ライフサイエンスコーパス: superconductivity

1 thin-film heterostructures designed to host superconductivity.

2 the debate on the origin of high-temperature superconductivity.

3 e role of dimensionality in high-temperature superconductivity.

4 ious puzzle in the field of high-temperature superconductivity.

5 ight into the electron pairing mechanisms of superconductivity.

6 ong candidate for chiral-triplet topological superconductivity.

7 trategy for tunable electronic transport and superconductivity.

8 could be integral to explaining its puzzling superconductivity.

9 electronic ground state has been obscured by superconductivity.

10 of beta-PdBi(2), to result in 3D topological superconductivity.

11 the fundamental physics of high-temperature superconductivity.

12 e-invigorated the quest for room temperature superconductivity.

13 on between ferromagnetism and unconventional superconductivity.

14 te is one promising way to yield topological superconductivity.

15 ge and energy transport, light emission, and superconductivity.

16 while phase fluctuations limit the domain of superconductivity.

17 structure for understanding the mechanism of superconductivity.

18 he essential ingredients of high-temperature superconductivity.

19 nding problem of the origin of the high-T(C) superconductivity.

20 for realizing and characterizing topological superconductivity.

21 coupling are capable of hosting topological superconductivity.

22 with scenarios for the evolution of high-T c superconductivity.

23 cal insulators, the Rashba effect, or p-wave superconductivity.

24 nd possibly high-transition-temperature (Tc) superconductivity.

25 d are ideal candidates to search for natural superconductivity.

26 tronic properties including room-temperature superconductivity.

27 nce of numerous correlated phases, including superconductivity.

28 c order to nontrivial topological phases and superconductivity.

29 -plane transport anisotropy, Weyl nodes, and superconductivity.

30 s may shed a light on the origin of high T c superconductivity.

31 nsity that points to possible unconventional superconductivity.

32 tic state and potential for high-temperature superconductivity.

33 n electronic state that hosts unconventional superconductivity.

34 ay be a primary pair glue for unconventional superconductivity.

35 p, and their connections to high-temperature superconductivity.

36 tronic quality, and clean-limit inorganic 2D superconductivity.

37 on that it may provide important clue to the superconductivity.

38 possible topological nature of the observed superconductivity.

39 Q, as anticipated when the PDW coexists with superconductivity.

40 e correlated insulator are a "mechanism" for superconductivity.

41 has reappeared in the context of topological superconductivity.

42 in which some regions show a fragile form of superconductivity.

43 the s-wave, consistent with the topological superconductivity.

44 nd understanding the origins of copper oxide superconductivity.

45 This includes superconductivity(1,2), magnetism(3), topological edge s

46 tructure, resulting in magic-angle flat-band superconductivity(1,2), the formation of moire excitons(

47 ysics is the observation of room-temperature superconductivity(1,2).

48 a wide range of emergent phenomena including superconductivity(1-3), magnetism(4), fractional Chern i

49 ronics and exciton-mediated high-temperature superconductivity(13).

50 structure has led to the recent discovery of superconductivity(3,4) and correlated insulating phases(

51 , resulting in Mott insulating behaviour and superconductivity(3,4).

52 transport properties such as unconventional superconductivity(4) and insulating behaviour driven by

53 quantum Hall effect(3) and high-temperature superconductivity(4)-and their critical roles in present

54 ideal candidates for realizing spin-triplet superconductivity(4).

55 able Mott insulators(4,5) and unconventional superconductivity(6).

56 m by the Bardeen-Cooper-Schrieffer theory of superconductivity(7-9).

57 nts in materials related to high-temperature superconductivity(8).

