The superconductivity confined in a two-dimensional interface exhibits many exotic phenomena that have certain counterparts in layered cuprates and iron-based superconductors, and thus provides rare opportunities to reveal the mystery of high temperature superconductivity therein. By constructing and tailoring hybrid heterostructures such as FeSe/
Publié le :
Sha Han 1, 2 ; Can-Li Song 3, 2 ; Xu-Cun Ma 3, 2 ; Qi-Kun Xue 4, 3, 5, 2

@article{CRPHYS_2021__22_S4_163_0, author = {Sha Han and Can-Li Song and Xu-Cun Ma and Qi-Kun Xue}, title = {Interface enhanced superconductivity in {FeSe/SrTiO}$_{3}$ and the hidden nature}, journal = {Comptes Rendus. Physique}, pages = {163--182}, publisher = {Acad\'emie des sciences, Paris}, volume = {22}, number = {S4}, year = {2021}, doi = {10.5802/crphys.87}, language = {en}, }
TY - JOUR AU - Sha Han AU - Can-Li Song AU - Xu-Cun Ma AU - Qi-Kun Xue TI - Interface enhanced superconductivity in FeSe/SrTiO$_{3}$ and the hidden nature JO - Comptes Rendus. Physique PY - 2021 SP - 163 EP - 182 VL - 22 IS - S4 PB - Académie des sciences, Paris DO - 10.5802/crphys.87 LA - en ID - CRPHYS_2021__22_S4_163_0 ER -
Sha Han; Can-Li Song; Xu-Cun Ma; Qi-Kun Xue. Interface enhanced superconductivity in FeSe/SrTiO$_{3}$ and the hidden nature. Comptes Rendus. Physique, Recent advances in 2D material physics, Volume 22 (2021) no. S4, pp. 163-182. doi : 10.5802/crphys.87. https://comptes-rendus.academie-sciences.fr/physique/articles/10.5802/crphys.87/
[1] et al. Interface-induced high-temperature superconductivity in single unit-cell FeSe films on SrTiO
[2] et al. Electronic origin of high-temperature superconductivity in single-layer FeSe superconductor, Nat. Commun., Volume 3 (2012), 931
[3] et al. Phase diagram and electronic indication of high-temperature superconductivity at 65 K in single-layer FeSe films, Nat. Mater., Volume 12 (2013) no. 7, pp. 605-610
[4] et al. Interface-induced superconductivity and strain-dependent spin density waves in FeSe/SrTiO
[5] et al. Interfacial mode coupling as the origin of the enhancement of T
[6] Meissner and mesoscopic superconducting states in 1–4 unit-cell FeSe films, Phys. Rev. B, Volume 90 (2014) no. 21, 214513
[7] Superconductivity above 100 K in single-layer FeSe films on doped SrTiO
[8] Interfacial superconductivity in FeSe ultrathin films on SrTiO
[9] Monolayer FeSe on SrTiO
[10] High-temperature superconductivity in one-unit-cell FeSe films, J. Phys.: Condens. Matter, Volume 29 (2017) no. 15, 153001
[11] Routes to high-temperature superconductivity: A lesson from FeSe/SrTiO
[12] Doping a Mott insulator: physics of high-temperature superconductivity, Rev. Mod. Phys., Volume 78 (2006), pp. 17-85
[13] A new frontier for superconductivity, Nat. Phys., Volume 10 (2014) no. 12, pp. 892-895
[14] High-temperature interface superconductivity between metallic and insulating copper oxides, Nature, Volume 455 (2008) no. 7214, pp. 782-785
[15] High-temperature superconductivity in a single copper–oxygen plane, Science, Volume 326 (2009) no. 5953, pp. 699-702
[16] Pressure induced static magnetic order in superconducting FeSe
[17] Unconventional superconductivity with a sign reversal in the order parameter of LaFeAsO
[18] Nematic pairing from orbital-selective spin fluctuations in FeSe, NPJ Quantum Mater., Volume 3 (2018) no. 1, 56
[19] Electron–phonon coupling enhanced by the FeSe/SrTiO
[20] Ab initio study of cross-interface electron–phonon couplings in FeSe thin films on SrTiO
[21] Neutron scattering and the B
[22] Electron–phonon coupling in cuprate and iron-based superconductors revealed by Raman scattering, Chin. Phys. B, Volume 22 (2013) no. 8, 087103
[23] Jahn–Teller physics and high-T
[24] Interface high-temperature superconductivity, Supercond. Sci. Technol., Volume 29 (2016) no. 12, 123001
