Superconductivity

<h2 id="history">History</h2>
Main article: <a href="/facts/History_of_superconductivity/wHsHnXKN">History of superconductivity</a>

Superconductivity was discovered on April 8, 1911, by Heike Kamerlingh Onnes, who was studying the resistance of solid mercury at <a href="/facts/Cryogenic/cw7dHAkp">cryogenic</a> temperatures using the recently produced <a href="/facts/Liquid_helium/JYXCAcDf">liquid helium</a> as a <a href="/facts/Refrigerant/rI60t5zU">refrigerant</a>.<a class="footnote-ref" id="fnref:8" href="#fn:8">8</a> At the temperature of 4.2 K, he observed that the resistance abruptly disappeared.<a class="footnote-ref" id="fnref:9" href="#fn:9">9</a> In the same experiment, he also observed the <a href="/facts/Superfluid/QuePDujN">superfluid</a> transition of helium at 2.2 K, without recognizing its significance. The precise date and circumstances of the discovery were only reconstructed a century later, when Onnes's notebook was found.<a class="footnote-ref" id="fnref:10" href="#fn:10">10</a> In subsequent decades, superconductivity was observed in several other materials. In 1913, <a href="/facts/Lead/EYljasJN">lead</a> was found to superconduct at 7 K, and in 1941 <a href="/facts/Niobium_nitride/ufUqc2N7">niobium nitride</a> was found to superconduct at 16 K.
Great efforts have been devoted to finding out how and why superconductivity works; the important step occurred in 1933, when <a href="/facts/Walther_Meissner/0QI9HA63">Meissner</a> and <a href="/facts/Robert_Ochsenfeld/smM2Yh9D">Ochsenfeld</a> discovered that superconductors expelled applied magnetic fields, a phenomenon which has come to be known as the Meissner effect.<a class="footnote-ref" id="fnref:11" href="#fn:11">11</a> In 1935, <a href="/facts/Fritz_London/9NvJ4MR7">Fritz</a> and <a href="/facts/Heinz_London/TMhHQxbe">Heinz London</a> showed that the Meissner effect was a consequence of the minimization of the electromagnetic <a href="/facts/Thermodynamic_free_energy/GtjtQqnq">free energy</a> carried by superconducting current.<a class="footnote-ref" id="fnref:12" href="#fn:12">12</a>

<h3>London constitutive equations</h3>
The theoretical model that was first conceived for superconductivity was completely classical: it is summarized by <a href="/facts/London_equations/d2T2FSAK">London constitutive equations</a>. It was put forward by the brothers Fritz and Heinz London in 1935, shortly after the discovery that magnetic fields are expelled from superconductors. A major triumph of the equations of this theory is their ability to explain the Meissner effect,<a class="footnote-ref" id="fnref:13" href="#fn:13">13</a> wherein a material exponentially expels all internal magnetic fields as it crosses the superconducting threshold. By using the London equation, one can obtain the dependence of the magnetic field inside the superconductor on the distance to the surface.<a class="footnote-ref" id="fnref:14" href="#fn:14">14</a>
The two constitutive equations for a superconductor by London are:

 
 
 
 
 
 
 ∂
 
 j
 
 
 
 ∂
 t
 
 
 
 =
 
 
 
 n
 
 e
 
 2
 
 
 
 m
 
 
 
 E
 
 ,
 
 
 ∇
 
 ×
 
 j
 
 =
 −
 
 
 
 n
 
 e
 
 2
 
 
 
 m
 
 
 
 B
 
 .
 
 
 {\displaystyle {\frac {\partial \mathbf {j} }{\partial t}}={\frac {ne^{2}}{m}}\mathbf {E} ,\qquad \mathbf {\nabla } \times \mathbf {j} =-{\frac {ne^{2}}{m}}\mathbf {B} .}

The first equation follows from <a href="/facts/Newton%2527s_second_law/XKzGTXK1">Newton's second law</a> for superconducting electrons.

<h3>Conventional theories (1950s)</h3>
During the 1950s, theoretical <a href="/facts/Condensed_matter_physics/EBVI5nmL">condensed matter</a> physicists arrived at an understanding of "conventional" superconductivity, through a pair of remarkable and important theories: the phenomenological <a href="/facts/Ginzburg%25E2%2580%2593Landau_theory/VAHPgSzY">Ginzburg–Landau theory</a> (1950) and the microscopic BCS theory (1957).<a class="footnote-ref" id="fnref:15" href="#fn:15">15</a><a class="footnote-ref" id="fnref:16" href="#fn:16">16</a>
In 1950, the <a href="/facts/Phenomenology_(particle_physics)/390KC4vG">phenomenological</a> <a href="/facts/Ginzburg%25E2%2580%2593Landau_theory/VAHPgSzY">Ginzburg–Landau theory</a> of superconductivity was devised by <a href="/facts/Lev_Landau/lNXQTC49">Landau</a> and <a href="/facts/Vitaly_Ginzburg/uscYaLgY">Ginzburg</a>.<a class="footnote-ref" id="fnref:17" href="#fn:17">17</a> This theory, which combined Landau's theory of second-order phase transitions with a <a href="/facts/Schr%25C3%25B6dinger_equation/3csgSIWF">Schrödinger</a>-like wave equation, had great success in explaining the macroscopic properties of superconductors. In particular, <a href="/facts/Alexei_Alexeyevich_Abrikosov/I4Gwb0yB">Abrikosov</a> showed that Ginzburg–Landau theory predicts the division of superconductors into the two categories now referred to as Type I and Type II. Abrikosov and Ginzburg were awarded the 2003 Nobel Prize for their work (Landau had received the 1962 Nobel Prize for other work, and died in 1968). The four-dimensional extension of the Ginzburg–Landau theory, the <a href="/facts/Coleman%25E2%2580%2593Weinberg_potential/YGcUHdX5">Coleman-Weinberg model</a>, is important in <a href="/facts/Quantum_field_theory/VoewsNJV">quantum field theory</a> and <a href="/facts/Cosmology/yM19zM7Y">cosmology</a>.
Also in 1950, Maxwell and Reynolds et al. found that the critical temperature of a superconductor depends on the <a href="/facts/Isotope/KD9B1y6o">isotopic mass</a> of the constituent element.<a class="footnote-ref" id="fnref:18" href="#fn:18">18</a><a class="footnote-ref" id="fnref:19" href="#fn:19">19</a> This important discovery pointed to the <a href="/facts/Electron/L0KBo5cW">electron</a>–<a href="/facts/Phonon/tflWW6vw">phonon</a> interaction as the microscopic mechanism responsible for superconductivity.
The complete microscopic theory of superconductivity was finally proposed in 1957 by <a href="/facts/John_Bardeen/kbj763Fh">Bardeen</a>, <a href="/facts/Leon_Neil_Cooper/058c4ER2">Cooper</a> and <a href="/facts/John_Robert_Schrieffer/DfX8s90T">Schrieffer</a>.<a class="footnote-ref" id="fnref:20" href="#fn:20">20</a> This BCS theory explained the superconducting current as a superfluid of Cooper pairs, pairs of electrons interacting through the exchange of phonons. For this work, the authors were awarded the Nobel Prize in 1972.
The BCS theory was set on a firmer footing in 1958, when <a href="/facts/N._N._Bogolyubov/39w1trXl">N. N. Bogolyubov</a> showed that the BCS wavefunction, which had originally been derived from a variational argument, could be obtained using a canonical transformation of the electronic <a href="/facts/Hamiltonian_(quantum_mechanics)/5XwK2HmD">Hamiltonian</a>.<a class="footnote-ref" id="fnref:21" href="#fn:21">21</a> In 1959, <a href="/facts/Lev_Gor%2527kov/9UC3v2CU">Lev Gor'kov</a> showed that the BCS theory reduced to the Ginzburg–Landau theory close to the critical temperature.<a class="footnote-ref" id="fnref:22" href="#fn:22">22</a><a class="footnote-ref" id="fnref:23" href="#fn:23">23</a>
Generalizations of BCS theory for conventional superconductors form the basis for the understanding of the phenomenon of <a href="/facts/Superfluidity/QuePDujN">superfluidity</a>, because they fall into the <a href="/facts/Lambda_transition/2b2LSW3y">lambda transition</a> universality class. The extent to which such generalizations can be applied to <a href="/facts/Unconventional_superconductor/smImcsMy">unconventional superconductors</a> is still controversial.