58 topological insulator with proximity-induced superconductivity-a promising platform to realize Majora

59 pted several fundamental questions: how does superconductivity adjust to two competing orders and are

60 he pocket, revealing the coexistence between superconductivity and antiferromagnetic ordering in the

61 iation of strange metals with unconventional superconductivity and antiferromagnetic QCPs(1-4) has le

62 by a crossover from weak- to strong-coupling superconductivity and appears upon entering the metallic

63 previously overlooked aspect of topological superconductivity and can serve as the basis for a uniqu

64 ature superconductors, the interplay between superconductivity and CDWs has become a key point in the

65 We reveal a delicate interplay between superconductivity and charge density wave and spin densi

66 ence, competition and/or cooperation between superconductivity and charge density waves (CDWs) in the

67 formation on the dynamical interplay between superconductivity and charge order.

68 possess interesting properties ranging from superconductivity and colossal magnetoresistance to phot

69 mions and broken electronic flavor symmetry; superconductivity and correlated insulators emerge from

70 gence of strongly correlated phases, such as superconductivity and correlated insulators.

71 gly peaked near the critical temperature for superconductivity and decreases with increasing doping.

72 K marked an advance towards room-temperature superconductivity and demonstrated the potential of H-do

73 erties, ranging from charge density waves to superconductivity and electrochemical activities.

74 Superconductivity and ferromagnetism are two antagonisti

75 promising platform for realizing topological superconductivity and for creating and manipulating Majo

76 ndence of the signal reveals the symmetry of superconductivity and indicates the existence of another

77 anomaly is representative of unconventional superconductivity and is interpreted as a direct signatu

78 tematic investigations of the unconventional superconductivity and its evolution with the Hubbard par

79 gnetic fields gives rise to unusual forms of superconductivity and magnetism in quantum many-body sys

80 to probe the influence of proximity-induced superconductivity and magnetism on the helical hinge sta

81 le collective phenomena in solids, including superconductivity and magnetism.

82 ndamental understanding of superfluidity and superconductivity and opens up new application possibili

83 as a platform for studying high-temperature superconductivity and other strongly correlated phenomen

84 c states of matter, including unconventional superconductivity and quantum magnetism.

85 l superconductivity because of its intrinsic superconductivity and spin-orbit-coupling.

86 s for exploring their exciting properties of superconductivity and the charge density wave (CDW).

87 reaking, especially regarding unconventional superconductivity and the interactions from which it ori

88 ect the Fermi-surface reconstruction to both superconductivity and the pseudogap phenomena.

89 nt discovery of correlated insulator states, superconductivity and the quantum anomalous Hall effect

90 ents reveal an intimate relationship between superconductivity and the unusual change in carrier dens

91 as anisotropic photodetection, electronics, superconductivity and thermoelectricity is being investi

92 re, to detect the mutual interaction between superconductivity and topological surface state, we inve

93 xide, and if so, whether the two-dimensional superconductivity and various related phenomena differ f

94 ed cuprates, the interplay of the pseudogap, superconductivity, and charge and spin ordering can give

95 the sites for doped oxygen, the mechanism of superconductivity, and practical guidelines for discover

96 , a better understanding of high-temperature superconductivity, and quantifying open quantum system d

97 ch as topological Mott state, unconventional superconductivity, and quantum spin liquid.

98 these results in the context of topological superconductivity, and show that the observed critical s

99 riety of electronic ground states, including superconductivity, antiferromagnetism, and heavy-fermion

100 Superconductivity appears in the cuprates when a spin or

101 Our results show that superconductivity appears only in those samples that hav

102 Advances in low-dimensional superconductivity are often realized through improvement

103 uantum critical phenomena and unconventional superconductivity are two major themes.

104 Neither the insulator-metal transition nor superconductivity are understood satisfactorily.

105 uprates-whose doping lies beyond the dome of superconductivity-are considered to be conventional Ferm

106 It is often speculated that high-T(c) superconductivity arises in a doped Mott insulator(1) as

107 ism of Eu coexists with the pressure-induced superconductivity around 2 GPa.

108 made to each of the dots in order to induce superconductivity, as well as probe electron transport.