[25] et al. Nodeless pairing in superconducting copper-oxide monolayer films on Bi
[26] Observation of interface superconductivity in a SnSe
[27] Hole-concentration dependence of band structure in (Bi,Pb)
[28] Pairing symmetry in cuprate superconductors, Rev. Mod. Phys., Volume 72 (2000), pp. 969-1016
[29] d-wave superconductor as a model of high-T
[30] et al. Presence of s-wave pairing in Josephson junctions made of twisted ultrathin Bi
[31] A high mobility electron gas at the LaAlO
[32] Evolution of high-temperature superconductivity from a low-T
[33] et al. Coexistence of superconductivity and antiferromagnetism in (Li
[34] et al. Common electronic origin of superconductivity in (Li,Fe)OHFeSe bulk superconductor and single-layer FeSe/SrTiO
[35] High-temperature superconductivity in potassium-coated multilayer FeSe thin films, Nat. Mater., Volume 14 (2015) no. 8, pp. 775-779
[36] et al. Anomalous correlation effects and unique phase diagram of electron-doped FeSe revealed by photoemission spectroscopy, Nat. Commun., Volume 7 (2016), 10840
[37] Superconductivity below 20 K in heavily electron-doped surface layer of FeSe bulk crystal, Nat. Commun., Volume 7 (2016), 11116
[38] FeSe(en)
[39] Substrate and band bending effects on monolayer FeSe on SrTiO
[40] Origin of charge transfer and enhanced electron–phonon coupling in single unit-cell FeSe films on SrTiO
[41] Direct imaging of electron transfer and its influence on superconducting pairing at FeSe/SrTiO
[42] Direct evidence of superconductivity and determination of the superfluid density in buried ultrathin FeSe grown on SrTiO
[43] Intrinsic interfacial van der Waals monolayers and their effect on the high-temperature superconductor FeSe/SrTiO
[44] et al. Interface enhanced superconductivity in monolayer FeSe films on MgO(001): charge transfer with atomic substitution, Sci. Bull., Volume 63 (2018) no. 12, pp. 747-752
[45] Electron mobilities in modulation-doped semiconductor heterojunction superlattices, Appl. Phys. Lett., Volume 33 (1978) no. 7, pp. 665-667
[46] Optical probe of electrostatic-doping in an n-type Mott insulator, Phys. Rev. B, Volume 75 (2007), 155103
[47] Change of carrier density at the pseudogap critical point of a cuprate superconductor, Nature, Volume 531 (2016) no. 7593, pp. 210-214
[48] et al. Persistence of magnetic excitations in La
[49] High-temperature superconductivity in space-charge regions of lanthanum cuprate induced by two-dimensional doping, Nat. Commun., Volume 6 (2015), 8586
[50] et al. Superconducting interfaces between insulating oxides, Science, Volume 317 (2007) no. 5842, pp. 1196-1199
[51] et al. Interface superconductor with gap behaviour like a high-temperature superconductor, Nature, Volume 502 (2013) no. 7472, pp. 528-531
[52] et al. Direct observation of a two-dimensional hole gas at oxide interfaces, Nat. Mater., Volume 17 (2018) no. 3, pp. 231-236
[53] Interface superconductivity, Physica C, Volume 514 (2015), pp. 189-198
[54] Why some interfaces cannot be sharp, Nat. Mater., Volume 5 (2006) no. 3, pp. 204-209
[55] Control of electronic conduction at an oxide heterointerface using surface polar adsorbates, Nat. Commun., Volume 2 (2011), 494
[56] et al. Ferroelectric control of the conduction at the LaAlO
[57] Tuning the two-dimensional electron gas at the LaAlO
[58] A possible superconductor-like state at elevated temperatures near metal electrodes in an LaAlO
[59]
[60] Artificial charge-modulationin atomic-scale perovskite titanate superlattices, Nature, Volume 419 (2002) no. 6905, pp. 378-380
[61] Electrical transport properties of polar heterointerface between KTaO
[62] Polar discontinuity doping of the LaVO
[63] Effect of A-site cation ordering on the magnetoelectric properties in [(LaMnO
[64] et al. High-mobility spin-polarized two-dimensional electron gases at EuO/KTaO
