cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1665329
title: Materials Data on ReH(CO)4 by Materials Project

description: ReH(CO)4 crystallizes in the trigonal P3_1 space group. The structure is one-dimensional and consists of three ReH(CO)4 ribbons oriented in the (0, 0, 1) direction. Re7+ is bonded to four C and two equivalent H1+ atoms to form corner-sharing ReH2C4 octahedra. The corner-sharing octahedral tilt angles are 47°. There are a spread of Re–C bond distances ranging from 1.93–2.00 Å. There is one shorter (1.86 Å) and one longer (1.88 Å) Re–H bond length. There are four inequivalent C sites. In the first C site, C is bonded in a linear geometry to one Re7+ and one O2- atom. The C–O bond length is 1.16 Å. In the second C site, C is bonded in a distorted linear geometry to one Re7+ and one O2- atom. The C–O bond length is 1.16 Å. In the third C site, C is bonded in a linear geometry to one Re7+ and one O2- atom. The C–O bond length is 1.16 Å. In the fourth C site, C is bonded in a distorted linear geometry to one Re7+ and one O2- atom. The C–O bond length is 1.16 Å. H1+ is bonded in a bent 120 degrees geometry to two equivalent Re7+ atoms. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C atom. In the third O2- site, O2- is bonded in a single-bond geometry to one C atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one C atom.
DOI: 10.17188/1665330
title: Materials Data on InGa3N4 by Materials Project

description: InGa3N4 is Enargite-like structured and crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. In3+ is bonded to four N3- atoms to form InN4 tetrahedra that share corners with six equivalent InN4 tetrahedra and corners with six GaN4 tetrahedra. There are three shorter (2.10 Å) and one longer (2.20 Å) In–N bond lengths. There are three inequivalent Ga3+ sites. In the first Ga3+ site, Ga3+ is bonded to four N3- atoms to form GaN4 tetrahedra that share corners with three equivalent InN4 tetrahedra and corners with nine GaN4 tetrahedra. There is one shorter (1.94 Å) and three longer (2.01 Å) Ga–N bond length. In the second Ga3+ site, Ga3+ is bonded to four N3- atoms to form GaN4 tetrahedra that share corners with three equivalent InN4 tetrahedra and corners with nine GaN4 tetrahedra. There is one shorter (1.97 Å) and three longer (2.01 Å) Ga–N bond length. In the third Ga3+ site, Ga3+ is bonded to four N3- atoms to form corner-sharing GaN4 tetrahedra. There is one shorter (1.97 Å) and three longer (2.01 Å) Ga–N bond length. There are four inequivalent N3- sites. In the first N3- site, N3- is bonded to three equivalent In3+ and one Ga3+ atom to form corner-sharing NIn3Ga tetrahedra. In the second N3- site, N3- is bonded to four Ga3+ atoms to form corner-sharing NGa4 tetrahedra. In the third N3- site, N3- is bonded to four Ga3+ atoms to form corner-sharing NGa4 tetrahedra. In the fourth N3- site, N3- is bonded to one In3+ and three equivalent Ga3+ atoms to form corner-sharing NInGa3 tetrahedra.
DOI: 10.17188/1665331
title: Materials Data on CsV2CrO7 by Materials Project

description: CsCrV2O7 crystallizes in the monoclinic P2/c space group. The structure is three-dimensional. Cs1+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Cs–O bond distances ranging from 3.13–3.45 Å. V5+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.64–2.46 Å. Cr3+ is bonded to six O2- atoms to form corner-sharing CrO6 octahedra. The corner-sharing octahedral tilt angles are 63°. There are a spread of Cr–O bond distances ranging from 1.98–2.05 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to three equivalent Cs1+ and one V5+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to three equivalent V5+ and one Cr3+ atom. In the third O2- site, O2- is bonded in a distorted water-like geometry to two equivalent Cs1+, one V5+, and one Cr3+ atom. In the fourth O2- site, O2- is bonded to two equivalent V5+ and two equivalent Cr3+ atoms to form distorted corner-sharing OV2Cr2 trigonal pyramids.
DOI: 10.17188/1665335
title: Materials Data on Y3Ga7Cu4 by Materials Project

