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Magnesium diboride

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Magnesium diboride
Ball-and-stick model of the part of the crystal structure of magnesium diboride
Identifiers
3D model (JSmol)
ChemSpider
ECHA InfoCard 100.031.352 Edit this at Wikidata
EC Number
  • 234-501-2
  • InChI=1S/2B.Mg ☒N
    Key: PZKRHHZKOQZHIO-UHFFFAOYSA-N ☒N
  • [B-]=[B-].[Mg+2]
  • [Mg+2].[Mg+2].[Mg+2].[Mg+2].[Mg+2].[Mg+2].[B-]1=[B-][B-]2=[B-][B-]=[B-]3[B-]=[B-][B-]4=[B-][B-]=[B-]5[B-]=[B-][B-]6=[B-][B-]=[B-]1[B-]7=[B-]2[B-]3=[B-]4[B-]5=[B-]67.[Mg+2].[Mg+2].[Mg+2].[Mg+2].[Mg+2].[Mg+2]
Properties
MgB2
Molar mass 45.93 g/mol
Density 2.57 g/cm3
Melting point 830 °C (1,530 °F; 1,100 K) (decomposes)
Structure
Hexagonal, hP3
P6/mmm, No. 191
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa).
☒N verify (what is checkY☒N ?)

Magnesium diboride is the inorganic compound of magnesium and boron with the formula MgB2. It is a dark gray, water-insoluble solid. The compound has attracted attention because it becomes superconducting at 39 K (−234 °C). In terms of its composition, MgB2 differs strikingly from most low-temperature superconductors, which feature mainly transition metals. Its superconducting mechanism is primarily described by BCS theory.

Superconductivity

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Magnesium diboride's superconducting properties were discovered in 2001.[1] Its critical temperature (Tc) of 39 K (−234 °C; −389 °F) is the highest amongst conventional superconductors. Among conventional (phonon-mediated) superconductors, it is unusual. Its electronic structure is such that there exist two types of electrons at the Fermi level with widely differing behaviours, one of them (sigma-bonding) being much more strongly superconducting than the other (pi-bonding). 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 MgB2 has nearly been achieved by modelling two energy gaps. In 2001 it was regarded as behaving more like a metallic than a cuprate superconductor.[2]

Semi-Meissner state

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Using BCS theory 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 coherence lengths (51 nm and 13 nm, respectively).[3] The corresponding London penetration depths are 33.6 nm and 47.8 nm. This implies that the Ginzburg-Landau parameters are 0.66±0.02 and 3.68, respectively. The first is less than 1/√2 and the second is greater, therefore the first seems to indicate marginal type I superconductivity and the second type II superconductivity.

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.[4] In particular, the potential energy between vortices is minimized at a critical distance. As a consequence there is a conjectured new phase called the semi-Meissner state, 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.

Experimental confirmation for this conjecture has arrived recently in MgB2 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 vortices assemble into domains where they may be separated by the critical distance. The term type-1.5 superconductivity was coined for this state.

Synthesis

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Magnesium diboride was synthesized and its structure confirmed in 1953.[5] The simplest synthesis involves high temperature reaction between boron and magnesium powders.[2] 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, sintering is minimal, although grain recrystallization is sufficient for Josephson quantum tunnelling between grains.[citation needed]

Superconducting magnesium diboride wire can be produced through the powder-in-tube (PIT) ex situ and in situ processes.[6] In the in situ variant, a mixture of boron and magnesium is reduced in diameter by conventional wire drawing. The wire is then heated to the reaction temperature to form MgB2. In the ex situ variant, the tube is filled with MgB2 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.[citation needed]

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.[7] The method allowed the manufacture of both high density (more than 90% of the theoretical density for MgB2) bulk materials and special hollow fibers. This method is equivalent to similar melt growth based methods such as the Infiltration and Growth Processing method used to fabricate bulk YBCO superconductors where the non-superconducting Y2BaCuO5 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 MgB2 and rebranded as Reactive Mg Liquid Infiltration. The process of Reactive Mg Liquid Infiltration in a boron preform to obtain MgB2 has been a subject of patent applications by the Italian company Edison S.p.A.[citation needed]

