ライフサイエンスコーパス: superconductivity

1 t becomes hidden by a dome of unconventional superconductivity.

2 up complex new possibilities for topological superconductivity.

3 he normal state is possibly the precursor of superconductivity.

4 agnetism is usually deemed incompatible with superconductivity.

5 r between individual layers does not destroy superconductivity.

6 role of electron correlations in the high-Tc superconductivity.

7 g effects such as the optical enhancement of superconductivity.

8 omalous metallic behavior and unconventional superconductivity.

9 gle crystals is almost 100%, confirming bulk superconductivity.

10 tronic properties including room-temperature superconductivity.

11 r concomitant suppression of phonon-mediated superconductivity.

12 ations lie at the origin of high-temperature superconductivity.

13 d test the effect of alloy complexity on the superconductivity.

14 vidence for prevailing phase fluctuations of superconductivity.

15 tallic conductivity, magnetic scattering and superconductivity.

16 ogap, non-Fermi liquids and high-temperature superconductivity.

17 rge balance is required in order to preserve superconductivity.

18 furnishes the development of unconventional superconductivity.

19 the 2D states, which is responsible for the superconductivity.

20 behaviour, heavy-fermions, or unconventional superconductivity.

21 uld be closely related to the suppression of superconductivity.

22 spin- and charge-order, and high-temperature superconductivity.

23 ue to the possibility of hosting topological superconductivity.

24 ent results in diminishing Tc and filametary superconductivity.

25 pper oxide superconductors and competes with superconductivity.

26 an essential ingredient of high-temperature superconductivity.

27 low-energy electronic properties, including superconductivity.

28 ions regarding the nature of one-dimensional superconductivity.

29 arameter in probing spin-fluctuation-induced superconductivity.

30 ntum ordered states such as high temperature superconductivity.

31 h present clear signatures of unconventional superconductivity.

32 many-body physics, such as high-temperature superconductivity.

33 tronic properties of the material, including superconductivity.

34 by quantum effects, such as superfluidity or superconductivity.

35 mmetries distinct from those associated with superconductivity.

36 suggested that charge ordering competes with superconductivity.

37 can be tailored to achieve high-temperature superconductivity.

38 d states, such as magnetism, charge order or superconductivity.

39 n the order parameters for the pseudogap and superconductivity.

40 scribe the essential details of copper oxide superconductivity.

41 as well as fundamental studies of mesoscopic superconductivity.

42 ergent geometry of the spatial landscape for superconductivity.

43 rsion of spintronics based on unconventional superconductivity.

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

45 c order to nontrivial topological phases and superconductivity.

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

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

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

49 nsity that points to possible unconventional superconductivity.

50 tic state and potential for high-temperature superconductivity.

51 n electronic state that hosts unconventional superconductivity.

52 ay be a primary pair glue for unconventional superconductivity.

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

54 On the other hand superconductivity, a commonly believed competing order,

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

56 er slightly above 2 mK and of heavy-electron superconductivity almost concomitantly with this order.

57 The multiband superconductivity along with electron-hole compensation

58 onstraints on the theoretical description of superconductivity and allow a unified understanding of t

59 ile hidden order provides an environment for superconductivity and anomalous metallic behavior, it's

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

61 na modes in nanowires with proximity-induced superconductivity and atomic chains, with small amounts

62 be accompanied by anomalous fluctuations of superconductivity and certain lattice phonons.

63 onductors, a rich competition occurs between superconductivity and charge density wave (CDW) order.

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

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

66 astonishing phenomena, for example, high-Tc superconductivity and colossal magnetoresistance (CMR) i

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

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

69 clusters as a favorable structural motif for superconductivity and develop empirical, molecule-based,

70 The coexistence and competition between superconductivity and electronic orders, such as spin or

71 Superconductivity and ferromagnetism are two antagonisti

72 the freestanding case of the coexistence of superconductivity and ferromagnetism in one two-dimensio

73 reported long-range proximity effect between superconductivity and ferromagnetism in YBCO/LCMO hetero

74 Consequently, the coexistence of superconductivity and ferromagnetism is usually observed

75 ergent properties such as unusual magnetism, superconductivity and heavy fermion behaviour, have been

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

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

78 The interplay of superconductivity and magnetism is a subject of ongoing

79 ly generalizable example of a material where superconductivity and magnetism may be intertwined.