description: Y3Cu4Ga7 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 10-coordinate geometry to five Cu and ten Ga atoms. There are a spread of Y–Cu bond distances ranging from 3.02–3.38 Å. There are a spread of Y–Ga bond distances ranging from 3.04–3.37 Å. In the second Y site, Y is bonded to four equivalent Cu and eight Ga atoms to form distorted YGa8Cu4 cuboctahedra that share edges with two equivalent GaY4Ga4Cu4 cuboctahedra and faces with two equivalent YGa8Cu4 cuboctahedra. All Y–Cu bond lengths are 3.14 Å. There are a spread of Y–Ga bond distances ranging from 3.07–3.15 Å. There are two inequivalent Cu sites. In the first Cu site, Cu is bonded in a 10-coordinate geometry to two equivalent Y, one Cu, and seven Ga atoms. The Cu–Cu bond length is 2.51 Å. There are a spread of Cu–Ga bond distances ranging from 2.55–2.79 Å. In the second Cu site, Cu is bonded in a 9-coordinate geometry to five Y, one Cu, and four Ga atoms. There are a spread of Cu–Ga bond distances ranging from 2.45–2.63 Å. There are four inequivalent Ga sites. In the first Ga site, Ga is bonded in a 10-coordinate geometry to four Y, two equivalent Cu, and four Ga atoms. There are a spread of Ga–Ga bond distances ranging from 2.58–2.72 Å. In the second Ga site, Ga is bonded in a 10-coordinate geometry to four Y, five Cu, and one Ga atom. The Ga–Ga bond length is 2.77 Å. In the third Ga site, Ga is bonded to four equivalent Y, four equivalent Cu, and four Ga atoms to form GaY4Ga4Cu4 cuboctahedra that share edges with two equivalent YGa8Cu4 cuboctahedra and faces with two equivalent GaY4Ga4Cu4 cuboctahedra. In the fourth Ga site, Ga is bonded in a 9-coordinate geometry to four Y, two Cu, and three equivalent Ga atoms.
DOI: 10.17188/1665336
title: Materials Data on LiV2NiO6 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: 10.17188/1665337
title: Materials Data on K2NiAuF6 by Materials Project

description: K2NiAuF6 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 F1- atoms to form KF12 cuboctahedra that share corners with twelve equivalent KF12 cuboctahedra, faces with six equivalent KF12 cuboctahedra, faces with four equivalent NiF6 octahedra, and faces with four equivalent AuF6 octahedra. All K–F bond lengths are 3.02 Å. Ni2+ is bonded to six equivalent F1- atoms to form NiF6 octahedra that share corners with six equivalent AuF6 octahedra and faces with eight equivalent KF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Ni–F bond lengths are 1.95 Å. Au2+ is bonded to six equivalent F1- atoms to form AuF6 octahedra that share corners with six equivalent NiF6 octahedra and faces with eight equivalent KF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Au–F bond lengths are 2.31 Å. F1- is bonded in a 6-coordinate geometry to four equivalent K1+, one Ni2+, and one Au2+ atom.
DOI: 10.17188/1665338
title: Materials Data on SrZnCl2 by Materials Project

description: SrCl2Zn crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional and consists of one SrCl2 framework and eight zinc molecules. In the SrCl2 framework, Sr is bonded to six equivalent Cl atoms to form distorted edge-sharing SrCl6 octahedra. There are two shorter (2.96 Å) and four longer (2.97 Å) Sr–Cl bond lengths. Cl is bonded in a trigonal non-coplanar geometry to three equivalent Sr atoms.
DOI: 10.17188/1665339
title: Materials Data on Mg4SiSn by Materials Project

description: Mg4SnSi is alpha bismuth trifluoride-derived structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are two inequivalent Mg sites. In the first Mg site, Mg is bonded to three equivalent Sn and one Si atom to form a mixture of edge and corner-sharing MgSiSn3 tetrahedra. All Mg–Sn bond lengths are 2.88 Å. The Mg–Si bond length is 2.77 Å. In the second Mg site, Mg is bonded to one Sn and three equivalent Si atoms to form a mixture of edge and corner-sharing MgSi3Sn tetrahedra. The Mg–Sn bond length is 2.91 Å. All Mg–Si bond lengths are 2.83 Å. Sn is bonded in a body-centered cubic geometry to eight Mg atoms. Si is bonded in a body-centered cubic geometry to eight Mg atoms.
DOI: 10.17188/1665340
title: Materials Data on Li4VGa3O8 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: 10.17188/1665341
title: Materials Data on Cd3(P3O14)2 by Materials Project

