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Magnesium diboride

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203: 130: 87: 33: 799:, sigma bond of boron is strong, and it induces large s-wave superconducting gap, and pi bond is weak and induces small s-wave gap. The quasiparticle states of the vortices of large gap are highly confined to the vortex core. On the other hand, the quasiparticle states of small gap are loosely bound to the vortex core. Thus they can be delocalized and overlap easily between adjacent vortices. Such delocalization can strongly contribute to the 24: 835: 358: 853: 507:, in which vortices are separated by the critical distance. When the applied flux is too small for the entire superconductor to be filled with a lattice of vortices separated by the critical distance, then there are large regions of type I superconductivity, a Meissner state, separating these domains. 498:
It has been predicted that when two different bands of electrons yield two quasiparticles, one of which has a coherence length that would indicate type I superconductivity and one of which would indicate type II, then in certain cases, vortices attract at long distances and repel at short distances.
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experiments at 4.2 Kelvin. The authors found that there are indeed regimes with a much greater density of vortices. Whereas the typical variation in the spacing between Abrikosov vortices in a type II superconductor is of order 1%, they found a variation of order 50%, in line with the idea that
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Xi, X.X.; Pogrebnyakov, A.V.; Xu, S.Y.; Chen, K.; Cui, Y.; Maertz, E.C.; Zhuang, C.G.; Li, Qi; Lamborn, D.R.; Redwing, J.M.; Liu, Z.K.; Soukiassian, A.; Schlom, D.G.; Weng, X.J.; Dickey, E.C.; Chen, Y.B.; Tian, W.; Pan, X.Q.; Cybart, S.A.; Dynes, R.C.; et al. (14 February 2007).
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An alternative technique, disclosed in 2003, employs reactive liquid infiltration of magnesium inside a granular preform of boron powders and was called Mg-RLI technique. The method allowed the manufacture of both high density (more than 90% of the theoretical density for
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Unlike elemental boron whose combustion is incomplete through the glassy oxide layered impeding oxygen diffusion, magnesium diboride burns completely when ignited in oxygen or in mixtures with oxidizers. Thus magnesium boride has been proposed as fuel in
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Larbalestier, D. C.; Cooley, L. D.; Rikel, M. O.; Polyanskii, A. A.; Jiang, J.; Patnaik, S.; Cai, X. Y.; Feldmann, D. M.; et al. (2001). "Strongly linked current flow in polycrystalline forms of the superconductor MgB2".
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Properties depend greatly on composition and fabrication process. Many properties are anisotropic due to the layered structure. 'Dirty' samples, e.g., with oxides at the crystal boundaries, are different from 'clean' samples.
966:(MTV) payloads. An application of magnesium diboride to hybrid rocket propulsion has also been investigated, mixing the compound in paraffin wax fuel grains to improve mechanical properties and combustion characteristics. 535:
powders. Formation begins at 650 °C; however, since magnesium metal melts at 652 °C, the reaction may involve diffusion of magnesium vapor across boron grain boundaries. At conventional reaction temperatures,
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B.A.Glowacki, M.Majoros, M.Vickers, J.E.Evetts, Y.Shi and I.McDougall, Superconductivity of powder-in-tube MgB2 wires, Superconductor Science and Technology, 14 (4) 193 (April 2001) | DOI: 10.1088/0953-2048/14/4/304
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Koch, Ernst-Christian; Hahma, Arno; Weiser, Volker; Roth, Evelin; Knapp, Sebastian (2012). "Metal-Fluorocarbon Pyrolants. XIII: High Performance Infrared Decoy Flare Compositions Based on MgB
456:). This is at odds with usual theories of phonon-mediated superconductivity which assume that all electrons behave in the same manner. Theoretical understanding of the properties of MgB 1657: 901:
cables has resulted in superconducting test cables able to carry 20,000 amperes for extremely high current distribution applications, such as the high luminosity upgrade of the
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Moshchalkov, V. V.; Menghini, Mariela; Nishio, T.; Chen, Q.; Silhanek, A.; Dao, V.; Chibotaru, L.; Zhigadlo, N.; Karpinski, J.; et al. (2009). "Type-1.5 Superconductors".