<h3>Niobium</h3>
The first practical application of superconductivity was developed in 1954 with <a href="/facts/Dudley_Allen_Buck/ocANH3uL">Dudley Allen Buck</a>'s invention of the <a href="/facts/Cryotron/dgKtPUaN">cryotron</a>.<a class="footnote-ref" id="fnref:24" href="#fn:24">24</a> Two superconductors with greatly different values of the critical magnetic field are combined to produce a fast, simple switch for computer elements.
Soon after discovering superconductivity in 1911, Kamerlingh Onnes attempted to make an electromagnet with superconducting windings but found that relatively low magnetic fields destroyed superconductivity in the materials he investigated. Much later, in 1955, G. B. Yntema<a class="footnote-ref" id="fnref:25" href="#fn:25">25</a> succeeded in constructing a small 0.7-tesla iron-core electromagnet with superconducting niobium wire windings. Then, in 1961, <a href="/facts/John_Eugene_Kunzler/XTvmw2d8">J. E. Kunzler</a>, E. Buehler, F. S. L. Hsu, and J. H. Wernick<a class="footnote-ref" id="fnref:26" href="#fn:26">26</a> made the startling discovery that, at 4.2 kelvin, <a href="/facts/Niobium%25E2%2580%2593tin/QnRWPr70">niobium–tin</a>, a compound consisting of three parts niobium and one part tin, was capable of supporting a current density of more than 100,000 amperes per square centimeter in a magnetic field of 8.8 tesla. The alloy was brittle and difficult to fabricate, but niobium–tin proved useful for generating magnetic fields as high as 20 tesla.
In 1962, T. G. Berlincourt and R. R. Hake<a class="footnote-ref" id="fnref:27" href="#fn:27">27</a><a class="footnote-ref" id="fnref:28" href="#fn:28">28</a> discovered that more ductile alloys of niobium and titanium are suitable for applications up to 10 tesla. Commercial production of <a href="/facts/Niobium%25E2%2580%2593titanium/FXMYDvaW">niobium–titanium</a> supermagnet wire immediately commenced at <a href="/facts/Westinghouse_Electric_Corporation/Nln2BzI3">Westinghouse Electric Corporation</a> and at <a href="/facts/Wah_Chang_Corporation/YK7WR2sY">Wah Chang Corporation</a>. Although niobium–titanium boasts less-impressive superconducting properties than those of niobium–tin, niobium–titanium became the most widely used "workhorse" supermagnet material, in large measure a consequence of its very high <a href="/facts/Ductility/SBJsahEk">ductility</a> and ease of fabrication. However, both niobium–tin and niobium–titanium found wide application in MRI medical imagers, bending and focusing magnets for enormous high-energy-particle accelerators, and other applications. Conectus, a European superconductivity consortium, estimated that in 2014, global economic activity for which superconductivity was indispensable amounted to about five billion euros, with MRI systems accounting for about 80% of that total.

<h3>Josephson effect</h3>
In 1962, <a href="/facts/Brian_David_Josephson/GG07CsRp">Josephson</a> made the important theoretical prediction that a supercurrent can flow between two pieces of superconductor separated by a thin layer of insulator.<a class="footnote-ref" id="fnref:29" href="#fn:29">29</a> This phenomenon, now called the <a href="/facts/Josephson_effect/2fvcdS8N">Josephson effect</a>, is exploited by superconducting devices such as <a href="/facts/SQUID/2FEvJ5wG">SQUIDs</a>. It is used in the most accurate available measurements of the <a href="/facts/Magnetic_flux_quantum/ywtHmBQW">magnetic flux quantum</a> Φ0 = h/(2e), where h is the <a href="/facts/Planck_constant/qGHAe3qq">Planck constant</a>. Coupled with the <a href="/facts/Quantum_Hall_effect/yK3zcCgu">quantum Hall resistivity</a>, this leads to a precise measurement of the Planck constant. Josephson was awarded the Nobel Prize for this work in 1973.<a class="footnote-ref" id="fnref:30" href="#fn:30">30</a>
In 2008, it was proposed that the same mechanism that produces superconductivity could produce a <a href="/facts/Superinsulator/oX9Baa9h">superinsulator</a> state in some materials, with almost infinite <a href="/facts/Electrical_resistance/hxSt0UAj">electrical resistance</a>.<a class="footnote-ref" id="fnref:31" href="#fn:31">31</a> The first development and study of superconducting <a href="/facts/Bose%25E2%2580%2593Einstein_condensate/76peCwfW">Bose–Einstein condensate</a> (BEC) in 2020 suggested a "smooth transition between" BEC and <a href="/facts/BCS_theory/KmlyhxPS">Bardeen-Cooper-Shrieffer</a> regimes.<a class="footnote-ref" id="fnref:32" href="#fn:32">32</a><a class="footnote-ref" id="fnref:33" href="#fn:33">33</a>