Hybrid physical–chemical vapor deposition (HPCVD) has been the most effective technique for depositing magnesium diboride (MgB2) thin films.[8] The surfaces of MgB2 films deposited by other technologies are usually rough and non-stoichiometric. In contrast, the HPCVD system can grow high-quality in situ pure MgB2 films with smooth surfaces, which are required to make reproducible uniform Josephson junctions, the fundamental element of superconducting circuits.

Electromagnetic properties

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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.[9]

  • The highest superconducting transition temperature Tc is 39 K.
  • MgB2 is a type-II superconductor, i.e. increasing magnetic field gradually penetrates into it.
  • Maximum critical current (Jc) is: 105 A/m2 at 20 T, 106 A/m2 at 18 T, 107 A/m2 at 15 T, 108 A/m2 at 10 T, 109 A/m2 at 5 T.[9]
  • As of 2008 : Upper critical field (Hc2): (parallel to ab planes) is ~14 T, (perpendicular to ab planes) ~3 T, in thin films up to 74 T, in fibers up to 55 T.[9]

Improvement by doping

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Various means of doping MgB2 with carbon (e.g. using 10% malic acid) can improve the upper critical field and the maximum current density[10][11] (also with polyvinyl acetate[12]).

5% doping with carbon can raise Hc2 from 16 to 36 T while lowering Tc only from 39 K to 34 K. The maximum critical current (Jc) is reduced, but doping with TiB2 can reduce the decrease.[13] (Doping MgB2 with Ti is patented.[14])

The maximum critical current (Jc) in magnetic field is enhanced greatly (approx double at 4.2 K) by doping with ZrB2.[15]

Even small amounts of doping lead both bands into the type II regime and so no semi-Meissner state may be expected.

Thermal conductivity

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MgB2 is a multi-band superconductor, that is each Fermi surface has different superconducting energy gap. For MgB2, 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.[16] 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.[17] Such delocalization can strongly contribute to the thermal conductivity, which shows abrupt increase above Hc1.[16]

Possible applications

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Superconductors

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Superconducting properties and low cost make magnesium diboride attractive for a variety of applications.[18][19] For those applications, MgB2 powder is compressed with silver metal (or 316 stainless steel) into wire and sometimes tape via the Powder-in-tube process.

In 2006 a 0.5 tesla open MRI superconducting magnet system was built using 18 km of MgB2 wires. This MRI used a closed-loop cryocooler, without requiring externally supplied cryogenic liquids for cooling.[20][21]

"...the next generation MRI instruments must be made of MgB2 coils instead of NbTi coils, operating in the 20–25 K range without liquid helium for cooling. ... Besides the magnet applications MgB2 conductors have potential uses in superconducting transformers, rotors and transmission cables at temperatures of around 25 K, at fields of 1 T."[19]

A project at CERN to make MgB2 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 Large Hadron Collider.[22]

The IGNITOR tokamak design was based on MgB2 for its poloidal coils.[23]

Thin coatings can be used in superconducting radio frequency cavities to minimize energy loss and reduce the inefficiency of liquid helium cooled niobium cavities.

Because of the low cost of its constituent elements, MgB2 has promise for use in superconducting low to medium field magnets, electric motors and generators, fault current limiters and current leads.[citation needed]

Propellants, explosives, pyrotechnics

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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.[24] Thus magnesium boride has been proposed as fuel in ram jets.[25] In addition the use of MgB2 in blast-enhanced explosives[26] and propellants has been proposed for the same reasons. Decoy flares containing magnesium diboride/Teflon/Viton display 30–60% increased spectral efficiency, Eλ (J g−1sr−1), compared to classical Magnesium/Teflon/Viton(MTV) payloads.[27] 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.[28]

