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The essence of superconductivity and superconductors.

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Many additional elements can be coaxed into asuperconductive state with the application <strong>of</strong> highpressure. For example, phosphorus appears to be theType 1 element with the highest Tc. But, it requirescompression pressures <strong>of</strong> 2.5 Mbar to reach a Tc <strong>of</strong>22 K (-251ºC).Type I <strong>superconductors</strong> are very pure metals thattypically have critical fields too low for use insuperconducting magnets.Type 2 <strong>superconductors</strong>Superconductors made from metallic compounds<strong>and</strong> alloys are called Type 2 <strong>superconductors</strong>. <strong>The</strong>recently-discovered superconducting "perovskites"(metal-oxide ceramics that normally have a ratio <strong>of</strong> 2metal atoms to every 3 oxygen atoms) belong to thisType 2 group. Besides being mechanically harderthan Type 1 <strong>superconductors</strong>, they exhibit muchhigher critical magnetic fields <strong>and</strong> higher Tc's thanType 1 <strong>superconductors</strong> by a mechanism that is stillnot completely understood.Type 2 <strong>superconductors</strong> - also known as the "hard"or high temperature <strong>superconductors</strong> - differ fromType 1 in that their transition from a normal to asuperconducting state is gradual across a region <strong>of</strong>"mixed state" behavior. Since a Type 2 will allowsome penetration by an external magnetic field intoits surface, this creates some rather novelmacroscopic phenomena where superconductorusually exist in a mixed state <strong>of</strong> normal <strong>and</strong>superconducting regions.Fig. 10. Mixed state <strong>of</strong> type 2 superconductor.This is sometimes called a vortex state, becausevortices <strong>of</strong> superconducting currents surround cores<strong>of</strong> normal material. As their critical temperatures areapproached, the normal cores are more closelypacked <strong>and</strong> eventually overlap as thesuperconducting state is lost. A size <strong>of</strong> about 300 nmis typical for the normal cores. While the Meissnereffect is modified to allow magnetic fields throughthe normal cores, magnetic fields are still excludedfrom the superconducting regions.<strong>The</strong> superconducting cuprates (copper-oxides) haveachieved astonishingly high Tc's when consideredthat by 1985 known Tc's had only reached 23 K forType 1. To date, the highest Tc attained at ambientpressure has been 138 K (-135ºC) <strong>and</strong> is held by athallium-doped, mercuric-cuprate comprised <strong>of</strong> theelements Mercury, Thallium, Barium, Calcium,Copper <strong>and</strong> Oxygen.One theory predicts an upper limit <strong>of</strong> about 200 Kfor the layered cuprates (Vladimir Kresin, Phys.1997). Others assert there is no limit. Either way, itis almost certain that other, more-synergisticcompounds still await discovery among the hightemperature<strong>superconductors</strong>.Atypical <strong>superconductors</strong>In 1986 a breakthrough discovery was made in thefield <strong>of</strong> <strong>superconductivity</strong>. Alex Müller <strong>and</strong> GeorgBednorz created a brittle ceramic compound thatsuperconducted at the highest temperature thenknown: 30 K (-243ºC). What made this discovery soremarkable was that ceramics are normallyinsulators. <strong>The</strong> Lanthanum, Barium, Copper <strong>and</strong>Oxygen compound that Müller <strong>and</strong> Bednorzsynthesized, behaved in a not-as-yet-understoodway.Organic <strong>superconductors</strong> are part <strong>of</strong> the organicconductor family which includes: molecular salts,polymers <strong>and</strong> pure carbon systems. Since these Tc'sare in the range <strong>of</strong> Type 1 <strong>superconductors</strong>,engineers have not yet found a practical applicationfor them. However, their rather unusual propertieshave made them the focus <strong>of</strong> intense research. <strong>The</strong>seproperties include giant magnetoresistance, rapidoscillations, quantum hall effect, <strong>and</strong> more.Discovered in 1993 by Bob Cava, borocarbides areone <strong>of</strong> the least-understood superconductor systems <strong>of</strong> all.It has always been assumed that <strong>superconductors</strong>cannot be formed from ferromagnetic transitionmetals - like iron, cobalt or nickel. It's the equivalent<strong>of</strong> trying to mix oil <strong>and</strong> water. However, in someborocarbides there is a "soap" that acts to bring theseadversaries together. Another not understoodphenomenon is that below Tc, where it shouldremain superconductive, there is a discordanttemperature at which the material retreats to a"normal", non-superconductive state.<strong>The</strong> Heavy Fermions are yet another example <strong>of</strong>atypical <strong>superconductors</strong>. Heavy fermions arecompounds containing rare-earth elements such asCe or Yb, or actinide elements such as U. <strong>The</strong>irconduction electrons <strong>of</strong>ten have effective massesseveral hundred times as great as that <strong>of</strong> "normal"electrons, resulting in what's known as low "Fermienergy". This makes them reluctant <strong>superconductors</strong>.Some <strong>of</strong> those materials display <strong>superconductivity</strong>through a mechanism that quickly runs afoul <strong>of</strong> BCStheory. Research suggests cooper-pairing in theheavy fermion systems arises from the magneticinteractions <strong>of</strong> the electron spins, rather than bylattice vibrations.In 1997 researchers discovered that at a temperaturevery near absolute zero an alloy <strong>of</strong> gold <strong>and</strong> indiumwas both a superconductor <strong>and</strong> a natural magnet.Conventional wisdom held that a material with suchproperties could not exist!In June 1999 New Zeal<strong>and</strong> researcher Dr. Tallon <strong>and</strong>Dr. Bernard discovered a ruthenium-cuprate whose136

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