<h3>2D materials</h3>
Multiple types of superconductivity are reported in devices made of <a href="/facts/Single-layer_materials/YnsFhbWg">single-layer materials</a>. Some of these materials can switch between conducting, insulating, and other behaviors.<a class="footnote-ref" id="fnref:34" href="#fn:34">34</a>
Twisting materials imbues them with a “<a href="/facts/Moir%25C3%25A9/nvxDu1qK">moiré</a>” pattern involving tiled hexagonal cells that act like atoms and host electrons. In this environment, the electrons move slowly enough for their collective interactions to guide their behavior. When each cell has a single electron, the electrons take on an antiferromagnetic arrangement; each electron can have a preferred location and magnetic orientation. Their intrinsic magnetic fields tend to alternate between pointing up and down. Adding electrons allows superconductivity by causing Cooper pairs to form. Fu and Schrade argued that electron-on-electron action was allowing both antiferromagnetic and superconducting states.<a class="footnote-ref" id="fnref:35" href="#fn:35">35</a>
The first success with 2D materials involved a twisted bilayer graphene sheet (2018, Tc ~1.7 K, 1.1° twist). A twisted three-layer graphene device was later shown to superconduct (2021, Tc ~2.8 K). Then an untwisted trilayer graphene device was reported to superconduct (2022, Tc 1-2 K). The latter was later shown to be tunable, easily reproducing behavior found in millions of other configurations. Directly observing what happens when electrons are added to a material or slightly weakening its electric field enables quick testing of an unprecedented number of recipes to see which lead to superconductivity.<a class="footnote-ref" id="fnref:36" href="#fn:36">36</a>
In four and five layer rhombohedral graphene, a form of superconductivity with spontaneously broken <a href="/facts/Time_reversal_symmetry/Tgf2LJMc">time reversal symmetry</a> known as "chiral superconductivity" was recently observed.<a class="footnote-ref" id="fnref:37" href="#fn:37">37</a>. These systems were not observed to have any superlattice effects, and they can flip between two possible magnetic states without exiting the superconducting phase.<a class="footnote-ref" id="fnref:38" href="#fn:38">38</a>. This is in strong contrast to other observations of superconductivity and magnetic fields. 
These devices have applications in <a href="/facts/Quantum_computing/nbbcgmvq">quantum computing</a>.
2D materials other than graphene have also been made to superconduct. <a href="/facts/Transition_metal_dichalcogenides/GTXXbDoV">Transition metal dichalcogenide</a> (TMD) sheets twisted at 5 degrees intermittently achieved superconduction by creating a Josephson junction. The device used used thin layers of <a href="/facts/Palladium/P7y0ESWf">palladium</a> to connect to the sides of a <a href="/facts/Tungsten_telluride/45R0wxMD">tungsten telluride</a> layer surrounded and protected by <a href="/facts/Boron_nitride/kumlPQRg">boron nitride</a>.<a class="footnote-ref" id="fnref:39" href="#fn:39">39</a> Another group demonstrated superconduction in <a href="/facts/Molybdenum_telluride/yYSrXn80">molybdenum telluride</a> (MoTe₂) in 2D <a href="/facts/Van_der_Waals_molecule/qcmsRbu0">van der Waals</a> materials using ferroelectric domain walls. The Tc was implied to be higher than typical TMDs (~5–10 K).<a class="footnote-ref" id="fnref:40" href="#fn:40">40</a>
A Cornell group added a 3.5-degree twist to an insulator that allowed electrons to slow down and interact strongly, leaving one electron per cell, exhibiting superconduction. Existing theories do not explain this behavior.
Fu and collaborators proposed that electrons arrange to form a repeating crystal that allows the electron grid to float independently of the background atomic nuclei and the electron grid to relax. Its ripples pair electrons the way phonons do, although this is unconfirmed.

<h2 id="classification">Classification</h2>
Main article: <a href="/facts/Superconductor_classification/rF31szzb">Superconductor classification</a>
Superconductors are classified according to many criteria. The most common are:

<h3>Response to a magnetic field</h3>
A superconductor can be <a href="/facts/Type_I_superconductor/xsosaCVK">Type I</a>, meaning it has a single <a href="/facts/Critical_field/z4rEQR1f">critical field</a>, above which superconductivity is lost and below which the magnetic field is completely expelled from the superconductor; or <a href="/facts/Type_II_superconductor/8V4UTGjY">Type II</a>, meaning it has two critical fields, between which it allows partial penetration of the magnetic field through isolated points<a class="footnote-ref" id="fnref:41" href="#fn:41">41</a> called <a href="/facts/Quantum_vortex/0Tzjncgk">vortices</a>.<a class="footnote-ref" id="fnref:42" href="#fn:42">42</a> Furthermore, in multicomponent superconductors it is possible to combine the two behaviours. In that case the superconductor is of <a href="/facts/Type-1.5_superconductor/LJBq6HWq">Type-1.5</a>.<a class="footnote-ref" id="fnref:43" href="#fn:43">43</a>

<h3>Theory of operation</h3>
A superconductor is <a href="/facts/Conventional_superconductor/9P4nzxyJ">conventional</a> if it is driven by electron–phonon interaction and explained by the <a href="/facts/BCS_theory/KmlyhxPS">BCS theory</a> or its extension, the Eliashberg theory. Otherwise, it is <a href="/facts/Unconventional_superconductor/smImcsMy">unconventional</a>.<a class="footnote-ref" id="fnref:44" href="#fn:44">44</a><a class="footnote-ref" id="fnref:45" href="#fn:45">45</a> Alternatively, a superconductor is called unconventional if the superconducting <a href="/facts/Order_parameter/eLP2BY8R">order parameter</a> transforms according to a non-trivial <a href="/facts/Irreducible_representation/Hu5geBgk">irreducible representation</a> of the system's <a href="/facts/Point_group/41NSqUN6">point group</a> or <a href="/facts/Space_group/2XQx0J7M">space group</a>.<a class="footnote-ref" id="fnref:46" href="#fn:46">46</a>

<h3>Critical temperature</h3>
A superconductor is generally considered <a href="/facts/High-temperature_superconductivity/MXtx2gvV">high-temperature</a> if it reaches a superconducting state above a temperature of 30 K (−243.15 °C);<a class="footnote-ref" id="fnref:47" href="#fn:47">47</a> as in the initial discovery by <a href="/facts/Georg_Bednorz/p14P6Sy6">Georg Bednorz</a> and <a href="/facts/K._Alex_M%25C3%25BCller/89oyE7oM">K. Alex Müller</a>.<a class="footnote-ref" id="fnref:48" href="#fn:48">48</a> It may also reference materials that transition to superconductivity when cooled using <a href="/facts/Liquid_nitrogen/IGWI1h00">liquid nitrogen</a> – that is, at only Tc > 77 K, although this is generally used only to emphasize that liquid nitrogen coolant is sufficient. Low temperature superconductors refer to materials with a critical temperature below 30 K, and are cooled mainly by <a href="/facts/Liquid_helium/JYXCAcDf">liquid helium</a> (Tc > 4.2 K). One exception to this rule is the <a href="/facts/Iron-based_superconductor/SCoUWGmS">iron pnictide</a> group of superconductors that display behaviour and properties typical of high-temperature superconductors, yet some of the group have critical temperatures below 30 K.