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powder, reduced in diameter, and sintered at 800 to 1000 °C. In both cases, later hot isostatic pressing at approximately 950 °C further improves the properties.
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and the known energy gaps of the pi and sigma bands of electrons (2.2 and 7.1 meV, respectively), the pi and sigma bands of electrons have been found to have two different
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Thin coatings can be used in superconducting radio frequency cavities to minimize energy loss and reduce the inefficiency of liquid helium cooled niobium cavities.
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is used as granular preform inside which YBCO based liquid phases are infiltrated to make superconductive YBCO bulk. This method has been copied and adapted for MgB
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differs strikingly from most low-temperature superconductors, which feature mainly transition metals. Its superconducting mechanism is primarily described by
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Yamada, H; Uchiyama, N; Matsumoto, A; Kitaguchi, H; Kumakura, H (2007). "The excellent superconducting properties of in situ powder-in-tube processed MgB
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conductors have potential uses in superconducting transformers, rotors and transmission cables at temperatures of around 25 K, at fields of 1 T."
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Nagamatsu, Jun; Nakagawa, Norimasa; Muranaka, Takahiro; Zenitani, Yuji; Akimitsu, Jun (2001). "Superconductivity at 39 K in magnesium diboride".
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has promise for use in superconducting low to medium field magnets, electric motors and generators, fault current limiters and current leads.
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and the second is greater, therefore the first seems to indicate marginal type I superconductivity and the second type II superconductivity.
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Nakai, Noriyuki; Ichioka, Masanori; MacHida, Kazushige (2002). "Field Dependence of Electronic Specific Heat in Two-Band Superconductors".
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Vajpayee, A; Awana, V; Balamurugan, S; Takayamamuromachi, E; Kishan, H; Bhalla, G (2007). "Effect of PVA doping on flux pinning in Bulk MgB
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Magnesium diboride was synthesized and its structure confirmed in 1953. The simplest synthesis involves high temperature reaction between
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Superconducting properties and low cost make magnesium diboride attractive for a variety of applications. For those applications, MgB
2645: 2164: 217: 1162:& Speight, Martin (2005). "Semi-Meissner state and neither type-I nor type-II superconductivity in multicomponent systems". 2111: 588: 1595: 378: 3423: 2157: 587:) bulk materials and special hollow fibers. This method is equivalent to similar melt growth based methods such as the 460:
has nearly been achieved by modelling two energy gaps. In 2001 it was regarded as behaving more like a metallic than a
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Bertoldi, A. E. M.; Bouziane, M.; Hendrick, P.; Vandevelde, C.; Lefebvre, M.; Veras, C. A. G. (28 May – 1 June 2018).
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Even small amounts of doping lead both bands into the type II regime and so no semi-Meissner state may be expected.
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coils, operating in the 20–25 K range without liquid helium for cooling. ... Besides the magnet applications MgB
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is a multi-band superconductor, that is each Fermi surface has different superconducting energy gap. For MgB
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Jones, Morton E. & Marsh, Richard E. (1954). "The Preparation and Structure of Magnesium Boride, MgB
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Giunchi, G.; Ceresara, S.; Ripamonti, G.; Chiarelli, S.; Spadoni, M.; et al. (6 August 2002). "MgB
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Koch, E.-C.; Weiser, V. and Roth, E. (2011), Combustion behaviour of Binary Pyrolants based on Mg, MgH
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powder is compressed with silver metal (or 316 stainless steel) into wire and sometimes tape via the
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is minimized at a critical distance. As a consequence there is a conjectured new phase called the
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Braccini, Valeria; Nardelli, Davide; Penco, Roberto; Grasso, Giovanni (2007). "Development of
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vortices assemble into domains where they may be separated by the critical distance. The term
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in blast-enhanced explosives and propellants has been proposed for the same reasons.
305: 169: 118: 1810: 1482: 1145: 693:) is: 10 A/m at 20 T, 10 A/m at 18 T, 10 A/m at 15 T, 10 A/m at 10 T, 10 A/m at 5 T. 624:(HPCVD) has been the most effective technique for depositing magnesium diboride (MgB 1129: 1084: 1019: 776:) in magnetic field is enhanced greatly (approx double at 4.2 K) by doping with ZrB 564: 1553: 611:. The process of Reactive Mg Liquid Infiltration in a boron preform to obtain MgB 563:
variant, a mixture of boron and magnesium is reduced in diameter by conventional
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Sologubenko, A. V.; Jun, J.; Kazakov, S. M.; Karpinski, J.; Ott, H. R. (2002).