109 With the discovery(1) of superconductivity at 203 kelvin in H(3)S, attention retu

110 The discovery of superconductivity at 260 K in hydrogen-rich compounds li

111 We induce superconductivity at a twist angle larger than 1.1 degre

112 The as-prepared sample exhibits bulk superconductivity at about 0.25 K, which is confirmed by

113 it is possible to maintain pressure-induced superconductivity at lower or even ambient pressures wit

114 vation of the properties of room-temperature superconductivity at lower pressures.

115 ed p-terphenyl has been fueled by reports of superconductivity at T(c) values surprisingly high for o

116 layer between the hBN and the TBG stabilizes superconductivity at twist angles much smaller than the

117 erials systems to control properties such as superconductivity, band topology, conductivity, and opti

118 , a new platform is reported for topological superconductivity based on hybrid Nb-In0.75 Ga0.25 As-qu

119 nique candidate for tunable bulk topological superconductivity because of its intrinsic superconducti

120 ates point toward a CDW state competing with superconductivity, but others raise the possibility of a

121 a prime candidate for realizing topological superconductivity by doping the topological insulator Bi

122 The capability of controlling superconductivity by light is highly desirable for activ

123 pts the question of whether high-temperature superconductivity can exist in an isolated monolayer of

124 Superconductivity can occur under conditions approaching

125 These data further indicate that superconductivity can occur without contribution from th

126 ctronic properties, such as conductivity and superconductivity, can be tuned and then used to create

127 associated with electronic phenomena such as superconductivity, colossal magnetoresistances (CMR), an

128 No superconductivity could be achieved for black phosphorus

129 ng and completely disappears precisely where superconductivity disappears.

130 h exhibit correlated states, Landau fans and superconductivity-display considerable local variation i

131 fluctuations are linked with T(C) Above the superconductivity dome, at x = 0.19, a conventional Ferm

132 Upon further cooling, signatures of superconductivity ('domes') emerge below 1 kelvin for th

133 ir potential applications in two-dimensional superconductivity, electronics, photonics, and informati

134 n extremely clean layered perovskite and its superconductivity emerges from a strongly correlated Fer

135 e of doping levels, including those at which superconductivity emerges in this system.

136 nventional superconductors is to unravel how superconductivity emerges upon cooling from the generall

137 in which the possibility of high-temperature superconductivity emerges.

138 The novel decompression-induced superconductivity enhancement implies that it is possibl

139 An unexpected superconductivity enhancement is reported in decompresse

140 en that the electron-phonon coupling affects superconductivity exponentially, this enhancement highli

141 t the interplay among charge, spin, orbital, superconductivity, ferromagnetism and ferroelectricity.

142 This mechanism provides a rare example of superconductivity from on-site Coulomb repulsion.

143 ctuations are argued to lead to spin-triplet superconductivity from pairing between opposite valleys.

144 Shedding light on the nature of spin-triplet superconductivity has been a long-standing quest in cond

145 It is the first time that superconductivity has been observed in a coordination po

146 The extraordinary superconductivity has been observed in a pressurized com

147 Correlated insulators and superconductivity have been previously observed only for

148 es, whereas correlated insulating states and superconductivity have been reported in twisted bilayer

149 In copper-oxides that show high-temperature superconductivity (HTS), the critical temperature (Tc) h

150 The discovery of unconventional superconductivity in (La,Ba)(2)CuO(4) (ref.

151 ding evidence for proximity-induced high-T c superconductivity in 1T-TaS2 with a surprisingly large e

152 strong detrimental effect of the CDW on bulk superconductivity in [Formula: see text] Using tunnel di

153 nt antiferromagnetic (AFM) order and induces superconductivity in a dome around the associated quantu

154 has been studied intensely after reports of superconductivity in a number of potassium- and rubidium

155 Here we report superconductivity in a photochemically transformed carbo

156 By combining topological band and superconductivity in a single material, they provide sig

157 l insulator state then further proceeding to superconductivity in a SOI compound BiTeI tuned via pres

158 Here we report signatures of tunable superconductivity in an ABC-trilayer graphene (TLG) and

159 Here we report the observation of superconductivity in an infinite-layer nickelate that is

160 nt in understanding and further tailoring of superconductivity in atomically thin materials.