<h3>Material</h3>

Superconductor material classes include <a href="/facts/Chemical_element/0jducgWD">chemical elements</a> (e.g. <a href="/facts/Mercury_(element)/WlxfoHva">mercury</a> or <a href="/facts/Lead/EYljasJN">lead</a>), <a href="/facts/Alloy/I7w7WQWR">alloys</a> (such as <a href="/facts/Niobium%25E2%2580%2593titanium/FXMYDvaW">niobium–titanium</a>, <a href="/facts/Germanium%25E2%2580%2593niobium/wIX4mRPu">germanium–niobium</a>, and <a href="/facts/Niobium_nitride/ufUqc2N7">niobium nitride</a>), <a href="/facts/Ceramic/9JKudpqX">ceramics</a> (<a href="/facts/YBCO/hkFJMegk">YBCO</a> and <a href="/facts/Magnesium_diboride/fsgNsNPP">magnesium diboride</a>), <a href="/facts/Iron-based_superconductor/SCoUWGmS">superconducting pnictides</a> (like fluorine-doped LaOFeAs), <a href="/facts/Single-layer_materials/YnsFhbWg">single-layer materials</a> such as <a href="/facts/Graphene/QDGUBaPt">graphene</a> and <a href="/facts/Chalcogenide/GTXXbDoV">transition metal dichalcogenides</a>,<a class="footnote-ref" id="fnref:49" href="#fn:49">49</a> or <a href="/facts/Organic_superconductor/Dk0Yv6wc">organic superconductors</a> (<a href="/facts/Fullerene/LPdnl8ox">fullerenes</a> and <a href="/facts/Carbon_nanotube/atuDPPaG">carbon nanotubes</a>; though perhaps these examples should be included among the chemical elements, as they are composed entirely of <a href="/facts/Carbon/ukrgQexo">carbon</a>).<a class="footnote-ref" id="fnref:50" href="#fn:50">50</a><a class="footnote-ref" id="fnref:51" href="#fn:51">51</a>

<h2 id="elementary-properties">Elementary properties</h2>

Several physical properties of superconductors vary from material to material, such as the critical temperature, the value of the <a href="/facts/Energy_gap/VMvKsyna">superconducting gap</a>, the critical magnetic field, and the critical current density at which superconductivity is destroyed. On the other hand, there is a class of properties that are independent of the underlying material. The Meissner effect, the quantization of the <a href="/facts/Magnetic_flux_quantum/ywtHmBQW">magnetic flux</a> or permanent currents, i.e. the state of zero resistance are the most important examples. The existence of these "universal" properties is rooted in the nature of the <a href="/facts/Symmetry_breaking/q3yqVlNQ">broken symmetry</a> of the superconductor and the emergence of off-diagonal long range order. Superconductivity is a <a href="/facts/Phase_(matter)/NkHXDdN3">thermodynamic phase</a>, and thus possesses certain distinguishing properties which are largely independent of microscopic details. Off diagonal long range order is closely connected to the formation of <a href="/facts/Cooper_pair/uHILVyXu">Cooper pairs</a>.

<h3>Zero electrical DC resistance</h3>

The simplest method to measure the <a href="/facts/Electrical_resistance/hxSt0UAj">electrical resistance</a> of a sample of some material is to place it in an <a href="/facts/Electrical_circuit/zt94kTW0">electrical circuit</a> in series with a <a href="/facts/Current_source/1UkYH0aG">current source</a> I and measure the resulting <a href="/facts/Voltage/EN2po6N2">voltage</a> V across the sample. The resistance of the sample is given by <a href="/facts/Ohm%2527s_law/PjfEyTgI">Ohm's law</a> as R = V / I. If the voltage is zero, this means that the resistance is zero.
Superconductors are also able to maintain a current with no applied voltage whatsoever, a property exploited in <a href="/facts/Superconducting_magnet/bRWH01s5">superconducting electromagnets</a> such as those found in <a href="/facts/Magnetic_resonance_imaging/Vh9yG9qq">MRI</a> machines. Experiments have demonstrated that currents in superconducting coils can persist for years without any measurable degradation. Experimental evidence points to a lifetime of at least 100,000 years. Theoretical estimates for the lifetime of a persistent current can exceed the estimated lifetime of the universe, depending on the wire geometry and the temperature.<a class="footnote-ref" id="fnref:52" href="#fn:52">52</a> In practice, currents injected in superconducting coils persisted for 28 years, 7 months, 27 days in a superconducting gravimeter in Belgium, from August 4, 1995 until March 31, 2024.<a class="footnote-ref" id="fnref:53" href="#fn:53">53</a><a class="footnote-ref" id="fnref:54" href="#fn:54">54</a> In such instruments, the measurement is based on the monitoring of the levitation of a superconducting niobium sphere with a mass of four grams.
In a normal conductor, an electric current may be visualized as a fluid of <a href="/facts/Electron/L0KBo5cW">electrons</a> moving across a heavy ionic lattice. The electrons are constantly colliding with the ions in the lattice, and during each collision some of the energy carried by the current is absorbed by the lattice and converted into <a href="/facts/Heat/e9QqQ0B2">heat</a>, which is essentially the vibrational <a href="/facts/Kinetic_energy/aJRxUd4p">kinetic energy</a> of the lattice ions. As a result, the energy carried by the current is constantly being dissipated. This is the phenomenon of electrical resistance and <a href="/facts/Joule_heating/eANEHVzP">Joule heating</a>.
The situation is different in a superconductor. In a conventional superconductor, the electronic fluid cannot be resolved into individual electrons. Instead, it consists of bound pairs of electrons known as <a href="/facts/Cooper_pair/uHILVyXu">Cooper pairs</a>. This pairing is caused by an attractive force between electrons from the exchange of <a href="/facts/Phonon/tflWW6vw">phonons</a>. This pairing is very weak, and small thermal vibrations can fracture the bond. Due to <a href="/facts/Quantum_mechanics/BRc3Mzgr">quantum mechanics</a>, the <a href="/facts/Energy_spectrum/wPUjkpqI">energy spectrum</a> of this Cooper pair fluid possesses an <a href="/facts/Energy_gap/VMvKsyna">energy gap</a>, meaning there is a minimum amount of energy ΔE that must be supplied in order to excite the fluid. Therefore, if ΔE is larger than the <a href="/facts/Thermal_energy/eVaKAC7K">thermal energy</a> of the lattice, given by kT, where k is the <a href="/facts/Boltzmann_constant/5DIejyR3">Boltzmann constant</a> and T is the <a href="/facts/Temperature/QyGe4gmj">temperature</a>, the fluid will not be scattered by the lattice.<a class="footnote-ref" id="fnref:55" href="#fn:55">55</a> The Cooper pair fluid is thus a <a href="/facts/Superfluid/QuePDujN">superfluid</a>, meaning it can flow without energy dissipation.
In the class of superconductors known as <a href="/facts/Type_II_superconductor/8V4UTGjY">type II superconductors</a>, including all known <a href="/facts/High-temperature_superconductor/MXtx2gvV">high-temperature superconductors</a>, an extremely low but non-zero resistivity appears at temperatures not too far below the nominal superconducting transition when an electric current is applied in conjunction with a strong magnetic field, which may be caused by the electric current. This is due to the motion of <a href="/facts/Abrikosov_vortex/6yP83ySP">magnetic vortices</a> in the electronic superfluid, which dissipates some of the energy carried by the current. If the current is sufficiently small, the vortices are stationary, and the resistivity vanishes. The resistance due to this effect is minuscule compared with that of non-superconducting materials, but must be taken into account in sensitive experiments. However, as the temperature decreases far enough below the nominal superconducting transition, these vortices can become frozen into a disordered but stationary phase known as a "vortex glass". Below this vortex glass transition temperature, the resistance of the material becomes truly zero.