80 ties at these novel quantum wells-such as 2D superconductivity and magnetism-are intimately connected

81 ssue in cuprates is the relationship between superconductivity and magnetism.

82 e observation of gate electric-field-induced superconductivity and metal-insulator transitions.

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

84 electrons and phonons that can also lead to superconductivity and other competing or entangled phase

85 ctrolyte gating is well suited to studies of superconductivity and other phenomena robust to disorder

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

87 is potentially relevant to high-temperature superconductivity and quantum-information applications,

88 ody Hubbard phenomena such as unconventional superconductivity and spin liquids are more difficult to

89 The occurrence of magnetic interactions, superconductivity and spin-orbit coupling in the same q2

90 nables investigation of an interplay between superconductivity and strongly correlated states in a tw

91 The observation of superconductivity and systematic Tc changes with nanostr

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

93 realizing hybrid systems in the search of 2D superconductivity and the design of novel electronic het

94 nced thermoelectric performance, topological superconductivity and the near-room-temperature quantum

95 cal point may provide an explanation for the superconductivity and the order parameter.

96 ve been argued to be the cause of the d-wave superconductivity and the pseudogap phenomena exhibited

97 logical states and excitations is to combine superconductivity and the quantum Hall (QH) effect.

98 e spatial extension and anisotropy of the 2D superconductivity and the Rashba spin-orbit field can be

99 d most recently by the discovery of Fe-based superconductivity and the recognition that spin-fluctuat

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

101 raised the question of the interplay between superconductivity and this competing phase.

102 provides insights into the interplay between superconductivity and topological physics.

103 ing large magnetoresistance, pressure-driven superconductivity and Weyl semimetal states.

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

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

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

107 n understanding of spin-mediated pairing for superconductivity; and resonant inelastic X-ray scatteri

108 Superconductivity appears in the cuprates when a spin or

109 d moment continuously decreases, yielding to superconductivity approximately x=0.05.

110 eoretical proposals that both nematicity and superconductivity are driven by spin fluctuations.

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

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

113 pplication is the realization of topological superconductivity as a basis for quantum information pro

114 excellent intermediate systems for studying superconductivity as it evolves between crystalline and

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

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

117 ing the hope for the possible realization of superconductivity at high pressure.

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

119 Together with recent studies of superconductivity at oxide heterostructure interfaces, t

120 We argue that the survival of superconductivity at Zeeman energies much larger than th

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

122 many spectacular electronic properties, with superconductivity being arguably the most notable except

123 Here, we report the observation of superconductivity below 20 K in surface electron-doped b

124 ing transition temperature and competes with superconductivity below this temperature for electronic

125 te can be destabilized toward unconventional superconductivity by either hole or electron doping.

126 ce by quantum oscillations on suppression of superconductivity by high applied magnetic fields, toget

127 allic magnetic state of FeTe is tuned toward superconductivity by substitution of a small amount of t

128 t the only known Fe-based material, in which superconductivity can be smoothly connected to the Mott-

129 ectronic correlations, such as magnetism and superconductivity, can be produced as the result of enha

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

131 e underdoped copper-oxides, high-temperature superconductivity condenses from a nonconventional metal

132 re we propose an alternative route to chiral superconductivity, consisting of the surface of an ordin

133 No superconductivity could be achieved for black phosphorus

134 n Fermi level pinning effect and, therefore, superconductivity could be generally used to probe and o

135 The theory of superconductivity developed by Bardeen, Cooper and Schri

136 ntertwined electronic orders in solids, with superconductivity developing from a charge-density wave