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Bray, J.W. (2009). "Superconductors in Applications; Some Practical Aspects".
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Magnesium diboride's superconducting properties were discovered in 2001. Its
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films with smooth surfaces, which are required to make reproducible uniform
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Development and Test of Magnesium-Based Additive for Hybrid Rockets Fuels
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is minimal, although grain recrystallization is sufficient for Josephson
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Experimental confirmation for this conjecture has arrived recently in MgB
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Vinod, K; Kumar, R G Abhilash; Syamaprasad, U (2007). "Prospects for MgB
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Eisterer, M (2007). "Magnetic properties and critical currents of MgB
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Superconducting magnesium diboride wire can be produced through the
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Except where otherwise noted, data are given for materials in their
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Hossain, M S A; et al. (2007). "Significant enhancement of H
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has been a subject of patent applications by the Italian company
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are 0.66±0.02 and 3.68, respectively. The first is less than 1/
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planes) ~3 T, in thin films up to 74 T, in fibers up to 55 T.
480:(51 nm and 13 nm, respectively). The corresponding 405:
at 39 K (−234 °C). In terms of its composition, MgB
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films deposited by other technologies are usually rough and
186: 878:"...the next generation MRI instruments must be made of MgB 452:) being much more strongly superconducting than the other ( 1299:
thin films by hybrid physical-chemical vapor deposition".
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are 33.6 nm and 47.8 nm. This implies that the
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Because of the low cost of its constituent elements, MgB
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830 °C (1,530 °F; 1,100 K) (decomposes)
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bulks at a low sintering temperature of 600 °C".
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only from 39 K to 34 K. The maximum critical current (
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tapes with both ethyltoluene and SiC powder added".