<h3>Phase transition</h3>

In superconducting materials, the characteristics of superconductivity appear when the temperature T is lowered below a critical temperature Tc. The value of this critical temperature varies from material to material. Conventional superconductors usually have critical temperatures ranging from around 20 <a href="/facts/Kelvin/E3trzC4C">K</a> to less than 1 K. Solid <a href="/facts/Mercury_(element)/WlxfoHva">mercury</a>, for example, has a critical temperature of 4.2 K. As of 2015, the highest critical temperature found for a conventional superconductor is 203 K for H2S, although high pressures of approximately 90 gigapascals were required.<a class="footnote-ref" id="fnref:56" href="#fn:56">56</a> <a href="/facts/Cuprate_superconductor/U0MqqhnQ">Cuprate superconductors</a> can have much higher critical temperatures: <a href="/facts/YBCO/hkFJMegk">YBa2Cu3O7</a>, one of the first cuprate superconductors to be discovered, has a critical temperature above 90 K, and mercury-based cuprates have been found with critical temperatures in excess of 130 K. The basic physical mechanism responsible for the high critical temperature is not yet clear. However, it is clear that a two-electron pairing is involved, although the nature of the pairing (
 
 
 
 s
 
 
 {\displaystyle s}
 
 wave vs. 
 
 
 
 d
 
 
 {\displaystyle d}
 
 wave) remains controversial.<a class="footnote-ref" id="fnref:57" href="#fn:57">57</a>
Similarly, at a fixed temperature below the critical temperature, superconducting materials cease to superconduct when an external <a href="/facts/Magnetic_field/Ta8Ev588">magnetic field</a> is applied which is greater than the critical magnetic field. This is because the <a href="/facts/Gibbs_free_energy/bvenDuzh">Gibbs free energy</a> of the superconducting phase increases quadratically with the magnetic field while the free energy of the normal phase is roughly independent of the magnetic field. If the material superconducts in the absence of a field, then the superconducting phase free energy is lower than that of the normal phase and so for some finite value of the magnetic field (proportional to the square root of the difference of the free energies at zero magnetic field) the two free energies will be equal and a phase transition to the normal phase will occur. More generally, a higher temperature and a stronger magnetic field lead to a smaller fraction of electrons that are superconducting and consequently to a longer <a href="/facts/London_penetration_depth/lTmmbTS0">London penetration depth</a> of external magnetic fields and currents. The penetration depth becomes infinite at the phase transition.
The onset of superconductivity is accompanied by abrupt changes in various physical properties, which is the hallmark of a <a href="/facts/Phase_transition/eLP2BY8R">phase transition</a>. For example, the electronic <a href="/facts/Heat_capacity/I63nzSyp">heat capacity</a> is proportional to the temperature in the normal (non-superconducting) regime. At the superconducting transition, it suffers a discontinuous jump and thereafter ceases to be linear. At low temperatures, it varies instead as e−α/T for some constant, α. This exponential behavior is one of the pieces of evidence for the existence of the <a href="/facts/Energy_gap/VMvKsyna">energy gap</a>.
The <a href="/facts/Second-order_transition/eLP2BY8R">order</a> of the superconducting <a href="/facts/Phase_transition/eLP2BY8R">phase transition</a> was long a matter of debate. Experiments indicate that the transition is second-order, meaning there is no <a href="/facts/Latent_heat/QCIWSGln">latent heat</a>. However, in the presence of an external magnetic field there is latent heat, because the superconducting phase has a lower entropy below the critical temperature than the normal phase. It has been experimentally demonstrated<a class="footnote-ref" id="fnref:58" href="#fn:58">58</a> that, as a consequence, when the magnetic field is increased beyond the critical field, the resulting phase transition leads to a decrease in the temperature of the superconducting material.
Calculations in the 1970s suggested that it may actually be weakly first-order due to the effect of long-range fluctuations in the electromagnetic field. In the 1980s it was shown theoretically with the help of a disorder field theory, in which the <a href="/facts/Vortex_line/2oQ6eT4d">vortex lines</a> of the superconductor play a major role, that the transition is of second order within the <a href="/facts/Type-II_superconductor/8V4UTGjY">type II</a> regime and of first order (i.e., <a href="/facts/Latent_heat/QCIWSGln">latent heat</a>) within the <a href="/facts/Type-I_superconductor/xsosaCVK">type I</a> regime, and that the two regions are separated by a <a href="/facts/Tricritical_point/DVLLRYNL">tricritical point</a>.<a class="footnote-ref" id="fnref:59" href="#fn:59">59</a> The results were strongly supported by Monte Carlo computer simulations.<a class="footnote-ref" id="fnref:60" href="#fn:60">60</a>

<h3>Meissner effect</h3>
Main article: <a href="/facts/Meissner_effect/VJLdDzzE">Meissner effect</a>

When a superconductor is placed in a weak external magnetic field H, and cooled below its transition temperature, the magnetic field is ejected. The Meissner effect does not cause the field to be completely ejected but instead, the field penetrates the superconductor but only to a very small distance, characterized by a parameter λ, called the <a href="/facts/London_penetration_depth/lTmmbTS0">London penetration depth</a>, decaying exponentially to zero within the bulk of the material. The Meissner effect is a defining characteristic of superconductivity. For most superconductors, the London penetration depth is on the order of 100 nm.
The Meissner effect is sometimes confused with the kind of <a href="/facts/Diamagnetism/dgFavn9K">diamagnetism</a> one would expect in a perfect electrical conductor: according to <a href="/facts/Lenz%2527s_law/8Atydpcb">Lenz's law</a>, when a changing magnetic field is applied to a conductor, it will induce an electric current in the conductor that creates an opposing magnetic field. In a perfect conductor, an arbitrarily large current can be induced, and the resulting magnetic field exactly cancels the applied field.
The Meissner effect is distinct from this – it is the spontaneous expulsion that occurs during transition to superconductivity. Suppose we have a material in its normal state, containing a constant internal magnetic field. When the material is cooled below the critical temperature, we would observe the abrupt expulsion of the internal magnetic field, which we would not expect based on Lenz's law.
The Meissner effect was given a phenomenological explanation by the brothers <a href="/facts/Fritz_London/9NvJ4MR7">Fritz</a> and <a href="/facts/Heinz_London/TMhHQxbe">Heinz London</a>, who showed that the electromagnetic <a href="/facts/Thermodynamic_free_energy/GtjtQqnq">free energy</a> in a superconductor is minimized provided 
 
 
 
 
 ∇
 
 2
 
 
 
 H
 
 =
 
 λ
 
 −
 2
 
 
 
 H
 
 
 