137 Iron-based superconductivity develops near an antiferromagnetic ord

138 he paper discusses fundamentals of record-TC superconductivity discovered under high pressure in sulf

139 Superconductivity emerges at Tc.

140 helimagnet CrAs has raised questions on how superconductivity emerges from the magnetic state and on

141 s of magnitude modulation in resistance, and superconductivity emerges in a textured charge-density w

142 Here we report that superconductivity emerges upon Se doping in CDW conducto

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

144 An unexpected superconductivity enhancement is reported in decompresse

145 ies could result in S/F hybrids that support superconductivity even when locally the vortex density e

146 c spectrum in the pseudogap phase from which superconductivity evolves.

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

148 The quantum spin Hall effect, chiral superconductivity, giant magnetoresistance and various e

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

150 Superconductivity has been reversibly induced/suppressed

151 enhancement of the electron-phonon coupling, superconductivity has never been observed.

152 quantum critical point, hidden by a dome of superconductivity, has been explicitly revealed and foun

153 ating magneto-resistance and pressure-driven superconductivity have been observed.

154 Superfluidity and superconductivity have been widely studied since the las

155 Recent developments in high-temperature superconductivity highlight a generic tendency of the cu

156 s of quantum critical points associated with superconductivity, however, has made it difficult to unr

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

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

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

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

161 We report robust superconductivity in all Ca-doped graphene laminates.

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

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

164 Since the discovery of superconductivity in boron-doped diamond with a critical

165 esistivity measurements demonstrate that the superconductivity in bulk polycrystalline hexagonal epsi

166 c quantum criticality promote unconventional superconductivity in CeRhIn5.

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

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

169 transition temperature (T c) of 10.6 K, and superconductivity in CrH3 is enhanced by the metallic hy

170 t to understand the electronic structure and superconductivity in cubic and tetragonal TiH2.

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

172 Here, we demonstrate superconductivity in ferecrystals: turbostratically diso

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

174 e metal layer, our work shows that achieving superconductivity in free-standing, metal decorated mono

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

176 find that Ca is the only dopant that induces superconductivity in graphene laminates above 1.8 K amon

177 Our device is designed to induce superconductivity in graphene via the proximity effect,

178 cal predictions regarding the possibility of superconductivity in graphene, its direct and unambiguou

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

180 The nature of superconductivity in hexagonal epsilon-NbN and the physi

181 Here we report induced superconductivity in high-mobility two-dimensional elect

182 e helpful for understanding the mechanism of superconductivity in high-Tc iron-based superconductors

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

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

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

186 xperimental basis for a successful theory of superconductivity in iron-based materials which takes in

187 Ever since the discovery of high-Tc superconductivity in layered cuprates, the roles that in

188 d was ignited by reports of high-temperature superconductivity in materials obtained by the reaction

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

190 will guide the future search for topological superconductivity in noncentrosymmetric materials.

191 Here we report the new discovery of superconductivity in polycrystalline hexagonal epsilon-N

192 to be correct and leads to the discovery of superconductivity in ReGa5.

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

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

195 Observations of robust superconductivity in some of the iron based superconduct

196 The results offer a new pathway to control superconductivity in spintronic devices.

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

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

199 The recent discovery of pressure (p) induced superconductivity in the binary helimagnet CrAs has rais

200 The discovery of high-temperature superconductivity in the copper oxides in 1986 triggered

201 Superconductivity in the cuprates exhibits many unusual

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

203 he interplay between ideal Weyl fermions and superconductivity in the half-Heusler compound LaPtBi.

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

205 Despite this potential, signatures of superconductivity in the QH regime remain scarce, and a

206 Our results demonstrate that superconductivity in the vicinity of quantum criticality

207 The uniformity of superconductivity in these thin films is established by

208 demonstrate that the dramatic enhancement of superconductivity in this compound correlates closely wi

209 remarkable consistency and demonstrate that superconductivity in this material is rather weak and me

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

211 rect evidence to date for interface-enhanced superconductivity in undoped Ca122, consistent with the

212 We searched for superconductivity in weakly interacting, metal decorated

213 Such universal superconductivity, independent of the chemical compositi

214 arge ordering (CO) instability competes with superconductivity inside the pseudogap state.