References

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  1. ^ Nagamatsu, Jun; Nakagawa, Norimasa; Muranaka, Takahiro; Zenitani, Yuji; Akimitsu, Jun (2001). "Superconductivity at 39 K in magnesium diboride". Nature. 410 (6824): 63–4. Bibcode:2001Natur.410...63N. doi:10.1038/35065039. PMID 11242039. S2CID 4388025.
  2. ^ a b 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". Nature. 410 (6825): 186–189. arXiv:cond-mat/0102216. Bibcode:2001Natur.410..186L. doi:10.1038/35065559. PMID 11242073. S2CID 4424264.
  3. ^ 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". Physical Review Letters. 102 (11): 117001. arXiv:0902.0997. Bibcode:2009PhRvL.102k7001M. doi:10.1103/PhysRevLett.102.117001. PMID 19392228. S2CID 10831135.
  4. ^ Babaev, Egor & Speight, Martin (2005). "Semi-Meissner state and neither type-I nor type-II superconductivity in multicomponent systems". Physical Review B. 72 (18): 180502. arXiv:cond-mat/0411681. Bibcode:2005PhRvB..72r0502B. doi:10.1103/PhysRevB.72.180502. S2CID 118146361.
  5. ^ Jones, Morton E. & Marsh, Richard E. (1954). "The Preparation and Structure of Magnesium Boride, MgB2". Journal of the American Chemical Society. 76 (5): 1434. doi:10.1021/ja01634a089.
  6. ^ 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
  7. ^ Giunchi, G.; Ceresara, S.; Ripamonti, G.; Chiarelli, S.; Spadoni, M.; et al. (6 August 2002). "MgB2 reactive sintering from elements". IEEE Transactions on Applied Superconductivity. 13 (2): 3060–3063. Bibcode:2003ITAS...13.3060G. doi:10.1109/TASC.2003.812090.
  8. ^ 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). "MgB2 thin films by hybrid physical-chemical vapor deposition". Physica C. 456 (1–2): 22–37. Bibcode:2007PhyC..456...22X. doi:10.1016/j.physc.2007.01.029.
  9. ^ a b c Eisterer, M (2007). "Magnetic properties and critical currents of MgB2". Superconductor Science and Technology. 20 (12): R47 – R73. Bibcode:2007SuScT..20R..47E. doi:10.1088/0953-2048/20/12/R01. S2CID 123577523.
  10. ^ Hossain, M S A; et al. (2007). "Significant enhancement of Hc2 and Hirr in MgB2+C4H6O5 bulks at a low sintering temperature of 600 °C". Superconductor Science and Technology. 20 (8): L51 – L54. Bibcode:2007SuScT..20L..51H. doi:10.1088/0953-2048/20/8/L03. S2CID 118204074.
  11. ^ Yamada, H; Uchiyama, N; Matsumoto, A; Kitaguchi, H; Kumakura, H (2007). "The excellent superconducting properties of in situ powder-in-tube processed MgB2 tapes with both ethyltoluene and SiC powder added". Superconductor Science and Technology. 20 (6): L30. Bibcode:2007SuScT..20L..30Y. doi:10.1088/0953-2048/20/6/L02. S2CID 95092135.
  12. ^ Vajpayee, A; Awana, V; Balamurugan, S; Takayamamuromachi, E; Kishan, H; Bhalla, G (2007). "Effect of PVA doping on flux pinning in Bulk MgB2". Physica C: Superconductivity. 466 (1–2): 46–50. arXiv:0708.3885. Bibcode:2007PhyC..466...46V. doi:10.1016/j.physc.2007.05.046. S2CID 118348153.
  13. ^ "MgB2 Properties Enhanced by Doping with Carbon Atoms". Azom.com. June 28, 2004.
  14. ^ Zhao, Yong et al. "MgB2—based superconductor with high critical current density, and method for manufacturing the same" U.S. patent 6,953,770, Issue date: Oct 11, 2005