 
 {\displaystyle \nabla ^{2}\mathbf {H} =\lambda ^{-2}\mathbf {H} \,}
 
 where H is the magnetic field and λ is the London penetration depth.
This equation, which is known as the <a href="/facts/London_equation/d2T2FSAK">London equation</a>, predicts that the magnetic field in a superconductor <a href="/facts/Exponential_decay/wLB1zYDP">decays exponentially</a> from whatever value it possesses at the surface.
A superconductor with little or no magnetic field within it is said to be in the Meissner state. The Meissner state breaks down when the applied magnetic field is too large. Superconductors can be divided into two classes according to how this breakdown occurs. In Type I superconductors, superconductivity is abruptly destroyed when the strength of the applied field rises above a critical value Hc. Depending on the geometry of the sample, one may obtain an intermediate state<a class="footnote-ref" id="fnref:61" href="#fn:61">61</a> consisting of a baroque pattern<a class="footnote-ref" id="fnref:62" href="#fn:62">62</a> of regions of normal material carrying a magnetic field mixed with regions of superconducting material containing no field. In Type II superconductors, raising the applied field past a critical value Hc1 leads to a mixed state (also known as the vortex state) in which an increasing amount of <a href="/facts/Magnetic_flux/jQMVxrnD">magnetic flux</a> penetrates the material, but there remains no resistance to the flow of electric current as long as the current is not too large. At a second critical field strength Hc2, superconductivity is destroyed. The mixed state is actually caused by vortices in the electronic superfluid, sometimes called <a href="/facts/Fluxon/RVAJetQE">fluxons</a> because the flux carried by these <a href="/facts/Abrikosov_vortex/6yP83ySP">vortices</a> is <a href="/facts/Quantum/4x5QTxGB">quantized</a>. Most pure <a href="/facts/Chemical_element/0jducgWD">elemental</a> superconductors, except <a href="/facts/Niobium/3zNI8AKp">niobium</a> and <a href="/facts/Carbon_nanotube/atuDPPaG">carbon nanotubes</a>, are Type I, while almost all impure and compound superconductors are Type II.

<h3>London moment</h3>
Main article: <a href="/facts/London_moment/xIWkgbzl">London moment</a>
Conversely, a spinning superconductor generates a magnetic field, precisely aligned with the spin axis. The effect, the London moment, was put to good use in <a href="/facts/Gravity_Probe_B/UkD1Vs5F">Gravity Probe B</a>. This experiment measured the magnetic fields of four superconducting gyroscopes to determine their spin axes. This was critical to the experiment since it is one of the few ways to accurately determine the spin axis of an otherwise featureless sphere.

<h2 id="high-temperature-superconductivity">High-temperature superconductivity</h2>
This section is an excerpt from <a href="/facts/High-temperature_superconductivity/MXtx2gvV">High-temperature superconductivity</a>.[<a href="https://en.wikipedia.org/w/index.php?title=High-temperature_superconductivity&action=edit">edit</a>]

<a href="/facts/High-temperature_superconductivity/MXtx2gvV">High-temperature superconductivity</a> (high-Tc or HTS) is superconductivity in <a href="/facts/Material/Rmt5HySL">materials</a> with a critical temperature (the temperature below which the material behaves as a superconductor) above 77 K (−196.2 °C; −321.1 °F), the <a href="/facts/Boiling_point/E2BK9QoS">boiling point</a> of <a href="/facts/Liquid_nitrogen/IGWI1h00">liquid nitrogen</a>.<a class="footnote-ref" id="fnref:63" href="#fn:63">63</a> They are "high-temperature" only relative to previously known superconductors, which function only closer to <a href="/facts/Absolute_zero/U3UyPl2K">absolute zero</a>. The first high-temperature superconductor was discovered in 1986 by <a href="/facts/IBM/QszA7nwd">IBM</a> researchers <a href="/facts/Georg_Bednorz/p14P6Sy6">Georg Bednorz</a> and <a href="/facts/K._Alex_M%25C3%25BCller/89oyE7oM">K. Alex Müller</a>.<a class="footnote-ref" id="fnref:64" href="#fn:64">64</a><a class="footnote-ref" id="fnref:65" href="#fn:65">65</a> Although the critical temperature is around 35.1 K (−238.1 °C; −396.5 °F), this material was modified by <a href="/facts/Ching-Wu_Chu/ggU3asoS">Ching-Wu Chu</a> to make the first high-temperature superconductor with critical temperature 93 K (−180.2 °C; −292.3 °F).<a class="footnote-ref" id="fnref:66" href="#fn:66">66</a> Bednorz and Müller were awarded the <a href="/facts/Nobel_Prize_in_Physics/o6w1nCbr">Nobel Prize in Physics</a> in 1987 "for their important break-through in the discovery of superconductivity in ceramic materials".<a class="footnote-ref" id="fnref:67" href="#fn:67">67</a> Most high-Tc materials are <a href="/facts/Type-II_superconductor/8V4UTGjY">type-II superconductors</a>.
The major advantage of high-temperature superconductors is that they can be cooled using liquid nitrogen,<a class="footnote-ref" id="fnref:68" href="#fn:68">68</a> in contrast to previously known superconductors, which require expensive and hard-to-handle coolants, primarily <a href="/facts/Liquid_helium/JYXCAcDf">liquid helium</a>. A second advantage of high-Tc materials is they retain their superconductivity in higher magnetic fields than previous materials. This is important when constructing <a href="/facts/Superconducting_magnet/bRWH01s5">superconducting magnets</a>, a primary application of high-Tc materials.
The majority of high-temperature superconductors are <a href="/facts/Ceramic/9JKudpqX">ceramics</a>, rather than the previously known metallic materials. Ceramic superconductors are suitable for some practical uses but encounter manufacturing issues. For example, most ceramics are <a href="/facts/Brittle/cn27H2vg">brittle</a>, which complicates wire fabrication.<a class="footnote-ref" id="fnref:69" href="#fn:69">69</a> 

The main class of high-temperature superconductors is <a href="/facts/Copper_oxide/zkwqCeLG">copper oxides</a> combined with other metals, especially the <a href="/facts/Rare-earth_barium_copper_oxide/TlqK6YR7">rare-earth barium copper oxides</a> (REBCOs) such as <a href="/facts/Yttrium_barium_copper_oxide/hkFJMegk">yttrium barium copper oxide</a> (YBCO). The second class of high-temperature superconductors in the practical classification is the <a href="/facts/Iron-based_superconductor/SCoUWGmS">iron-based compounds</a>.<a class="footnote-ref" id="fnref:70" href="#fn:70">70</a><a class="footnote-ref" id="fnref:71" href="#fn:71">71</a> <a href="/facts/Magnesium_diboride/fsgNsNPP">Magnesium diboride</a> is sometimes included in high-temperature superconductors: It is relatively simple to manufacture, but it superconducts only below 39 K (−234.2 °C), which makes it unsuitable for liquid nitrogen cooling.
<h2 id="applications">Applications</h2>
Main article: <a href="/facts/Technological_applications_of_superconductivity/JtPmV9Ls">Technological applications of superconductivity</a>