161 n signatures, of a PDW state coexisting with superconductivity in Bi(2)Sr(2)CaCu(2)O(8+delta).

162 It is plausible that this is due to superconductivity in Bi2Se3 topological surface states i

163 pecies contributing to the recently observed superconductivity in compressed phosphine.

164 The origin of high-temperature superconductivity in copper oxides and the nature of the

165 In the quest to understand high-temperature superconductivity in copper oxides, debate has been focu

166 Suppression of superconductivity in disordered systems is a fundamental

167 The occurrence of superconductivity in doped SrTiO(3) at low carrier densi

168 microscopic mechanism underlying an enhanced superconductivity in electron-doped iron selenide superc

169 the interplay between the MI transition and superconductivity in FeSe-based materials.

170 or transition in WTe2 layers and an enhanced superconductivity in few-layer MoTe2 .

171 the issue by investigating proximity-induced superconductivity in gapped graphene and comparing norma

172 The discovery of superconductivity in H(3) S at 203 K marked an advance t

173 icroscopic mechanism underlying the enhanced superconductivity in heavily electron-doped iron-selenid

174 initio calculations phonon-mediated high-T c superconductivity in hole-doped diamond-like cubic cryst

175 ther investigate and understand conventional superconductivity in hydrogen rich superhydrides.

176 Recently, high-temperature conventional superconductivity in hydrogen-rich materials has been re

177 The onset of superconductivity in In2 Se3 occurs at 41.3 GPa with a c

178 e interactions that lead to the emergence of superconductivity in iron-based materials remain a subje

179 The results strongly suggest that superconductivity in K(2-x) Fe(4+y) Se(5) critically dep

180 This study investigates the evolution of superconductivity in K(2-x)Fe(4+y)Se(5) using temperatur

181 apped 3D time-reversal-invariant topological superconductivity in K-doped beta-PdBi(2).

182 discovery of correlated insulator states and superconductivity in magic-angle twisted bilayer graphen

183 physical control parameters for the onset of superconductivity in MB(2) C(2) hetero-graphene material

184 predict the possibility of room-temperature superconductivity in metals that have certain favourable

185 The magnetic field dependence of the superconductivity in nanocrystalline boron doped diamond

186 xpected to shed light on the growing area of superconductivity in nanostructured materials.

187 ngs hint toward magnetic fluctuation-induced superconductivity in potassium-doped p-terphenyl, which

188 erostructures resulted in the observation of superconductivity in purely carbon-based systems and rea

189 The realization of unconventional superconductivity in SLG offers an exciting new route fo

190 Finding of superconductivity in solid O2 on the border of an insula

191 n degrees of freedom, to probe the nature of superconductivity in Sr(2)RuO(4) and its evolution under

192 rectly probing the microscopic mechanisms of superconductivity in strongly correlated systems.

193 gap support the presence of the topological superconductivity in superconducting Sn(1-) (x) Pb(x) Te

194 Understanding the superconductivity in T d-MoTe2, which was proposed to be

195 heoretical explanations for the emergence of superconductivity in TBG and open up avenues towards eng

196 We infer that the proximity-induced high-T c superconductivity in the 1T-TaS2 is driven by coupling t

197 potentially shedding light on the origin of superconductivity in the cuprates.Exploration of the ele

198 It is demonstrated that proximity-induced superconductivity in the In0.75 Ga0.25 As-quantum-well 2

199 wards the goal of achieving room-temperature superconductivity in the near future.

200 enomena that complicate our understanding of superconductivity in these materials.

201 hus to understand the optimal conditions for superconductivity in thin films: which microscopic param

202 ction between the normal state responses and superconductivity in this system.