description: (Cd(PO4)2)3(O2)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional and consists of four hydrogen peroxide molecules and one Cd(PO4)2 framework. In the Cd(PO4)2 framework, there are two inequivalent Cd sites. In the first Cd site, Cd is bonded to four O atoms to form CdO4 tetrahedra that share corners with four PO4 tetrahedra. There are a spread of Cd–O bond distances ranging from 2.16–2.18 Å. In the second Cd site, Cd is bonded in a distorted square co-planar geometry to six O atoms. There are a spread of Cd–O bond distances ranging from 2.19–2.81 Å. There are three inequivalent P sites. In the first P site, P is bonded to four O atoms to form PO4 tetrahedra that share corners with two equivalent CdO4 tetrahedra and corners with two PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.49–1.62 Å. In the second P site, P is bonded to four O atoms to form PO4 tetrahedra that share corners with two equivalent CdO4 tetrahedra and corners with two PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.50–1.62 Å. In the third P site, P is bonded to four O atoms to form corner-sharing PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.50–1.64 Å. There are twelve inequivalent O sites. In the first O site, O is bonded in a distorted bent 120 degrees geometry to one Cd and one P atom. In the second O site, O is bonded in a distorted bent 150 degrees geometry to one Cd and one P atom. In the third O site, O is bonded in a single-bond geometry to one Cd atom. In the fourth O site, O is bonded in a bent 150 degrees geometry to one Cd and one P atom. In the fifth O site, O is bonded in a bent 150 degrees geometry to one Cd and one P atom. In the sixth O site, O is bonded in a bent 120 degrees geometry to two P atoms. In the seventh O site, O is bonded in a single-bond geometry to one P atom. In the eighth O site, O is bonded in a bent 120 degrees geometry to two P atoms. In the ninth O site, O is bonded in a distorted bent 120 degrees geometry to one Cd and one O atom. The O–O bond length is 1.24 Å. In the tenth O site, O is bonded in a single-bond geometry to one O atom. In the eleventh O site, O is bonded in a bent 120 degrees geometry to two P atoms. In the twelfth O site, O is bonded in a bent 150 degrees geometry to one Cd and one P atom.
DOI: 10.17188/1665342
title: Materials Data on Rb3H(SO4)2 by Materials Project

description: Rb3H(SO4)2 crystallizes in the monoclinic Cc space group. The structure is three-dimensional. there are three inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 12-coordinate geometry to two equivalent H1+ and ten O2- atoms. There are one shorter (3.01 Å) and one longer (3.02 Å) Rb–H bond lengths. There are a spread of Rb–O bond distances ranging from 2.85–3.30 Å. In the second Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Rb–O bond distances ranging from 3.00–3.22 Å. In the third Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Rb–O bond distances ranging from 3.02–3.31 Å. H1+ is bonded in a linear geometry to two equivalent Rb1+ and two O2- atoms. There is one shorter (1.07 Å) and one longer (1.45 Å) H–O bond length. There are two inequivalent S6+ sites. In the first S6+ site, S6+ is bonded in a tetrahedral geometry to four O2- atoms. There is three shorter (1.47 Å) and one longer (1.60 Å) S–O bond length. In the second S6+ site, S6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of S–O bond distances ranging from 1.48–1.53 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted water-like geometry to three Rb1+, one H1+, and one S6+ atom. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to three Rb1+, one H1+, and one S6+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to four Rb1+ and one S6+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to four Rb1+ and one S6+ atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to four Rb1+ and one S6+ atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to four Rb1+ and one S6+ atom. In the seventh O2- site, O2- is bonded in a distorted single-bond geometry to three Rb1+ and one S6+ atom. In the eighth O2- site, O2- is bonded in a distorted single-bond geometry to three Rb1+ and one S6+ atom.
DOI: 10.17188/1665343
title: Materials Data on ZrCo3 by Materials Project

description: ZrCo3 is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Zr is bonded to twelve Co atoms to form a mixture of face and corner-sharing ZrCo12 cuboctahedra. There are six shorter (2.69 Å) and six longer (2.70 Å) Zr–Co bond lengths. There are two inequivalent Co sites. In the first Co site, Co is bonded in a 12-coordinate geometry to four equivalent Zr and eight Co atoms. There are a spread of Co–Co bond distances ranging from 2.44–2.93 Å. In the second Co site, Co is bonded in a 12-coordinate geometry to four equivalent Zr and eight equivalent Co atoms.
DOI: 10.14457/cu.the.2017.665
title: ภาวะซึมเศร้าและปัจจัยที่เกี่ยวข้องในผู้ป่วยหญิงที่มารับการรักษา ณ คลินิกมีบุตรยาก โรงพยาบาลจุฬาลงกรณ์

