงค์เพื่อศึกษาการเปิดรับ ทัศนคติต่อส่วนประสมทางการตลาด และแนวโน้มพฤติกรรมการซื้อสินค้าทาง E-Commerce ของ Generation X เป็นการศึกษาวิจัยเชิงปริมาณ (Quantitative Research) รูปแบบวิจัยเชิงสำรวจ โดยใช้แบบสอบถาม เป็นเครื่องมือในการเก็บรวบรวมข้อมูลกับกลุ่มตัวอย่าง โดยมีช่วงอายุตั้งแต่ 41-55 ปี ที่เคยเปิดรับสื่อ E-Commerce และเคยซื้อสินค้าทาง E-Commerce อย่างน้อย 1 ครั้ง จำนวน 300 คน ผลการศึกษาพบว่า Generation X มีพฤติกรรมการเปิดรับสื่อประเภทโซเชียลมีเดียมากที่สุด โดยมีระยะเวลาในการเปิดรับสื่อ E- commerce ระดับน้อย และทัศนคติต่อส่วนประสมทางการตลาดของธุรกิจ E-Commerce ของ Generation X ด้านช่องทางการจัดจำหน่ายมีค่าเฉลี่ยมากที่สุด รองมาคือ ด้านราคา ด้านการส่งเสริมการตลาด ด้านการรักษาความเป็นส่วนตัว ด้านผลิตภัณฑ์ และด้านการให้บริการส่วนบุคคล ตามลำดับ โดยการทดสอบสมมติฐานทั้ง 2 ข้อ 1) ผลการศึกษาพบว่า การเปิดรับสื่อ (ความถี่) มีความสัมพันธ์กันกับทัศนคติต่อส่วนประสมทางการตลาดของธุรกิจ E-Commerce ด้านราคา และการเปิดรับสื่อ (ระยะเวลา) มีความสัมพันธ์กันกับทัศนคติต่อส่วนประสมทางการตลาดของธุรกิจ E-Commerce ส่วนประสมทางการตลาดรวม ด้านการส่งเสริมการตลาด ด้านราคา และด้านการให้บริการส่วนบุคคล 2) ทัศนคติต่อส่วนประสมทางการตลาดมีความสัมพันธ์กับแนวโน้มพฤติกรรมการซื้อสินค้าทาง E-Commerce ของ Generation X
DOI: 10.17188/1733768
title: Materials Data on VBO4 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: 10.17188/1733769
title: Materials Data on MnAlN2 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: 10.17188/1733770
title: Materials Data on NaMnPO4 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: 10.14457/tu.the.2019.1113
title: ปัจจัยที่มีอิทธิพลต่อความผูกพันในการใช้เฟซบุ๊กเพจการศึกษาของประชากรเจเนอเรชันซี (Z)

description: การวิจัยนี้มีวัตถุประสงค์ 1.) เพื่อศึกษาความสัมพันธ์ของบุคลิกภาพห้าองค์ประกอบ แรงจูงใจในการใช้สื่อ พฤติกรรมการใช้สื่อและความผูกพันในการใช้สื่อเฟซบุ๊กเพจการศึกษาของเจเนอเรชันซี (Z) 2.) เพื่อศึกษาความแตกต่างของลักษณะทางประชากรเจเนอเรชันซี (Z) แรงจูงใจในการใช้สื่อและพฤติกรรมการใช้สื่อเฟซบุ๊กเพจการศึกษา เป็นการศึกษาวิจัยเชิงปริมาณ (Quantitative Research) รูปแบบวิจัยเชิงสำรวจ (Survey Research) โดยใช้แบบสอบถาม (Questionnaire) เป็นเครื่องมือในการเก็บรวบรวมข้อมูลกับกลุ่มตัวอย่างที่เป็นประชากรไทยที่มีอายุระหว่าง 16 – 24 ปี เป็นผู้ที่ติดตามเฟซบุ๊กเพจการศึกษาอย่างน้อย 1 เพจ จำนวน 400 ชุด ผลการวิจัยพบว่า ประชากรเจเนอเรชันซี (Z) ที่มีบุคลิกภาพห้าองค์ประกอบ แรงจูงใจในการใช้สื่อและพฤติกรรมการใช้สื่อมีความสัมพันธ์ต่อความผูกพันในการใช้สื่อเฟซบุ๊กเพจการศึกษา และประชากรเจเนอเรชันซี (Z) ที่มีอายุ 16-18 ปี เข้าใช้เฟซบุ๊กเพจการศึกษามากกว่าอายุ 19-24 ปี ผลการวิจัยยังพบว่า ประชากรเจเนอเรชันซี (Z) ที่มีอายุ เพศ และระดับการศึกษาที่แตกต่างกันจะมีจำนวนครั้งในการใช้เฟซบุ๊กเพจการศึกษาไม่แตกต่างกัน
DOI: 10.17188/1733771
title: Materials Data on Yb2TlIn by Materials Project

description: Yb2TlIn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Yb is bonded in a body-centered cubic geometry to four equivalent Tl and four equivalent In atoms. All Yb–Tl bond lengths are 3.35 Å. All Yb–In bond lengths are 3.35 Å. Tl is bonded in a body-centered cubic geometry to eight equivalent Yb atoms. In is bonded in a body-centered cubic geometry to eight equivalent Yb atoms.