665:The highest superconducting transition temperature 1558:Properties Enhanced by Doping with Carbon Atoms" 1031: 1029: 168: 1658:"Thermal conductivity of single crystalline MgB 958:display 30–60% increased spectral efficiency, E 595:superconductors where the non-superconducting Y 448:with widely differing behaviours, one of them ( 55: 1783:IEEE Transactions on Applied Superconductivity 1261:IEEE Transactions on Applied Superconductivity 2639: 2165: 2146:, US Department of Energy Research News, 2001 8: 499:In particular, the potential energy between 733:and the maximum current density (also with 2646: 2632: 2624: 2172: 2158: 2150: 1905:wires and their applications to magnets". 1872:. Columbus Superconductors. Archived from 1334: 1332: 1330: 201: 128: 106: 15: 2085: 2025:"Light metal explosives and propellants" 1831:superconductors for magnet application". 1741: 1677: 1513: 1175: 1111: 1050: 622:Hybrid physical–chemical vapor deposition 589:Infiltration and Growth Processing method 2049:Si and Polytetrafluoroethylene/Viton®". 1822: 1820: 1730:Journal of the Physical Society of Japan 1221:Journal of the American Chemical Society 867:system was built using 18 km of MgB 1651: 1649: 974: 830: 247: 222: 197: 2687: 2103: 255:......1=2==3=4==5=6==17=23=45=67...... 119: 3140: 2051:Propellants, Explosives, Pyrotechnics 1833:Superconductor Science and Technology 1455:Superconductor Science and Technology 1408:Superconductor Science and Technology 1345:Superconductor Science and Technology 933:Propellants, explosives, pyrotechnics 803:, which shows abrupt increase above H 229:Key: PZKRHHZKOQZHIO-UHFFFAOYSA-N 7: 2670: 762:can reduce the decrease. (Doping MgB 708:planes) is ~14 T, (perpendicular to 575:variant, the tube is filled with MgB 2128:Essential Science Indicators on MgB 1600:in the powder-in-tube processed MgB 1259:reactive sintering from elements". 871:wires. This MRI used a closed-loop 159: 14: 758:) is reduced, but doping with TiB 740:5% doping with carbon can raise H 628:) thin films. The surfaces of MgB 1981:Si and Polytetrafluoroethylene, 851: 842: 833: 356: 31: 22: 962:(J gsr), compared to classical 744:from 16 to 36 T while lowering 609:Reactive Mg Liquid Infiltration 352:(at 25 °C , 100 kPa). 2137:Old material makes a new debut 1596:"Doping effects of ZrC and ZrB 1130:10.1103/PhysRevLett.102.117001 950:containing magnesium diboride/ 769:The maximum critical current ( 1: 640:system can grow high-quality 3434:Non-stoichiometric compounds 2012:, Issued: November 24, 1981. 1907:Physica C: Superconductivity 1502:Physica C: Superconductivity 942:. In addition the use of MgB 725:with carbon (e.g. using 10% 434:conventional superconductors 2110:: CS1 maint: date format ( 1927:10.1016/j.physc.2007.01.030 1532:10.1016/j.physc.2007.05.046 1365:10.1088/0953-2048/20/12/R01 1321:10.1016/j.physc.2007.01.029 721:Various means of doping MgB 519:was coined for this state. 3455: 3142: 1845:10.1088/0953-2048/20/1/R01 1696:10.1103/PhysRevB.66.014504 1584:, Issue date: Oct 11, 2005 1475:10.1088/0953-2048/20/6/L02 1428:10.1088/0953-2048/20/8/L03 1194:10.1103/PhysRevB.72.180502 686:Maximum critical current ( 656:Electromagnetic properties 517:type-1.5 superconductivity 486:Ginzburg-Landau parameters 2689: 2667: 2187: 2006:pyrotechnic composition" 1940:CERN high current project 1803:10.1109/TASC.2009.2019287 1628:10.1007/s11434-006-2155-4 860:In 2006 a 0.5 tesla open 482:London penetration depths 346: 314: 290:45.93 g/mol 263: 238: 213: 39: 30: 21: 1608:Chinese Science Bulletin 1281:10.1109/TASC.2003.812090 919:for its poloidal coils. 