Superinsulator

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A superinsulator is a material that at low but finite temperatures does not conduct electricity, i.e. has an infinite resistance so that no electric current passes through it. [1] The phenomenon of superinsulation can be regarded as an exact dual to superconductivity.

Contents

The superinsulating state can be destroyed by increasing the temperature and applying an external magnetic field and voltage. A superinsulator was first predicted by M. C. Diamantini, P. Sodano, and C. A. Trugenberger in 1996 [2] who found a superinsulating ground state dual to superconductivity, emerging at the insulating side of the superconductor-insulator transition in the Josephson junction array due to electric-magnetic duality. Superinsulators were independently rediscovered by T. Baturina and V. Vinokur in 2008 [3] on the basis of duality between two different symmetry realizations of the uncertainty principle and experimentally found in titanium nitride (TiN) films. The 2008 measurements revealed giant resistance jumps interpreted as manifestations of the voltage threshold transition to a superinsulating state which was identified as the low-temperature confined phase emerging below the charge Berezinskii-Kosterlitz-Thouless transition. These jumps were similar to earlier findings of the resistance jumps in indium oxide (InO) films. [4] The finite-temperature phase transition into the superinsulating state was finally confirmed by Mironov et al. in NbTiN films in 2018. [5]

Other researchers have seen the similar phenomenon in disordered indium oxide films. [6]

Mechanism

Both superconductivity and superinsulation rest on the pairing of conduction electrons into Cooper pairs. In superconductors, all the pairs move coherently, allowing for the electric current without resistance. In superinsulators, both Cooper pairs and normal excitations are confined and the electric current cannot flow. A mechanism behind superinsulation is the proliferation of magnetic monopoles at low temperatures. [7] In two dimensions (2D), magnetic monopoles are quantum tunneling events (instantons) that are often referred to as monopole “plasma”. In three dimensions (3D), monopoles form a Bose condensate. Monopole plasma or monopole condensate squeezes Faraday's electric field lines into thin electric flux filaments or strings dual to Abrikosov vortices in superconductors. Cooper pairs of opposite charges at the end of these electric strings feel an attractive linear potential. When the corresponding string tension is large, it is energetically favorable to pull out of vacuum many charge-anticharge pairs and to form many short strings rather than to continue stretching the original one. As a consequence, only neutral “electric pions” exist as asymptotic states and the electric conduction is absent. This mechanism is a single-color version of the confinement mechanism that binds quarks into hadrons.

Because the electric forces are much weaker than strong forces of the particle physics, the typical size of “electric pions” well exceeds the size of corresponding elementary particles. This implies that preparing the samples that are sufficiently small, one can peer inside an “electric pion,” where electric strings are loose and Coulomb interactions are screened, hence electric charges are effectively unbound and move as if they were in the metal. The low-temperature saturation of the resistance to metallic behavior has been observed in TiN films with small lateral dimensions.

Future applications

Superinsulators could potentially be used as a platform for high-performance sensors and logical units. Combined with superconductors, superinsulators could be used to create switching electrical circuits with no energy loss as heat. [8]

Related Research Articles

<span class="mw-page-title-main">Superconductivity</span> Electrical conductivity with exactly zero resistance

Superconductivity is a set of physical properties observed in certain materials where electrical resistance vanishes and magnetic fields are expelled from the material. Any material exhibiting these properties is a superconductor. Unlike an ordinary metallic conductor, whose resistance decreases gradually as its temperature is lowered, even down to near absolute zero, a superconductor has a characteristic critical temperature below which the resistance drops abruptly to zero. An electric current through a loop of superconducting wire can persist indefinitely with no power source.

Unconventional superconductors are materials that display superconductivity which is not explained by the usual BCS theory or its extension, the Eliashberg theory. The pairing in unconventional superconductors may originate from some other mechanism than the electron–phonon interaction. Alternatively, a superconductor is called unconventional if the superconducting order parameter transforms according to a non-trivial irreducible representation of the point group or space group of the system.

<span class="mw-page-title-main">High-temperature superconductivity</span> Superconductive behavior at temperatures much higher than absolute zero

High-temperature superconductors are defined as materials with critical temperature above 77 K, the boiling point of liquid nitrogen. They are only "high-temperature" relative to previously known superconductors, which function at even colder temperatures, close to absolute zero. The "high temperatures" are still far below ambient, and therefore require cooling. The first breakthrough of high-temperature superconductor was discovered in 1986 by IBM researchers Georg Bednorz and K. Alex Müller. Although the critical temperature is around 35.1 K, this new type of superconductor was readily modified by Ching-Wu Chu to make the first high-temperature superconductor with critical temperature 93 K. Bednorz and Müller were awarded the Nobel Prize in Physics in 1987 "for their important break-through in the discovery of superconductivity in ceramic materials". Most high-Tc materials are type-II superconductors.

A room-temperature superconductor is a hypothetical material capable of displaying superconductivity above 0 °C, operating temperatures which are commonly encountered in everyday settings. As of 2023, the material with the highest accepted superconducting temperature was highly pressurized lanthanum decahydride, whose transition temperature is approximately 250 K (−23 °C) at 200 GPa.