[65] et al. Two-dimensional superconductivity and anisotropic transport at KTaO
[66] Visualizing the evolution from the Mott insulator to a charge-ordered insulator in lightly doped cuprates, Nat. Phys., Volume 12 (2016) no. 11, pp. 1047-1051
[67] Electronic structure of La
[68] Angle-resolved photoemission studies of the cuprate superconductors, Rev. Mod. Phys., Volume 75 (2003) no. 2, 473
[69] Chemical potential shift in overdoped and underdoped La
[70] Enhanced superconductivity in surface-electron-doped iron pnictide Ba(Fe
[71] Superconductivity below 20 K in heavily electron-doped surface layer of FeSe bulk crystal, Nat. Commun., Volume 7 (2016), 11116
[72] et al. Enhanced superconductivity accompanying a Lifshitz transition in electron-doped FeSe monolayer, Nat. Commun., Volume 8 (2017), 14988
[73] et al. Lifting of xz
[74] et al. Tuning the band structure and superconductivity in single-layer FeSe by interface engineering, Nat. Commun., Volume 5 (2014), 5044 | DOI
[75] et al. Distinct Fermi surface topology and nodeless superconducting gap in a Tl
[76] et al. Nodeless superconducting gap in A
[77] Orbital-dependent Fermi surface shrinking as a fingerprint of nematicity in FeSe, Phys. Rev. B, Volume 94 (2016), 155138 | DOI
[78] Strong nodeless pairing on separate electron Fermi surface sheets in (Tl,K)Fe
[79] et al. Common Fermi-surface topology and nodeless superconducting gap of K
[80] et al. Absence of a holelike Fermi surface for the iron-based K
[81] et al. Band structure and Fermi surface of an extremely overdoped iron-based superconductor KFe
[82] et al. Angle-resolved photoemission spectroscopy of tetragonal CuO: evidence for intralayer coupling between cupratelike sublattices, Phys. Rev. Lett., Volume 113 (2014), 187001 | DOI
[83] Topology of the Fermi surface and band structure near the Fermi level in the Pb-doped Bi
[84] et al. Missing quasiparticles and the chemical potential puzzle in the doping evolution of the cuprate superconductors, Phys. Rev. Lett., Volume 93 (2004), 267002
[85] Chemical potential shift in lightly doped to optimally doped Ca
[86] Chemical potential shift in lightly doped to overdoped Bi
[87] et al. Appearance of universal metallic dispersion in a doped Mott insulator, Phys. Rev. B, Volume 78 (2008), 104513 | DOI
[88] Doping-dependent evolution of the electronic structure of La
[89] Antiferromagnetism in metals: from the cuprate superconductors to the heavy Fermion materials, J. Phys.: Condens. Matter, Volume 24 (2012) no. 29, 294205
[90] Chemical potential shift in Nd
[91] et al. Doping dependence of an n-type cuprate superconductor investigated by angle-resolved photoemission spectroscopy, Phys. Rev. Lett., Volume 88 (2002), 257001 | DOI
[92] et al. Fermi surface and quasiparticle excitations of overdoped Tl
[93] Two-Fermi-surface superconducting state and a nodal d-wave energy gap of the electron-doped Sm
[94] et al. Importance of the Fermi-surface topology to the superconducting state of the electron-doped pnictide Ba(Fe
[95] Strongly enhanced temperature dependence of the chemical potential in FeSe, Phys. Rev. B, Volume 95 (2017), 195111 | DOI
[96] Unusual temperature dependence of band dispersion in Ba(Fe
[97] et al. Large temperature dependence of the number of carriers in Co-doped BaFe
[98] et al. Evolution of the pseudogap from Fermi arcs to the nodal liquid, Nat. Phys., Volume 2 (2006) no. 7, pp. 447-451 | DOI
[99] Charge transfer and electron–phonon coupling in monolayer FeSe on Nb-doped SrTiO
[100] Large phonon band gap in SrTiO
[101] Electron phonon coupling versus photoelectron energy loss at the origin of replica bands in photoemission of FeSe on SrTiO
[102] et al. Evidence of cooperative effect on the enhanced superconducting transition temperature at the FeSe/SrTiO
[103] et al. Lattice dynamics of ultrathin FeSe films on SrTO