2031:, Issued: April 5, 2005 1100:Physical Review Letters 915:design was based on MgB 591:used to fabricate bulk 2063:10.1002/prep.201200044 964:Magnesium/Teflon/Viton 865:superconducting magnet 766:with Ti is patented.) 681:type-II superconductor 462:cuprate superconductor 436:. Among conventional ( 2028:U.S. patent 6,875,294 2009:U.S. patent 4,302,259 1581:U.S. patent 6,953,770 903:Large Hadron Collider 811:Possible applications 717:Improvement by doping 801:thermal conductivity 787:Thermal conductivity 731:upper critical field 698:Upper critical field 423:critical temperature 397:with the formula MgB 3424:Magnesium compounds 2181:Magnesium compounds 2087:10.2514/6.2018-2383 1919:2007PhyC..456..209B 1795:2009ITAS...19.2533B 1752:2002JPSJ...71...23N 1688:2002PhRvB..66a4504S 1620:2006ChSBu..51.2669M 1524:2007PhyC..466...46V 1467:2007SuScT..20L..30Y 1420:2007SuScT..20L..51H 1357:2007SuScT..20R..47E 1313:2007PhyC..456...22X 1273:2003ITAS...13.3060G 1233:10.1021/ja01634a089 1186:2005PhRvB..72r0502B 1122:2009PhRvL.102k7001M 1061:2001Natur.410..186L 996:2001Natur.410...63N 650:Josephson junctions 636:. In contrast, the 505:semi-Meissner state 468:Semi-Meissner state 18: 17:Magnesium diboride 2142:2021-02-08 at the 1951:Ignitor fact sheet 1760:10.1143/JPSJ.71.23 729:) can improve the 696:As of 2008 : 634:non-stoichiometric 559:processes. In the 542:quantum tunnelling 395:inorganic compound 391:Magnesium diboride 379:Infobox references 16: 3439:Ceramic materials 3406: 3405: 3400: 3399: 2621: 2620: 2132:(1992 – May 2002) 2097:978-1-62410-562-3 1666:Physical Review B 1614:(21): 2669–2672. 1164:Physical Review B 1045:(6825): 186–189. 882:coils instead of 735:polyvinyl acetate 607:and rebranded as 478:coherence lengths 417:Superconductivity 387:Chemical compound 385: 384: 322:Crystal structure 182:CompTox Dashboard 88:Interactive image 81:Interactive image 3446: 2671: 2648: 2641: 2634: 2625: 2613: 2612: 2611: 2603: 2602: 2594: 2593: 2174: 2167: 2160: 2151: 2116: 2115: 2109: 2101: 2089: 2073: 2067: 2066: 2038: 2032: 2030: 2019: 2013: 2011: 1994:Ward, J. R. "MgH 1992: 1986: 1959: 1953: 1948: 1942: 1937: 1931: 1930: 1913:(1–2): 209–217. 1894: 1888: 1887: 1885: 1884: 1878: 1871: 1863: 1857: 1856: 1824: 1815: 1814: 1789:(3): 2533–2539. 1778: 1772: 1771: 1745: 1743:cond-mat/0111088 1725: 1719: 1718: 1716: 1715: 1706:. Archived from 1681: 1679:cond-mat/0201517 1653: 1644: 1643: 1638:. Archived from 1591: 1585: 1583: 1572: 1566: 1565: 1564:. June 28, 2004. 1550: 1544: 1543: 1517: 1493: 1487: 1486: 1446: 1440: 1439: 1383: 1377: 1376: 1336: 1325: 1324: 1291: 1285: 1284: 1267:(2): 3060–3063. 1252: 1246: 1243: 1237: 1236: 1212: 1206: 1205: 1179: 1177:cond-mat/0411681 1156: 1150: 1149: 1115: 1095: 1089: 1088: 1069:10.1038/35065559 1054: 1052:cond-mat/0102216 1033: 1024: 1023: 1004:10.1038/35065039 979: 855: 846: 837: 704:): (parallel to 544:between grains. 