description: การวิจัยครั้งนี้เป็นการวิจัยเชิงพรรณนา ณ จุดเวลาใดเวลาหนึ่ง เพื่อศึกษาภาวะซึมเศร้าและปัจจัยที่เกี่ยวข้องในผู้ป่วยหญิงที่มารับการรักษา ณ คลินิกมีบุตรยาก โรงพยาบาลจุฬาลงกรณ์ เก็บรวบรวมข้อมูลจากผู้ป่วยหญิงที่มารับการรักษา ณ คลินิกมีบุตรยากจำนวน 111 คน โดยใช้แบบสอบถามแบบตอบด้วยตนเองซึ่งประกอบ ด้วยแบบสอบถามข้อมูลทั่วไป แบบสอบถามข้อมูลเกี่ยวกับปัจจัยของภาวะมีบุตรยาก แบบสอบถามภาวะซึมเศร้า ของ Beck Depression Inventory - IA (BDI-IA) แบบวัดสัมพันธภาพระหว่างคู่สมรส ของ The Spinner Dyadic Adjustment Scale (DAS) แบบสอบถามความรู้สึกหลากหลายมิติเกี่ยวกับความช่วยเหลือทางสังคม ของ A revised Thai version of Multidimentional Scale of Perceived Social Support (r-T-MSPSS) การวิเคราะห์ข้อมูลใช้ Univariate analysis (ได้แก่ t-test และ Chi-Square) เพื่อทดสอบปัจจัยที่มีความสัมพันธ์กับภาวะซึมเศร้า และใช้ Multivariate Analysis เพื่อหาปัจจัยทำนายภาวะซึมเศร้าในผู้หญิงกลุ่มนี้ ผลการศึกษาพบความชุกของภาวะซึมเศร้าอยู่ที่ ร้อยละ 21.6 โดยมีปัจจัยที่สัมพันธ์กับภาวะซึมเศร้าเมื่อวิเคราะห์โดยวิธี Multivariate analysis 4 ปัจจัย ได้แก่ ความไม่เพียงพอของรายได้ การมีประวัติแท้งบุตร สาเหตุการมีบุตรยากจากการมีพังผืดในอุ้งเชิงกราน และการมีแรงสนับสนุนทางสังคมระดับต่ำ
DOI: 10.17188/1665344
title: Materials Data on Dy3C4 by Materials Project

description: Dy3C4 crystallizes in the tetragonal P4/mnc space group. The structure is three-dimensional. there are four inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven C+2.25- atoms. There are a spread of Dy–C bond distances ranging from 2.35–2.85 Å. In the second Dy3+ site, Dy3+ is bonded to seven C+2.25- atoms to form distorted DyC7 pentagonal bipyramids that share a cornercorner with one DyC6 octahedra, corners with two equivalent DyC7 pentagonal bipyramids, edges with three DyC6 octahedra, edges with two equivalent DyC7 pentagonal bipyramids, and faces with two equivalent DyC7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 1°. There are a spread of Dy–C bond distances ranging from 2.50–2.76 Å. In the third Dy3+ site, Dy3+ is bonded to six C+2.25- atoms to form DyC6 octahedra that share corners with two equivalent DyC6 octahedra, corners with four equivalent DyC7 pentagonal bipyramids, and edges with four equivalent DyC7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 0°. There are two shorter (2.50 Å) and four longer (2.61 Å) Dy–C bond lengths. In the fourth Dy3+ site, Dy3+ is bonded to six C+2.25- atoms to form DyC6 octahedra that share a cornercorner with one DyC6 octahedra and edges with four equivalent DyC7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 0°. There are a spread of Dy–C bond distances ranging from 2.34–2.64 Å. There are seven inequivalent C+2.25- sites. In the first C+2.25- site, C+2.25- is bonded to six Dy3+ atoms to form a mixture of edge and corner-sharing CDy6 octahedra. The corner-sharing octahedra tilt angles range from 0–85°. In the second C+2.25- site, C+2.25- is bonded in a 2-coordinate geometry to four equivalent Dy3+ and two equivalent C+2.25- atoms. Both C–C bond lengths are 1.35 Å. In the third C+2.25- site, C+2.25- is bonded to six Dy3+ atoms to form a mixture of edge and corner-sharing CDy6 octahedra. The corner-sharing octahedral tilt angles are 0°. In the fourth C+2.25- site, C+2.25- is bonded to six Dy3+ atoms to form a mixture of edge and corner-sharing CDy6 octahedra. The corner-sharing octahedral tilt angles are 0°. Both C–Dy bond lengths are 2.35 Å. In the fifth C+2.25- site, C+2.25- is bonded to six Dy3+ atoms to form a mixture of edge and corner-sharing CDy6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of C–Dy bond distances ranging from 2.35–2.64 Å. In the sixth C+2.25- site, C+2.25- is bonded in a 6-coordinate geometry to five Dy3+ and one C+2.25- atom. The C–C bond length is 1.31 Å. In the seventh C+2.25- site, C+2.25- is bonded to five Dy3+ and one C+2.25- atom to form a mixture of edge and corner-sharing CDy5C octahedra. The corner-sharing octahedra tilt angles range from 4–85°.
DOI: 10.14457/cu.the.2017.697
title: การศึกษาความสัมพันธ์ของระดับการติดสีสารมิวซินในชิ้นเนื้อของผู้ป่วยโรคผื่นผิวหนังลูปัสอีริย์ธีมาโตซัส ชนิดดิสคอยด์ กับการเป็นการเป็นโรคลูปัสอีริย์ทีมาโตซัสทั่วร่างในโรงพยาบาลจุฬาลงกรณ์ สภากาชาดไทย