203 re observed, so the existence of topological superconductivity in topological crystalline insulators

204 al experiments to induce hidden order and/or superconductivity in U compounds with the tetragonal bod

205 reasonable explanation for the emergence of superconductivity in undoped Ca122 single crystals.

206 We report the discovery of spin-triplet superconductivity in UTe(2), featuring a transition temp

207 resent the observation of a partially melted superconductivity in which pairing fluctuations condense

208 Such universal superconductivity, independent of the chemical compositi

209 y, but others raise the possibility of a CDW-superconductivity intertwined order or more elusive pair

210 s indicate that a route to robust long-range superconductivity involves destabilizing insulating char

211 ity of BaPb1-x Bi x O3--a material for which superconductivity is "adjacent" to a competing CDW phase

212 m of high-transition-temperature (high-T(c)) superconductivity is a central problem in condensed matt

213 In cuprate superconductors, superconductivity is accompanied by a plethora of orders

214 Conventional superconductivity is caused by electron-phonon coupling.

215 proving definitively that the model supports superconductivity is challenging.

216 rt signatures of the PDW in the regime where superconductivity is destroyed by quantum phase fluctuat

217 s the evidence that in the overdoped regime, superconductivity is determined primarily by the couplin

218 The superconductivity is due to a structural transformation

219 Superconductivity is established by the observation of z

220 findings demonstrate a first ever case where superconductivity is hosted by a lattice with periodic b

221 At nu ~ -2, superconductivity is observed below critical temperature

222 in TBG in regions of the phase diagram where superconductivity is observed.

223 ransition temperature T(c) of unconventional superconductivity is often tunable.

224 so that unconventional magnetically-mediated superconductivity is possible, although a large T c valu

225 For LaH(10) and YH(10), the onset of superconductivity is predicted to occur at critical temp

226 Such superconductivity is realized via ionic gating in indivi

227 als to include actinide elements, shows that superconductivity is robust in this sub-group, and opens

228 ecessary for the "flat/steep" band model for superconductivity is satisfied in O-doped Y2 O2 Bi.

229 or the smallest twist angle of 0.79 degrees, superconductivity is still observed despite the TBG exhi

230 lly thin superconductors, with a caveat that superconductivity is strongly depleted unless enhanced b

231 ortant discovery leading to room-temperature superconductivity is the pressure-driven disproportionat

232 tly been found superconducting, the observed superconductivity is unlikely topological because of the

233 ials exhibiting correlated phenomena such as superconductivity, magnetism, and ferroelectricity have

234 and proximity to metallic states with nodal superconductivity mark this d-band system as unconventio

235 in a material that exhibits high-temperature superconductivity may not be a coincidence.

236 Superconductivity mediated by phonons is typically conve

237 hat regions with F-CDW correlations suppress superconductivity more strongly than those with AF-CDW c

238 pe-II TWSs, as well as the interplay between superconductivity (MoTe2 was discovered to be supercondu

239 This contrasts the type-I superconductivity observed for the majority of Ga phases

240 The absence of superconductivity observed in previous related experimen

241 This result verifies unconventional superconductivity of beta-Bi(2)Pd and is consistent with

242 d to understand the structure, stability and superconductivity of CeH(9).

243 Surprisingly, the role in superconductivity of electronic states originating from

244 We attribute it to intrinsic superconductivity of heavily doped individual phosphoren

245 The surface groups also control superconductivity of niobium carbide MXenes.

246 The superconductivity of the Sn(1-) (x) Pb(x) Te-Pb heterost

247 The bulk superconductivity of topological crystalline insulators

248 Superconductivity often emerges in proximity of other sy

249 We study the dependence of its superconductivity on anisotropic strain.

250 n active part, cooperating or competing with superconductivity, or may appear accidentally in such sy

251 rimental evidence of phase-tuned topological superconductivity, our devices are compatible with super

252 InSb 2DEGs and provide evidence of ballistic superconductivity over micron-scale lengths.

253 in magnetic fields large enough to suppress superconductivity, over a wide doping range(2) that incl

254 orm strain fields induce complex patterns of superconductivity, owing to the strong dependence of the

255 Its zero-resistance superconductivity persists from ambient pressure to the

256 f oxygen vacancies in different sites on the superconductivity properties of irradiated Y(Dy)BCO film

257 e of different electronic phenomena, such as superconductivity, pseudo-gap, magnetism, and density wa

258 The superconductivity realized at the interface between Bi(2

259 of superconductivity-unambiguous evidence of superconductivity reflecting chiral structure in which t

260 erconductors, and their role in establishing superconductivity remains an open question.