494: 493: 369: 363: 360: 359: 342:P6/mmm, No. 191 271:Chemical formula 206: 205: 190: 188: 172: 161: 140: 132: 121: 110: 90: 83: 59: 35: 26: 19: 3454: 3453: 3449: 3448: 3447: 3445: 3444: 3443: 3429:Superconductors 3409: 3408: 3407: 3402: 3401: 3371: 3360: 3338: 3333: 3331: 3323: 3318: 3316: 3308: 3303: 3301: 3293: 3288: 3286: 3278: 3273: 3271: 3263: 3258: 3256: 3248: 3243: 3241: 3233: 3225: 3220: 3218: 3207: 3202: 3200: 3192: 3187: 3185: 3177: 3172: 3170: 3162: 3157: 3155: 3046: 3038: 3030: 3026: 3018: 3010: 3002: 2997: 2995: 2984: 2941: 2927: 2919: 2911: 2901: 2863: 2858: 2855: 2847: 2843: 2835: 2831: 2826: 2824: 2805: 2797: 2787: 2782: 2780: 2755: 2747: 2742: 2740: 2732: 2682: 2678: 2663: 2662: 2652: 2622: 2617: 2610: 2607: 2606: 2605: 2601: 2598: 2597: 2596: 2592: 2589: 2588: 2587: 2585: 2580: 2576: 2572: 2564: 2560: 2552: 2548: 2544: 2536: 2532: 2524: 2520: 2511: 2503: 2499: 2491: 2487: 2479: 2471: 2448: 2444: 2440: 2432: 2424: 2411: 2407: 2399: 2391: 2387: 2383: 2375: 2367: 2363: 2355: 2351: 2343: 2335: 2327: 2323: 2315: 2311: 2303: 2295: 2291: 2287: 2279: 2275: 2271: 2267: 2259: 2255: 2251: 2247: 2239: 2235: 2231: 2223: 2219: 2211: 2203: 2195: 2183: 2178: 2144:Wayback Machine 2131: 2124: 2119: 2106:cite conference 2102: 2098: 2075: 2074: 2070: 2048: 2044: 2040: 2039: 2035: 2026: 2020: 2016: 2007: 2005: 2001: 1997: 1993: 1989: 1985:, Reims, France 1980: 1976: 1972: 1968: 1964: 1960: 1956: 1949: 1945: 1938: 1934: 1904: 1896: 1895: 1891: 1882: 1880: 1876: 1869: 1865: 1864: 1860: 1830: 1826: 1825: 1818: 1780: 1779: 1775: 1727: 1726: 1722: 1713: 1711: 1661: 1655: 1654: 1647: 1603: 1599: 1594:Ma, Y. (2006). 1593: 1592: 1588: 1579: 1573: 1569: 1557: 1552: 1551: 1547: 1499: 1495: 1494: 1490: 1452: 1448: 1447: 1443: 1405: 1401: 1397: 1393: 1390:and Hirr in MgB 1389: 1385: 1384: 1380: 1351:(12): R47–R73. 1342: 1338: 1337: 1328: 1298: 1293: 1292: 1288: 1258: 1254: 1253: 1249: 1244: 1240: 1218: 1214: 1213: 1209: 1158: 1157: 1153: 1097: 1096: 1092: 1035: 1034: 1027: 981: 980: 976: 972: 961: 945: 935: 928: 918: 900: 889: 881: 870: 856: 847: 838: 823: 818: 816:Superconductors 813: 806: 798: 794: 789: 779: 775: 765: 761: 757: 750: 743: 724: 719: 703: 692: 678: 671: 658: 647: 631: 627: 614: 606: 602: 598: 586: 578: 570: 525: 513: 491: 489: 470: 459: 438:phonon-mediated 431: 419: 408: 403:superconducting 400: 388: 381: 376: 375: 374:  ?) 365: 361: 357: 353: 339: 324: 279: 273: 259: 256: 251: 246: 245: 234: 231: 230: 227: 221: 220: 209: 191: 184: 175: 162: 150: 113: 93: 73: 62: 49: 12: 11: 5: 3452: 3450: 3442: 3441: 3436: 3431: 3426: 3421: 3411: 3410: 3404: 3403: 3398: 3397: 3394: 3391: 3388: 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2014: 2003: 1999: 1995: 1987: 1978: 1974: 1970: 1966: 1962: 1954: 1943: 1932: 1902: 1889: 1858: 1828: 1816: 1773: 1720: 1659: 1645: 1642:on 2012-02-15. 1601: 1597: 1586: 1567: 1555: 1545: 1508:(1–2): 46–50. 1497: 1488: 1450: 1441: 1414:(8): L51–L54. 1403: 1399: 1395: 1391: 1387: 1378: 1340: 1326: 1307:(1–2): 22–37. 1296: 1286: 1256: 1247: 1238: 1216: 1207: 1170:(18): 180502. 1151: 1106:(11): 117001. 1090: 1025: 990:(6824): 63–4. 