Unconventional superconductor

Unconventional superconductors are materials that display superconductivity but that do not conform to BCS theory and
Nikolay Bogolyubov theory or its extensions.

The first unconventional triplet superconductor, organic material (TMTSF)₂PF₆,was discovered by Denis Jerome and Klaus Bechgaard in 1979 [D. Jérome, A. Mazaud, M. Ribault, K. Bechgaard, Superconductivity in a synthetic organic conductor: (TMTSF)₂PF₆] , J. Phys. Lett. (Paris) 41, L95 (1980).] . Recent experimental works by Paul Chaikin's and Michael Naughton's groups as well as theoretical analysis of their data by Andrei Lebed have firmly confirmed unconventional triplet nature of superconducting pairing in (TMTSF)₂X (X=PF₆, ClO₄, ...) organic materials. [K. Bechgaard, K. Carneiro, M. Olsen, F. Rasmussen and C.S. Jacobsen, Zero-pressure organic superconductor: di-(tetramethyltetraselenafulvalenium)-perchlorate [(TMTSF)₂ClO₄] , Phys. Rev. Lett. 46, 852 (1981).] The first unconventional singlet d-wave superconductor was discovered by J.G. Bednorz and K.A. Müller in 1986. It was a Lanthanum-based cuprate perovskite material with critical temperature of approximately 35 K (-238 degrees Celsius). This was well above the highest critical temperature known at the time ("T"_c=23 K) and thus the new family of materials were called high-temperature superconductors. Bednorz and Müller received the Nobel prize for Physics for this discovery in 1987.

Since then, many other high-temperature superconductors have been synthesized. As early as 1987,superconductivity above 77 K, the boiling point of nitrogen, was achieved. This is highly significant from the point of view of the technological applications of superconductivity, because liquid nitrogen is far less expensive than liquid helium, which is required to cool conventional superconductors down to their critical temperature. The current record critical temperature is about "T"_c=133 K (-140 °C) at standard pressure, and somewhat higher critical temperatures can be achieved at high pressure. Nevertheless at present it is considered unlikely that cuprate perovskite materials will achieve room-temperature superconductivity.

On the other hand, in recent years other unconventional superconductors have been discovered. These include some that do not superconduct at high temperatures, such as the strontium-ruthenate oxide compounds, but that, like the high-temperature superconductors, are unconventional in other ways (for example, the origin of the attractive force leading to the formation of Cooper pairs may be different from the one postulated in BCS theory). In addition to this, superconductors that have unusually high values of "T"_c but that are not cuprate perovskites have been discovered. Some of them may be extreme examples of conventional superconductors (this is suspected of magnesium diboride, MgB₂, with "T"_c=39 K). Others display more unconventional features.

In 2008 a new class (layered oxypnictide superconductors), for example LaOFeAs, discovered that do not include Copper [cite journal
title = Superconductivity at 43K in an iron-based layered compound LaO_1-xF_xFeAs
author = Hiroki Takahashi, Kazumi Igawa, Kazunobu Arii, Yoichi Kamihara, Masahiro Hirano, Hideo Hosono
journal = Nature
volume = 453
issue =
pages = 376–378
year = 2008
url =
doi = 10.1038/nature06972 ] [http://www.sciam.com/article.cfm?id=iron-exposed-as-high-temp-superconductor] [ [http://www.sciencedaily.com/releases/2008/05/080528140242.htm New High-Temperature Superconductors Are Iron-based With Unusual Magnetic Properties ] ] . An oxypnictide of Samarium seems to have a T_c of about 43K which is higher than predicted by BCS theory [http://arxiv.org/abs/0803.3603v2 Samarium oxypnictide ] .Tests at up to 45 Tesla [ [http://www.planetanalog.com/news/showArticle.jhtml?articleID=208401297 High-temp superconductors pave way for 'supermagnets' ] ] [ [http://www.nature.com/nature/journal/v453/n7197/abs/nature07058.html Two-band superconductivity in LaFeAsO: 0.89: F: 0.11: at very high magnetic fields : Abstract : Nature ] ] suggest the upper critical field of LaFeAsO_0.89F_0.11 may be around 64 Tesla.

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