[104] Large electron–phonon interactions from FeSe phonons in a monolayer, New J. Phys., Volume 17 (2015) no. 7, 073027
[105] et al. Molecular beam epitaxy growth and post-growth annealing of FeSe films on SrTiO
[106] Interaction of phonons and Dirac Fermions on the surface of Bi
[107] Density of phonon states in superconducting FeSe as a function of temperature and pressure, Phys. Rev. B, Volume 81 (2010), 184510 | DOI
[108] Coexistence of isotropic and extended s-wave order parameters in FeSe as revealed by low-temperature specific heat, Phys. Rev. B, Volume 84 (2011), 220507
[109] What makes the T
[110] First-principles study of magnetic frustration in FeSe epitaxial films on SrTiO
[111] et al. Interface ferroelectric transition near the gap-opening temperature in a single-unit-cell FeSe film grown on Nb-Doped SrTiO
[112] et al. Role of SrTiO
[113] et al. Enhanced superconducting state in FeSe/SrTiO
[114] et al. Femtosecond electron–phonon lock-in by photoemission and X-ray free-electron laser, Science, Volume 357 (2017) no. 6346, pp. 71-75 | DOI
[115] et al. Observation of high-T
[116] et al. Interface induced high temperature superconductivity in single unit-cell FeSe on SrTiO
[117] High-temperature superconductivity in single-unit-cell FeSe films on anatase TiO
[118] Coexistence of replica bands and superconductivity in FeSe monolayer films, Phys. Rev. Lett., Volume 118 (2017), 067002 | DOI
[119] et al. Superconductivity above 28 K in single unit cell FeSe films interfaced with GaO
[120] et al. Strong interplay between stripe spin fluctuations, nematicity and superconductivity in FeSe, Nat. Mater., Volume 15 (2016) no. 2, pp. 159-163 | DOI
[121] First-principles study of FeSe epitaxial films on SrTiO
[122] Antiferromagnetic ground state with pair-checkerboard order in FeSe, Phys. Rev. B, Volume 91 (2015), 020504
[123] et al. Antiferromagnetic order in epitaxial FeSe films on SrTiO
[124] Dipolar phonons and electronic screening in monolayer FeSe on SrTiO
[125] Coexistence of magnetic order and two-dimensional superconductivity at LaAlO
[126] et al. Observation of antiferromagnetic domains in epitaxial thin films, Science, Volume 287 (2000) no. 5455, pp. 1014-1016 | DOI
[127] Spin-resolved electron–phonon coupling in FeSe and KFe
[128] Antiferromagnetic FeSe monolayer on SrTiO
[129] Effects of charge doping and constrained magnetization on the electronic structure of an FeSe monolayer, J. Phys.: Condens. Matter, Volume 25 (2013) no. 10, 105506
[130] Stimulated emission of Cooper pairs in a high-temperature cuprate superconductor, Sci. Rep., Volume 6 (2016), 29100
[131] Handbook of High-temperature Superconductivity: Theory and Experiment, Springer, New York, NY, USA, 2007 | Zbl
[132] et al. Three-dimensional collective charge excitations in electron-doped copper oxide superconductors, Nature, Volume 563 (2018) no. 7731, pp. 374-378 | DOI
- Observation of Selective Excitation of Raman Inactive Phonon Mode of Strontium Titanate Through Anti-Stokes Hyper-Raman Scattering Process, Journal of Infrared, Millimeter, and Terahertz Waves, Volume 45 (2024) no. 11-12, p. 999 | DOI:10.1007/s10762-024-01014-8
- Transition to Metallic and Superconducting States Induced by Thermal or Electrical Deoxidation of the Dislocation Network in the Surface Region of SrTiO3, Nanomaterials, Volume 14 (2024) no. 23, p. 1944 | DOI:10.3390/nano14231944
- When superconductivity crosses over: From BCS to BEC, Reviews of Modern Physics, Volume 96 (2024) no. 2 | DOI:10.1103/revmodphys.96.025002
- Two-dimensional van der Waals: Characterization and manipulation of superconductivity, Acta Physica Sinica, Volume 71 (2022) no. 18, p. 187401 | DOI:10.7498/aps.71.20220638
Cité par 4 documents. Sources : Crossref
Commentaires - Politique
Vous devez vous connecter pour continuer.
S'authentifier