973: 971: 968: 959: 943: 934: 931: 926: 916: 898: 887: 879: 868: 858: 857: 850: 848: 841: 839: 832: 826:Powder-in-tube 821: 817: 814: 812: 809: 804: 796: 792: 788: 785: 777: 773: 763: 759: 755: 748: 741: 722: 718: 715: 714: 713: 701: 694: 690: 684: 676: 673: 669: 657: 654: 645: 629: 625: 612: 604: 600: 596: 584: 576: 568: 549:powder-in-tube 524: 521: 511: 469: 466: 457: 429: 418: 415: 406: 398: 386: 383: 382: 377: 355: 354: 350:standard state 347: 344: 343: 340: 335: 332: 331: 325: 320: 317: 316: 312: 311: 308: 302: 301: 298: 292: 291: 288: 282: 281: 277: 274: 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In the 538:sintering 533:magnesium 523:Synthesis 442:electrons 147:234-501-2 139:EC Number 2140:Archived 1811:30296918 1562:Azom.com 1483:95092135 1146:10831135 1138:19392228 1077:11242073 1012:11242039 940:ram jets 672:is 39 K. 644:pure MgB 501:vortices 170:15987061 108:13118398 3419:Borides 3143:  2655:Borides 1915:Bibcode 1899:ex situ 1791:Bibcode 1748:Bibcode 1684:Bibcode 1616:Bibcode 1520:Bibcode 1463:Bibcode 1416:Bibcode 1353:Bibcode 1309:Bibcode 1269:Bibcode 1182:Bibcode 1118:Bibcode 1085:4424264 1057:Bibcode 1020:4388025 992:Bibcode 913:tokamak 910:IGNITOR 642:in situ 573:ex situ 561:in situ 557:in situ 553:ex situ 490:√ 444:at the 393:is the 372:what is 370: ( 296:Density 280: 157:PubChem 2429:Mg(OH) 2360:Mg(HCO 2348:Mg(HCO 2320:Mg(ClO 2308:Mg(ClO 2094:  2045:and Mg 2023:et al. 1851:  1809:  1766:  1702:  1634:  1604:tapes" 1576:et al. 1538:  1481:  1434:  1371:  1200:  1144:  1136:  1083:  1075:  1039:Nature 1018:  1010:  984:Nature 952:Teflon 551:(PIT) 472:Using 367:verify 364:  243:SMILES 2404:Mg(NO 2372:MgHPO 1965:, MgB 1877:(PDF) 1870:(PDF) 1849:S2CID 1807:S2CID 1764:S2CID 1738:arXiv 1700:S2CID 1674:arXiv 1632:S2CID 1536:S2CID 1510:arXiv 1479:S2CID 1432:S2CID 1369:S2CID 1198:S2CID 1172:arXiv 1142:S2CID 1108:arXiv 1081:S2CID 1047:arXiv 1016:S2CID 956:Viton 679:is a 638:HPCVD 599:BaCuO 529:boron 218:InChI 70:JSmol 2573:(CrO 2476:MgSO 2468:MgSO 2458:MgSe 2453:MgPo 2380:Mg(H 2300:MgCl 2208:MgCO 2200:MgBr 2112:link 2092:ISBN 1977:, Mg 1969:, Mg 1554:"MgB 1295:"MgB 1134:PMID 1073:PMID 1008:PMID 908:The 895:CERN 884:NbTi 593:YBCO 555:and 531:and 3396:No 3393:Md 3390:Fm 3387:Es 3384:Cf 3381:Bk 3378:Cm 3375:Am 3368:PuB 3364:Np 3353:Pa 3350:Th 3347:Ac 3344:** 3335:YbB 3328:YbB 3320:TmB 3313:TmB 3305:ErB 3298:ErB 3290:HoB 3283:HoB 3275:DyB 3268:DyB 3260:TbB 3253:TbB 3245:GdB 3238:GdB 3230:EuB 3222:SmB 3215:SmB 3211:Pm 3204:NdB 3197:NdB 3189:PrB 3182:PrB 3174:CeB 3167:CeB 3159:LaB 3152:LaB 3136:Og 3133:Ts 3130:Lv 3127:Mc 3124:Fl 3121:Nh 3118:Cn 3115:Rg 3112:Ds 3109:Mt 3106:Hs 3103:Bh 3100:Sg 3097:Db 3094:Rf 3091:Lr 3088:** 3085:Ra 3082:Fr 3077:Rn 3074:At 3071:Po 3068:Bi 3065:Pb 3062:Tl 3059:Hg 3056:Au 3053:Pt 3050:Ir 3043:OsB 3035:ReB 3015:TaB 3007:HfB 2999:LuB 2992:LuB 2981:BaB 2977:Cs 2972:Xe 2966:Te 2963:Sb 2960:Sn 2957:In 2954:Cd 2951:Ag 2948:Pd 2945:Rh 2938:RuB 2934:Tc 2931:Mo 2924:NbB 2916:ZrB 2898:SrB 2894:Rb 2889:Kr 2886:Br 2883:Se 2880:As 2877:Ge 2874:Ga 2871:Zn 2868:Cu 2821:FeB 2817:Mn 2813:CrB 2802:TiB 2794:ScB 2784:CaB 2777:CaB 2768:Ar 2765:Cl 2752:SiB 2744:AlB 2737:AlB 2729:MgB 2725:Na 2720:Ne 2700:Be 2697:Li 2692:He 2604:MgO 2533:SiO 2484:MgU 2463:MgS 2441:(PO 2421:MgO 2416:MgO 2396:MgI 2340:MgH 2332:MgF 2284:MgC 2272:MgN 2228:MgC 2216:MgC 2192:MgB 2082:doi 2059:doi 1923:doi 1911:456 1841:doi 1799:doi 1756:doi 1692:doi 1624:doi 1528:doi 1506:466 1500:". 