Superconductors are promising candidate materials for devising fundamental circuit elements of electronic, spintronic, and quantum technologies. One such example is a superconducting diode,<a class="footnote-ref" id="fnref:72" href="#fn:72">72</a> in which supercurrent flows along one direction only, that promise dissipationless superconducting and semiconducting-superconducting hybrid technologies.
<a href="/facts/Superconducting_magnet/bRWH01s5">Superconducting magnets</a> are some of the most powerful <a href="/facts/Electromagnet/3YMYtSMX">electromagnets</a> known. They are used in <a href="/facts/Magnetic_resonance_imaging/Vh9yG9qq">MRI</a>/<a href="/facts/NMR/pGYAn9Bz">NMR</a> machines, <a href="/facts/Mass_spectrometer/RH5WBHJ2">mass spectrometers</a>, the beam-steering magnets used in <a href="/facts/Particle_accelerator/Pkuc08xC">particle accelerators</a> and plasma confining magnets in some <a href="/facts/Tokamaks/kDtb8Bsw">tokamaks</a>. They can also be used for magnetic separation, where weakly magnetic particles are extracted from a background of less or non-magnetic particles, as in the <a href="/facts/Pigment/I3clCYkF">pigment</a> industries. They can also be used in large wind turbines to overcome the restrictions imposed by high electrical currents, with an industrial grade 3.6 megawatt superconducting windmill generator having been tested successfully in Denmark.<a class="footnote-ref" id="fnref:73" href="#fn:73">73</a>
In the 1950s and 1960s, superconductors were used to build experimental digital computers using <a href="/facts/Cryotron/dgKtPUaN">cryotron</a> switches.<a class="footnote-ref" id="fnref:74" href="#fn:74">74</a> More recently, superconductors have been used to make <a href="/facts/Digital_circuit/3kJcKbkw">digital circuits</a> based on <a href="/facts/Rapid_single_flux_quantum/ufw0Ro72">rapid single flux quantum</a> technology and <a href="/facts/RF_and_microwave_filter/jSmB1Md9">RF and microwave filters</a> for <a href="/facts/Mobile_phone/H3EcqD9h">mobile phone</a> base stations.
Superconductors are used to build <a href="/facts/Josephson_junction/2fvcdS8N">Josephson junctions</a> which are the building blocks of <a href="/facts/SQUID/2FEvJ5wG">SQUIDs</a> (superconducting quantum interference devices), the most sensitive <a href="/facts/Magnetometer/dqX9g1og">magnetometers</a> known. SQUIDs are used in <a href="/facts/Scanning_SQUID_microscope/GWIq55sM">scanning SQUID microscopes</a> and <a href="/facts/Magnetoencephalography/epvUfx7A">magnetoencephalography</a>. Series of Josephson devices are used to realize the <a href="/facts/International_System_of_Units/S7YLglNz">SI</a> <a href="/facts/Volt/KF18MXP2">volt</a>. Superconducting photon detectors<a class="footnote-ref" id="fnref:75" href="#fn:75">75</a> can be realised in a variety of device configurations. Depending on the particular mode of operation, a <a href="/facts/Superconductor%25E2%2580%2593insulator%25E2%2580%2593superconductor/HQYdBut2">superconductor–insulator–superconductor</a> Josephson junction can be used as a photon <a href="/facts/Detector/RN8SXbjs">detector</a> or as a <a href="/facts/Electronic_mixer/KU8MfcyE">mixer</a>. The large resistance change at the transition from the normal to the superconducting state is used to build thermometers in cryogenic <a href="/facts/Calorimeter/Njp46oI8">micro-calorimeter</a> photon <a href="/facts/Detector/RN8SXbjs">detectors</a>. The same effect is used in ultrasensitive <a href="/facts/Bolometer/5YlzCoe8">bolometers</a> made from superconducting materials. <a href="/facts/Superconducting_nanowire_single-photon_detector/y0jCvWMr">Superconducting nanowire single-photon detectors</a> offer high speed, low noise single-photon detection and have been employed widely in advanced <a href="/facts/Photon_counting/eaF6pJts">photon-counting</a> applications.<a class="footnote-ref" id="fnref:76" href="#fn:76">76</a>
Other early markets are arising where the relative efficiency, size and weight advantages of devices based on <a href="/facts/High-temperature_superconductivity/MXtx2gvV">high-temperature superconductivity</a> outweigh the additional costs involved. For example, in <a href="/facts/Wind_turbine/lUfWqfLg">wind turbines</a> the lower weight and volume of superconducting generators could lead to savings in construction and tower costs, offsetting the higher costs for the generator and lowering the total <a href="/facts/Levelized_cost_of_electricity/cjRmY0xa">levelized cost of electricity</a> (LCOE).<a class="footnote-ref" id="fnref:77" href="#fn:77">77</a>
Promising future applications include high-performance <a href="/facts/Smart_grid/hR4pu3nH">smart grid</a>, <a href="/facts/Electric_power_transmission/I9w3lRmM">electric power transmission</a>, <a href="/facts/Transformer/EYYfXWrF">transformers</a>, <a href="/facts/SMES/uaXkhIXm">power storage devices</a>, <a href="/facts/Fusion_power/jyETSzm4">compact fusion power devices</a>, <a href="/facts/Electric_motor/ArD7BGDa">electric motors</a> (e.g. for vehicle propulsion, as in <a href="/facts/Vactrain/z0EFBkm1">vactrains</a> or <a href="/facts/Maglev_train/2o7UVAM5">maglev trains</a>), <a href="/facts/Magnetic_levitation_device/0QHxYmB2">magnetic levitation devices</a>, <a href="/facts/Fault_current_limiter/C575v5gh">fault current limiters</a>, enhancing spintronic devices with superconducting materials,<a class="footnote-ref" id="fnref:78" href="#fn:78">78</a> and superconducting <a href="/facts/Magnetic_refrigeration/Uup1rPD6">magnetic refrigeration</a>. However, superconductivity is sensitive to moving magnetic fields, so applications that use <a href="/facts/Alternating_current/qxICS3xa">alternating current</a> (e.g. transformers) will be more difficult to develop than those that rely upon <a href="/facts/Direct_current/r9MNUx84">direct current</a>. Compared to traditional power lines, <a href="/facts/Superconducting_transmission_line/JtPmV9Ls">superconducting transmission lines</a> are more efficient and require only a fraction of the space, which would not only lead to a better environmental performance but could also improve public acceptance for expansion of the electric grid.<a class="footnote-ref" id="fnref:79" href="#fn:79">79</a> Another attractive industrial aspect is the ability for high power transmission at lower voltages.<a class="footnote-ref" id="fnref:80" href="#fn:80">80</a> Advancements in the efficiency of cooling systems and use of cheap coolants such as liquid nitrogen have also significantly decreased cooling costs needed for superconductivity.

<h2 id="nobel-prizes">Nobel Prizes</h2>
As of 2022, there have been five <a href="/facts/Nobel_Prize_in_Physics/o6w1nCbr">Nobel Prizes in Physics</a> for superconductivity related subjects:

<ul><li><a href="/facts/Heike_Kamerlingh_Onnes/bJk48dFD">Heike Kamerlingh Onnes</a> (1913), "for his investigations on the properties of matter at low temperatures which led, inter alia, to the production of liquid helium".</li>
<li><a href="/facts/John_Bardeen/kbj763Fh">John Bardeen</a>, <a href="/facts/Leon_N._Cooper/058c4ER2">Leon N. Cooper</a>, and <a href="/facts/J._Robert_Schrieffer/DfX8s90T">J. Robert Schrieffer</a> (1972), "for their jointly developed theory of superconductivity, usually called the <a href="/facts/BCS_theory/KmlyhxPS">BCS-theory</a>".</li>
<li><a href="/facts/Leo_Esaki/DP0IvTgb">Leo Esaki</a>, <a href="/facts/Ivar_Giaever/TPQYgKPj">Ivar Giaever</a>, and <a href="/facts/Brian_D._Josephson/GG07CsRp">Brian D. Josephson</a> (1973), "for their experimental discoveries regarding tunneling phenomena in semiconductors and superconductors, respectively" and "for his theoretical predictions of the properties of a supercurrent through a tunnel barrier, in particular those phenomena which are generally known as the Josephson effects".</li>
<li><a href="/facts/Georg_Bednorz/p14P6Sy6">Georg Bednorz</a> and <a href="/facts/K._Alex_M%25C3%25BCller/89oyE7oM">K. Alex Müller</a> (1987), "for their important break-through in the discovery of superconductivity in ceramic materials".</li>
<li><a href="/facts/Alexei_A._Abrikosov/I4Gwb0yB">Alexei A. Abrikosov</a>, <a href="/facts/Vitaly_L._Ginzburg/uscYaLgY">Vitaly L. Ginzburg</a>, and <a href="/facts/Anthony_J._Leggett/z6AcXNbA">Anthony J. Leggett</a> (2003), "for pioneering contributions to the theory of superconductors and superfluids".<a class="footnote-ref" id="fnref:81" href="#fn:81">81</a></li></ul>
<h2 id="see-also">See also</h2>
<ul><li><a href="/facts/Hydrogen_cryomagnetics/MjGJ9dzk">Hydrogen cryomagnetics</a> – Use of cryogenic liquid hydrogen to cool an electromagnet</li>
<li><a href="/facts/MXenes/tSzMcSDj">MXenes</a> – Class of two-dimensional inorganic compounds</li>
<li><a href="/facts/Potential_applications_of_graphene/vgYvcHJy">Potential applications of graphene</a></li>
<li><a href="/facts/Superconducting_magnetic_energy_storage/wydmfHw1">Superconducting magnetic energy storage</a> – Energy storage technique</li></ul>

<h2 id="further-reading">Further reading</h2>
<ul><li><a href="/facts/International_Electrotechnical_Commission/hSK0kjwI">IEC</a> standard <a href="https://webstore.iec.ch/preview/info_iec61788-3%7Bed2.0%7Den.pdf">60050-815:2000, International Electrotechnical Vocabulary (IEV) – Part 815: Superconductivity</a> <a href="https://web.archive.org/web/20200307195214/https://webstore.iec.ch/preview/info_iec61788-3%7Bed2.0%7Den.pdf">Archived</a> 2020-03-07 at the <a href="/facts/Wayback_Machine/nmQ3a6JC">Wayback Machine</a>.</li>
<li>Kleinert, Hagen (1989). <a href="http://www.physik.fu-berlin.de/~kleinert/kleiner_reb1/contents1.html">"Superflow and Vortex Lines"</a>. Gauge Fields in Condensed Matter. Vol. 1. World Scientific. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-9971-5-0210-2.</li>
<li>Larkin, Anatoly; Varlamov, Andrei (2005). Theory of Fluctuations in Superconductors. Oxford University Press. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-19-852815-9.</li>
<li>Lebed, A. G. (2008). The Physics of Organic Superconductors and Conductors. Vol. 110 (1st ed.). Springer. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-3-540-76667-4.</li>
<li>Matricon, Jean; Waysand, Georges; Glashausser, Charles (2003). The Cold Wars: A History of Superconductivity. Rutgers University Press. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-8135-3295-0.</li>
<li><a href="https://www.sciencedaily.com/releases/2006/08/060817101658.htm">"Physicist Discovers Exotic Superconductivity"</a>. <a href="/facts/ScienceDaily/P1y9dmwH">ScienceDaily</a>. 17 August 2006.</li>
<li>Tinkham, Michael (2004). Introduction to Superconductivity (2nd ed.). Dover Books. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-486-43503-9.</li>
<li>Tipler, Paul; Llewellyn, Ralph (2002). Modern Physics (4th ed.). W. H. Freeman. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-7167-4345-3.</li>
<li>O'Mahony, Shane M.; University of Oxford (2022). <a href="https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9477408">"On the electron pairing mechanism of copper-oxide high temperature superconductivity"</a>. <a href="/facts/Proceedings_of_the_National_Academy_of_Sciences/w75CThX0">Proceedings of the National Academy of Sciences</a>. 119 (37): e2207449119. <a href="/facts/ArXiv_(identifier)/H6EtgnBe">arXiv</a>:<a href="https://arxiv.org/abs/2108.03655">2108.03655</a>. <a href="/facts/Bibcode_(identifier)/9HtdQSGB">Bibcode</a>:<a href="https://ui.adsabs.harvard.edu/abs/2022PNAS..11907449O">2022PNAS..11907449O</a>. <a href="/facts/Doi_(identifier)/muM9Etpq">doi</a>:<a href="https://doi.org/10.1073%2Fpnas.2207449119">10.1073/pnas.2207449119</a>. <a href="/facts/PMC_(identifier)/dX1zMt71">PMC</a> <a href="https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9477408">9477408</a>. <a href="/facts/PMID_(identifier)/JlHAvMHt">PMID</a> <a href="https://pubmed.ncbi.nlm.nih.gov/36067325">36067325</a>.</li>
<li>Charlie Wood, <a href="/facts/Quanta_Magazine/FkbYnGtU">Quanta Magazine</a> (2022). <a href="https://www.quantamagazine.org/high-temperature-superconductivity-understood-at-last-20220921/">"High-Temperature Superconductivity Understood at Last"</a>.</li></ul>
<h2 id="external-links">External links</h2>

Wikiquote has quotations related to Superconductivity.

<ul><li><a href="http://alfredleitner.com/">Video about Type I Superconductors: R=0/transition temperatures/ B is a state variable/ Meissner effect/ Energy gap(Giaever)/ BCS model</a></li>
<li><a href="https://web.archive.org/web/20100821182614/http://www.msm.cam.ac.uk/ascg/lectures/">Lectures on Superconductivity (series of videos, including interviews with leading experts)</a></li>
<li><a href="https://www.youtube.com/watch?v=indyz6O-Xyw&feature=user">YouTube Video Levitating magnet</a></li>
<li><a href="http://www.doitpoms.ac.uk/tlplib/superconductivity/index.php">DoITPoMS Teaching and Learning Package – "Superconductivity"</a></li>
<li><a href="https://feynmanlectures.caltech.edu/III_21.html">The Schrödinger Equation in a Classical Context: A Seminar on Superconductivity – The Feynman Lectures on Physics</a>.</li></ul>

<h2 id="references">References</h2>

<ol>
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<li id="fn:3">Bardeen, John; Cooper, Leon; Schrieffer, J. R. (December 1, 1957). "Theory of Superconductivity". Physical Review. 108 (5): 1175. Bibcode:1957PhRv..108.1175B. doi:10.1103/physrev.108.1175. S2CID 73661301. Retrieved June 6, 2014. Reprinted in Bogoliubov, Nikolaĭ Nikolaevich, ed. (1963). The Theory of Superconductivity. Vol. 4. Gordon and Breach. p. 73. OCLC 537010. <a href="https://books.google.com/books?id=_QKPGDG-cuAC&q=%22persist+indefinitely&pg=PA76" target="_blank">https://books.google.com/books?id=_QKPGDG-cuAC&q=%22persist+indefinitely&pg=PA76</a> <a href="#fnref:3" class="footnote-back-ref">↩</a></li>
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</ol>

Superconductivity open-in-new

Superconductivity