  15. ^ Ma, Y. (2006). "Doping effects of ZrC and ZrB2 in the powder-in-tube processed MgB2 tapes". Chinese Science Bulletin. 51 (21): 2669–2672. Bibcode:2006ChSBu..51.2669M. doi:10.1007/s11434-006-2155-4. S2CID 198141335. Archived from the original on 2012-02-15.
  16. ^ a b Sologubenko, A. V.; Jun, J.; Kazakov, S. M.; Karpinski, J.; Ott, H. R. (2002). "Thermal conductivity of single crystalline MgB2". Physical Review B. 66 (1): 14504. arXiv:cond-mat/0201517. Bibcode:2002PhRvB..66a4504S. doi:10.1103/PhysRevB.66.014504. S2CID 119539678. Archived from the original on 2012-02-14. Retrieved 2008-12-18.
  17. ^ Nakai, Noriyuki; Ichioka, Masanori; MacHida, Kazushige (2002). "Field Dependence of Electronic Specific Heat in Two-Band Superconductors". Journal of the Physical Society of Japan. 71 (1): 23–26. arXiv:cond-mat/0111088. Bibcode:2002JPSJ...71...23N. doi:10.1143/JPSJ.71.23. S2CID 119418871.
  18. ^ Bray, J.W. (2009). "Superconductors in Applications; Some Practical Aspects". IEEE Transactions on Applied Superconductivity. 19 (3): 2533–2539. Bibcode:2009ITAS...19.2533B. doi:10.1109/TASC.2009.2019287. S2CID 30296918.
  19. ^ a b Vinod, K; Kumar, R G Abhilash; Syamaprasad, U (2007). "Prospects for MgB2 superconductors for magnet application". Superconductor Science and Technology. 20: R1 – R13. doi:10.1088/0953-2048/20/1/R01. S2CID 122933298.
  20. ^ "First MRI system based on the new Magnesium Diboride superconductor" (PDF). Columbus Superconductors. Archived from the original (PDF) on 2007-06-30. Retrieved 2008-09-22.
  21. ^ Braccini, Valeria; Nardelli, Davide; Penco, Roberto; Grasso, Giovanni (2007). "Development of ex situ processed MgB2 wires and their applications to magnets". Physica C: Superconductivity. 456 (1–2): 209–217. Bibcode:2007PhyC..456..209B. doi:10.1016/j.physc.2007.01.030.
  22. ^ CERN high current project
  23. ^ Ignitor fact sheet
  24. ^ Koch, E.-C.; Weiser, V. and Roth, E. (2011), Combustion behaviour of Binary Pyrolants based on Mg, MgH2, MgB2, Mg3N2, Mg2Si and Polytetrafluoroethylene, EUROPYRO 2011, Reims, France
  25. ^ Ward, J. R. "MgH2 and Sr(NO3)2 pyrotechnic composition" U.S. patent 4,302,259, Issued: November 24, 1981.
  26. ^ Wood, L.L. et al. "Light metal explosives and propellants" U.S. patent 6,875,294, Issued: April 5, 2005
  27. ^ Koch, Ernst-Christian; Hahma, Arno; Weiser, Volker; Roth, Evelin; Knapp, Sebastian (2012). "Metal-Fluorocarbon Pyrolants. XIII: High Performance Infrared Decoy Flare Compositions Based on MgB2 and Mg2Si and Polytetrafluoroethylene/Viton®". Propellants, Explosives, Pyrotechnics. 37 (4): 432. doi:10.1002/prep.201200044.
  28. ^ Bertoldi, A. E. M.; Bouziane, M.; Hendrick, P.; Vandevelde, C.; Lefebvre, M.; Veras, C. A. G. (28 May – 1 June 2018). Development and Test of Magnesium-Based Additive for Hybrid Rockets Fuels. 15th International Conference on Space Operations. American Institute of Aeronautics and Astronautics. doi:10.2514/6.2018-2383. ISBN 978-1-62410-562-3.
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