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The Little–Parks effect was discovered in 1962 by William A. Little and Ronald D. Parks in experiments with empty and thin-walled superconducting cylinders subjected to a parallel magnetic field. It was one of the first experiments to indicate the importance of Cooper-pairing principle in BCS theory.

<span class="mw-page-title-main">Pseudogap</span> State at which a Fermi surface has a partial energy gap in condensed matter physics

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<span class="mw-page-title-main">Proximity effect (superconductivity)</span> Phenomena that occur when a superconductor is in contact with a non-superconductor

Proximity effect or Holm–Meissner effect is a term used in the field of superconductivity to describe phenomena that occur when a superconductor (S) is placed in contact with a "normal" (N) non-superconductor. Typically the critical temperature of the superconductor is suppressed and signs of weak superconductivity are observed in the normal material over mesoscopic distances. The proximity effect is known since the pioneering work by R. Holm and W. Meissner. They have observed zero resistance in SNS pressed contacts, in which two superconducting metals are separated by a thin film of a non-superconducting metal. The discovery of the supercurrent in SNS contacts is sometimes mistakenly attributed to Brian Josephson's 1962 work, yet the effect was known long before his publication and was understood as the proximity effect.

Cuprate superconductors are a family of high-temperature superconducting materials made of layers of copper oxides (CuO2) alternating with layers of other metal oxides, which act as charge reservoirs. At ambient pressure, cuprate superconductors are the highest temperature superconductors known. However, the mechanism by which superconductivity occurs is still not understood.

Ferromagnetic superconductors are materials that display intrinsic coexistence of ferromagnetism and superconductivity. They include UGe2, URhGe, and UCoGe. Evidence of ferromagnetic superconductivity was also reported for ZrZn2 in 2001, but later reports question these findings. These materials exhibit superconductivity in proximity to a magnetic quantum critical point.

<span class="mw-page-title-main">Iron-based superconductor</span>

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References

  1. Mironov, A.; Diamantini, M. C.; Trugenberger, C. A.; Vinokur, V. M. (2022-11-19). "Relaxation electrodynamics of superinsulators". Scientific Reports. 12 (1): 19918. arXiv: 2207.00791 . Bibcode:2022NatSR..1219918M. doi:10.1038/s41598-022-24460-7. ISSN   2045-2322. PMC   9675743 . PMID   36402824. S2CID   250264815.
  2. Diamantini, M.C.; Sodano, P.; Trugenberger, C.A. (1996). "Gauge theories of Josephson junction arrays". Nuclear Physics B. 474 (3): 641–677. arXiv: hep-th/9511168 . Bibcode:1996NuPhB.474..641D. doi:10.1016/0550-3213(96)00309-4. S2CID   16002482.
  3. Vinokur, Valerii M.; Baturina, Tatyana I.; Fistul, Mikhail V.; Mironov, Aleksey Yu.; Baklanov, Mikhail R.; Strunk, Christoph (2008). "Superinsulator and quantum synchronization". Nature. 452 (7187): 613–615. Bibcode:2008Natur.452..613V. doi:10.1038/nature06837. ISSN   0028-0836. PMID   18385735. S2CID   205212720.
  4. Sambandamurthy, G.; Engel, L. W.; Johansson, A.; Peled, E.; Shahar, D. (2005). "Experimental Evidence for a Collective Insulating State in Two-Dimensional Superconductors". Physical Review Letters. 94 (1): 017003. arXiv: cond-mat/0403480 . Bibcode:2005PhRvL..94a7003S. doi:10.1103/PhysRevLett.94.017003. ISSN   0031-9007. PMID   15698122. S2CID   26180507.
  5. Mironov, Alexey Yu.; Silevitch, Daniel M.; Proslier, Thomas; Postolova, Svetlana V.; Burdastyh, Maria V.; Gutakovskii, Anton K.; Rosenbaum, Thomas F.; Vinokur, Valerii V.; Baturina, Tatyana I. (2018). "Charge Berezinskii-Kosterlitz-Thouless transition in superconducting NbTiN films". Scientific Reports . 8 (1): 4082. arXiv: 1707.09679 . Bibcode:2018NatSR...8.4082M. doi: 10.1038/s41598-018-22451-1 . ISSN   2045-2322. PMC   5840303 . PMID   29511317.
  6. Ovadia, M.; Sacépé, B.; Shahar, D. (2009). "Electron-Phonon Decoupling in Disordered Insulators". Physical Review Letters . 102 (17): 176802. Bibcode:2009PhRvL.102q6802O. doi:10.1103/PhysRevLett.102.176802. PMID   19518807.
  7. Diamantini, M. C.; Trugenberger, C. A.; Vinokur, V. M. (2018). "Confinement and asymptotic freedom with Cooper pairs". Communications Physics. 1 (1): 77. arXiv: 1807.01984 . Bibcode:2018CmPhy...1...77D. doi: 10.1038/s42005-018-0073-9 . ISSN   2399-3650.
  8. "Newly discovered 'superinsulators' promise to transform materials research, electronics design". Physorg.com. April 7, 2008.