Introduction to Superconductivity
By H. Alloul. 2011
3,499 citations recorded by the source corpus.
Subfields: Atomic and Molecular Physics, and Optics, Condensed Matter Physics
View Paper: https://www.semanticscholar.org/paper/d0e46527db28653ffdf05d1be4c24f5b617a7cd7
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Atomic and Molecular Physics, and Optics
- K. Novoselov
- Takashi Taniguchi
- Kenji Watanabe
- A.K. Geim
- C. Beenakker
- N. M. R. Peres
- P. Jarillo-Herrero
- Sylvia Serfaty
In Condensed Matter Physics
- Takashi Taniguchi
- Kenji Watanabe
- Sylvia Serfaty
- P. Jarillo-Herrero
- C. Beenakker
- Javier D. Sanchez-Yamagishi
- Matthias Troyer
- Etienne Sandier
Citations in the corpus
- General Theory of Josephson Diodes (2021, background): “In general, the Josephson junction can be understood from the Ginzburg-Landau (G-L) theory [2, 3, 41].”
- A Review of the Terahertz Conductivity of Bulk and Nano-Materials (2012, methodology): “4BiO3 the characteristic σ2 ∝ 1/ω was also observed [200], and although the measured frequency range was well below the superconducting gap 2∆ was obtained by fitting the imaginary conductivity using σ2/σn = (π∆/ω) tanh(∆/2kBT ), where σn is the normal state conductivity immediately above Tc [201].”
- Comparing the Fundamental Physics and Device Performance of Transparent, Conductive Nanostructured Networks with Conventional Transparent Conducting Oxides (2012, background): “[20,30] It may be possible to use something like Equation 1 if either the real or imaginary conductivity is negligible (with slight changes in the functional form),[31] but this is simply not the case with SWNT networks.”
- Josephson-junction-embedded transmission-line resonators: From Kerr medium to in-line transmon (2012, neutral): “In this situation, the Josephson potential ĤJ = −EJ cos(2πδ̂/ 0) is replaced with [29]”
- NIKA: A millimeter-wave kinetic inductance camera (2010, methodology): “Here we present an overview of the operating principles of the detector arrays, a summary of the principal instrument design elements, and the results from the first measurement run.”
- From the Ginzburg-Landau Model to Vortex Lattice Problems (2010, methodology): “We refer to the classic monographs and textbooks by De Gennes [DeG], Saint-James Sarma - Thomas [SST], Tinkham [Ti].”
- Engineered platforms for topological superconductivity and Majorana zero modes (2021, background): “The change in winding number, related to the Little-Parks effect [67], was indeed key to understanding the possible transition into a topologically nontrivial state.”
- Correlated insulator behaviour at half-filling in magic-angle graphene superlattices (2018, background): “) observed in nonmagic-angle TwBLG (which is just twice that of monolayer graphene) [1, 7].”
- Materials challenges and opportunities for quantum computing hardware (2021, background): “The junction critical current that governs the inductance of the qubit is exponentially sensitive to the thickness of the tunnel barrier ( 76 ), which is typically an amorphous AlO x layer (Fig.”
- Quantum oscillations of the critical current and high-field superconducting proximity in ballistic graphene (2015, methodology): “Marked deviations from equation (2) occur in B> 5mT (Fig.”
- Microwave response of vortices in superconducting thin films of Re and Al (2008, background): “Because superconductivity is suppressed in the core of a vortex, the motion of vortices leads to dissipation, as is typically characterized by the flux-flow vortex viscosity η = Φ0Bc2/ρn, where Φ0 is the flux quantum, h/2e, ρn is the normal-state resistivity of the material, and Bc2 is the upper-cri”
- Induced superconductivity in the quantum spin Hall edge (2013, background): “The particular shape of the critical current interference pattern depends on the phase-sensitive summation of the supercurrents traversing the junction [26].”
- Electrodynamics of correlated electron materials (2011, methodology): “The electrodynamics were experimentally measured by Glover and Tinkham (1957) using far-infrared techniques (Tinkham, 1996).”
- Superconductivity, superfluidity and quantum geometry in twisted multilayer systems (2021, background): “The electrodynamic properties of superconducting materials are captured by the constitutive relation (in London gauge) [5, 24]”
- Detecting superlight dark matter with Fermi-degenerate materials (2015, background): “As the energy deposits drop and approach the gap, an additional factor that takes into account the presence of the superconducting gap, a so-called coherence factor — similar to a form factor — kicks in [30]; this factor depends on energy and has an effect”
- Supercurrent: Vector hair for an AdS black hole (2008, background): “The phase structure we find can be interpreted by comparing with the known behaviour of superfluids [15].”