261 erspective on the nature of high-temperature superconductivity (SC).

262 m structurally homogeneous mixed valency, to superconductivity, spectral anomalies, and unexplained p

263 rial platform to study the interplay between superconductivity, spin-orbit interaction and magnetism.

264 T N beyond a critical doping level at which superconductivity starts to emerge, and scales with the

265 terrelation of nematicity and unconventional superconductivity, suggesting nematicity to be common am

266 ng such diverse phenomena as ferromagnetism, superconductivity, superfluidity and the Higgs mechanism

267 found to be necessary to access topological superconductivity that hosts Majorana modes (non-Abelian

268 nd signatures of coexisting Kondo effect and superconductivity that show competing spatial modulation

269 structure and correlation phenomena (such as superconductivity) that are determined by both the atomi

270 phases of matter, including high-temperature superconductivity, the fractional quantum Hall effect, q

271 2212 become extremely tunable; our survey of superconductivity, the pseudogap, charge order and the M

272 m technology, with applications ranging from superconductivity to biosensing, the realization of a st

273 s, relevant in active areas of research from superconductivity to resistive memory to catalysis.

274 High magnetic fields suppress cuprate superconductivity to reveal an unusual density wave (DW)

275 We attribute the glassy superconductivity to the morphological granularity of th

276 e pseudogap has been attributed to precursor superconductivity, to the existence of preformed pairs a

277 promising platform for realizing topological superconductivity (TSC).

278 Here we report the nonreciprocity of superconductivity-unambiguous evidence of superconductiv

279 ting new route for the development of p-wave superconductivity using two-dimensional materials with t

280 cular, we find signatures of odd-parity bulk superconductivity via upper-critical field and magnetiza

281 (x))(2) exhibits multiple evidence for nodal superconductivity via various experimental probes, such

282 Recently, superconductivity was discovered in thin films of the in

283 Superconductivity was evidenced by the observation of ze

284 Unconventional superconductivity was predicted in single-layer graphene

285 Proximity-effect-induced superconductivity was studied in epitaxial topological i

286 Non-saturating magnetoresistance and superconductivity were also observed in T d-MoTe2.

287 t antiferromagnetism and experimentally show superconductivity when doped, the hexagonal forms of FeS

288 ed Mott insulators, such as high-temperature superconductivity, whereas the half-filled parent state

289 opose a versatile mechanism for spin-triplet superconductivity which emerges through a melting of mac

290 lows the Bardeen-Cooper-Schrieffer theory of superconductivity, which describes the condensation of e

291 of strong-correlation physics(2-5), notably superconductivity, which emerges close to interaction-in

292 The nematic fluctuations induce superconductivity with a broad dome in the superconducti

293 escribed by a model based on strong coupling superconductivity with a coupling constant lambda ~ 2.

294 Here we report superconductivity with a critical temperature of around

295 Upon proper annealing, superconductivity with a T(c) up to 25 K emerges in the

296 .41(1) angstrom and exhibits phonon mediated superconductivity with a transition temperatures T(c) ~

297 umerous long-standing predictions for exotic superconductivity with fragile pairing symmetries.

298 lations plays a key role in realizing robust superconductivity with high-Tc and high-Hc2.

299 esistant refractory metals that also exhibit superconductivity with large upper critical fields.

300 e the feasibility of sustaining spin-triplet superconductivity with this mechanism by considering a n