description: ที่มา: การติดสีของสารมิวซินในชั้นหนังแท้เป็นองค์ประกอบหนึ่งที่ใช้ช่วยในการวินิจฉัยโรคผื่นผิวหนังลูปัสอีริย์ทีมาโตซัส ชนิดดิสคอยด์ และในการะบวนเกิดโรค สารมิวซินในชั้นหนังแท้เป็นสิ่งที่ทำให้ผื่นผิวหนังอักเสบมากขึ้น อย่างไรก็ตามยังไม่เคยมีการศึกษาว่าการติดสีของสารมิวซินเป็นปัจจัยบอกการเกิดโรคลูปัสอีริย์ทีมาโตซัสทั่วร่างในผู้ป่วยมาก่อนวัตถุประสงค์: ต้องการศึกษาความสามารถในการพยากรณ์การเกิดโรคลูปัสอีริย์ทีมาโตซัสทั่วร่าง (เอสแอลอี) ในผู้ป่วยโรคผื่นผิวหนังลูปัสอีริย์ทีมาโตซัส ชนิดดิสคอยด์ โดยใช้ระดับการติดสีของสารมิวซินในชั้นหนังแท้เป็นงานวิจัยแบบ exploratory study เพื่อมุ่งหวังงานวิจัยต่อยอดวิธีการศึกษา: การวิจัย ณ จุดเวลาใดเวลาหนึ่ง โดยการสืบค้นผู้ป่วยที่วินิจฉัยว่าเป็นโรคผื่นผิวหนังลูปัสอีริย์ทีมาโตซัส ชนิดดิสคอยด์จากการผลพยาธิวิทยา ตั้งแต่ปี 2554-2560 จำนวน 77 คน ณ โรงพยาบาลจุฬาลงกรณ์ สภากาชาดไทย นำชิ้นเนื้อมาย้อมสี H&E, PAS, Alcian blue เพื่อยืนยันการวินิจฉัย และประเมินการติดสีมิวซินจากชั้น papillary dermis, supficial reticular dermis, deep reticular dermis โดยให้คะแนน 0-3 ในแต่ละชั้น (mucin score) หลังจากนั้นเก็บข้อมูลการวินิจฉัยโรคลูปัสอีริย์ทีมาโตซัสทั่วร่างและผลทางห้องปฏิบัติการของผู้ป่วยจากเวชระเบียนผลการศึกษา: : พบผู้ป่วยโรคผื่นผิวหนังลูปัสอีริย์ทีมาโตซัส ชนิดดิสคอยด์อย่างเดียว จำนวน 49 คน ผู้ป่วยโรคผื่นผิวหนังลูปัสอีริย์ทีมาโตซัส ชนิดดิสคอยด์ที่พัฒนาเป็นโรคลูปัสอีริย์ทีมาโตซัสทั่วร่าง จำนวน 8 คน ผู้ป่วยโรคลูปัสอีริย์ทีมาโตซัสทั่วร่างที่มีผื่นผิวหนังลูปัสอีริย์ทีมาโตซัสชนิดดิสคอยด์ภายหลัง จำนวน 5 คน และผู้ป่วยโรคลูปัสอีริย์ทีมาโตซัสทั่วร่างที่มีผื่นผิวหนังลูปัสอีริย์ทีมาโตซัสชนิดดิสคอยด์ พร้อมกันขณะวินิจฉัย จำนวน 15 คน พบว่าค่าเฉลี่ยของการติดสีสารมิวซิน [OR=0.97 (95%CI0.49-1.92)] ค่าสูงสุดของการติดสีสารมิวซิน [OR=0.98 (95%CI0.6-1.58)] การติดสีของสารมิวซินแต่ละชั้นหนังแท้ [Papillary dermis : OR=0.7 (95%0.31-1.57), Superficial reticular dermis: OR=1.06 (95%CI0.62-1.85), Deep reticular dermis: OR=1.04 (95%CI0.64-1.66)] และการพบการติดสีของสารมิวซิน [OR=1.01 (95%CI0.31-3.32] ในชิ้นเนื้อของผู้ป่วยผื่นผิวหนังลูปัสอีริย์ทีมาโตซัสชนิดดิสคอยด์ ไม่สัมพันธ์กับการเป็นโรคโรคลูปัสอีริย์ทีมาโตซัสทั่วร่าง โดยปรับปัจจัยเรื่องของเพศและการกระจายของผื่น นอกจากนี้ยังพบว่าค่าเฉลี่ยของการติดสีสารมิวซินมีความแตกต่างอย่างมีนัยสำคัญในผู้ป่วยโรคผื่นผิวหนังลูปัสอีริย์ทีมาโตซัสชนิดดิสคอยด์ที่สูบบุหรี่และไม่สูบบุหรี่ (p-value=0.013)สรุปผล: การติดสีของสารมิวซินในชั้นหนังแท้ไม่สามารถใช้ในการพยากรณ์การเกิดโรคลูปัสอีริย์ทีมาโตซัสทั่วร่างในผู้ป่วยโรคผื่นผิวหนังลูปัสอีริย์ทีมาโตซัส ชนิดดิสคอยด์ ได้ การสูบบุหรี่อาจเป็นปัจจัยที่สัมพันธ์กับปริมาณมิวซินในผู้ป่วยโรคผื่นผิวหนังลูปัสอีริย์ทีมาโตซัส ชนิดดิสคอยด์ อย่างไรก็ตามอาจมีปัจจัยจำกัดในเรื่องของจำนวนคนไข้ ความเสื่อมของชิ้นเนื้อ ตำแหน่งที่ตัดชิ้นเนื้อของผู้ป่วย และระยะเวลาติดตามการเกิดโรคโรคลูปัสอีริย์ทีมาโตซัสทั่วร่าง
DOI: 10.17188/1665346
title: Materials Data on Mo3(PO4)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: 10.17188/1665347
title: Materials Data on NaCaGaSi2O7 by Materials Project

description: NaCaGaSi2O7 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. Na1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Na–O bond distances ranging from 2.44–2.91 Å. Ca2+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.39–2.76 Å. Ga3+ is bonded to four O2- atoms to form GaO4 tetrahedra that share corners with four SiO4 tetrahedra. There are a spread of Ga–O bond distances ranging from 1.84–1.87 Å. There are two inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one SiO4 tetrahedra and corners with two equivalent GaO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.59–1.69 Å. In the second Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one SiO4 tetrahedra and corners with two equivalent GaO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.60–1.67 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Na1+, one Ca2+, and one Si4+ atom. In the second O2- site, O2- is bonded in a 1-coordinate geometry to one Na1+, two equivalent Ca2+, and one Si4+ atom. In the third O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Ca2+, one Ga3+, and one Si4+ atom. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Na1+, one Ga3+, and one Si4+ atom. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to one Na1+, one Ca2+, one Ga3+, and one Si4+ atom. In the sixth O2- site, O2- is bonded in a 2-coordinate geometry to one Na1+, one Ca2+, one Ga3+, and one Si4+ atom. In the seventh O2- site, O2- is bonded in a 4-coordinate geometry to one Na1+, one Ca2+, and two Si4+ atoms.