1471:doi 1424:doi 1361:doi 1343:". 1317:doi 1305:456 1277:doi 1229:doi 1219:". 1190:doi 1126:doi 1104:102 1065:doi 1043:410 1000:doi 988:410 862:MRI 791:MgB 737:). 675:MgB 583:MgB 329:hP3 276:MgB 187:EPA 160:CID 3415:: 3357:UB 3148:* 2988:* 2969:I 2908:YB 2860:Ni 2852:Ni 2840:Co 2828:Fe 2809:V 2796:12 2773:K 2762:S 2759:P 2746:12 2717:F 2714:O 2711:N 2708:C 2600:46 2591:24 2569:Mg 2557:Mg 2545:Si 2541:Mg 2529:Mg 2521:Ga 2517:Mg 2512:Si 2508:Mg 2500:Al 2496:Mg 2437:Mg 2384:PO 2290:10 2286:14 2258:14 2252:Mg 2250:10 2246:12 2108:}} 2104:{{ 2090:. 2055:37 2053:. 1921:. 1909:. 1847:. 1837:20 1835:. 1819:^ 1805:. 1797:. 1787:19 1785:. 1762:. 1754:. 1746:. 1734:71 1732:. 1698:. 1690:. 1682:. 1670:66 1668:. 1664:. 1648:^ 1630:. 1622:. 1612:51 1610:. 1606:. 1560:. 1534:. 1526:. 1518:. 1504:. 1477:. 1469:. 1459:20 1457:. 1430:. 1422:. 1412:20 1410:. 1394:+C 1388:c2 1367:. 1359:. 1349:20 1347:. 1329:^ 1315:. 1303:. 1275:. 1265:13 1263:. 1225:76 1223:. 1196:. 1188:. 1180:. 1168:72 1166:. 1140:. 1132:. 1124:. 1116:. 1102:. 1079:. 1071:. 1063:. 1055:. 1041:. 1028:^ 1014:. 1006:. 998:. 986:. 905:. 807:. 805:c1 780:. 742:c2 710:ab 706:ab 702:c2 700:(H 464:. 413:. 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2234:6 2232:H 2230:6 2222:4 2220:O 2218:2 2210:3 2202:2 2194:2 2173:e 2166:t 2159:v 2130:2 2114:) 2100:. 2084:: 2065:. 2061:: 2047:2 2043:2 2004:2 2002:) 2000:3 1996:2 1979:2 1975:2 1973:N 1971:3 1967:2 1963:2 1929:. 1925:: 1917:: 1903:2 1886:. 1855:. 1843:: 1829:2 1813:. 1801:: 1793:: 1770:. 1758:: 1750:: 1740:: 1717:. 1694:: 1686:: 1676:: 1662:" 1660:2 1626:: 1618:: 1602:2 1598:2 1556:2 1542:. 1530:: 1522:: 1512:: 1498:2 1485:. 1473:: 1465:: 1451:2 1438:. 1426:: 1418:: 1404:5 1402:O 1400:6 1398:H 1396:4 1392:2 1375:. 1363:: 1355:: 1341:2 1323:. 1319:: 1311:: 1297:2 1283:. 1279:: 1271:: 1257:2 1235:. 1231:: 1217:2 1204:. 1192:: 1184:: 1174:: 1148:. 1128:: 1120:: 1110:: 1087:. 1067:: 1059:: 1049:: 1022:. 1002:: 994:: 960:λ 954:/ 944:2 927:2 917:2 899:2 888:2 880:2 869:2 822:2 797:2 793:2 778:2 774:c 771:J 764:2 760:2 756:c 753:J 749:c 746:T 723:2 691:c 688:J 677:2 670:c 667:T 646:2 630:2 626:2 613:2 605:2 601:5 597:2 585:2 577:2 569:2 512:2 492:2 458:2 430:c 427:T 425:( 407:2 399:2 362:N 278:2 189:) 185:( 72:)

Index

Ball-and-stick model of the part of the crystal structure of magnesium diboride

CAS Number
12007-25-9
JSmol
Interactive image
Interactive image
ChemSpider
13118398
ECHA InfoCard
100.031.352
Edit this at Wikidata
EC Number
PubChem
15987061
CompTox Dashboard
DTXSID60893677
Edit this at Wikidata
InChI
SMILES
Chemical formula
Molar mass
Density
Melting point
Crystal structure
hP3
Space group
standard state
verify
what is

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