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

216 Conventional superconductivity is caused by electron-phonon coupling.

217 a maximum near x approximately 0.01 and that superconductivity is destroyed near x approximately 0.02

218 ic critical threshold value beyond which the superconductivity is destroyed.

219 The superconductivity is due to a structural transformation

220 At low density, where superconductivity is found in the analogous 2DEL at the

221 n the disordered phase, and the promotion of superconductivity is likely to emerge from an enhanced c

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

223 Such superconductivity is realized via ionic gating in indivi

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

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

226 A key actor in the conventional theory of superconductivity is the induced interaction between ele

227 A central question in iron-based superconductivity is the mechanism by which the paired e

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

229 in and charge ordering and their relation to superconductivity, is intensely debated.

230 he search for mechanisms of high-temperature superconductivity it is critical to know the electronic

231 )(Fe2As2)5 provides opportunities to explore superconductivity layer by layer, because it contains bo

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

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

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

235 oulomb pair-breaking (which usually destroys superconductivity) may be averted due to a screened long

236 It was theoretically proposed that superconductivity might be induced by enhancing the elec

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

238 chnologically promising phenomena related to superconductivity, multiferroicity, mangetoresistivity,

239 C2 local symmetry, whose emergence precedes superconductivity, naturally accounts for a propensity f

240 S topology are favourable conditions for the superconductivity, not only for iron chalcogenides, but

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

242 Nevertheless, superconductivity occurs at the quantum critical point o

243 Superconductivity occurs via the formation of a compound

244 o play a critical role in the unconventional superconductivity of cuprates, Fe-based and heavy-fermio

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

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

247 perature, melting temperature and a possible superconductivity of hexagonal epsilon-NbN all increase

248 We argue that superconductivity of n-doped SrTiO3 results from the int

249 Superconductivity of n-doped SrTiO3, which remained enig

250 ffects of polytypism and polymorphism on the superconductivity of TaSe2, one of the archetypal member

251 Dynamical stability and superconductivity of tin hydrides are systematically inv

252 Superconductivity often emerges in proximity of other sy

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

254 A recently experimental discovered of superconductivity on the border of long-range magnetic o

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

256 from 850 degrees C, reveals the emergence of superconductivity over a narrow time window.

257 The observed dome-shaped superconductivity phase diagram provides insights into t

258 or developments in fields such as magnetism, superconductivity, photonics and electronics.

259 s the phase separation between magnetism and superconductivity point to a conventional mechanism of t

260 Surprisingly, superconductivity re-appeared rapidly above 13 GPa, with

261 Our results suggest that the superconductivity recently observed by Drozdov, Eremets,

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

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

264 ithout magnetism whose relationship with its superconductivity remains unclear.

265 imensional crossover and to the spin triplet superconductivity, remains elusive.

266 This CDW coexists and competes with superconductivity (SC) below the transition temperature

267 including fundamental problems in mesoscopic superconductivity, scalable superconducting electronics,

268 ver, in a large region of the phase diagram, superconductivity sets in from a ferromagnetic normal st

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

270 made superconducting strips a mainstream of superconductivity studies.

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

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

273 omain walls define many important effects in superconductivity, superfluidity, magnetism, liquid crys

274 pproximately 6 GPa the sudden enhancement of superconductivity (Tc</=38.3 K) accompanies a suppressio

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

276 ditional Bardeen-Cooper-Schrieffer theory of superconductivity, the amplitude for the propagation of

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

278 subtle forms of matter, such as magnetism or superconductivity, they can even cause the electrons in

279 asurements strongly evidences unconventional superconductivity through a spontaneous appearance of an

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

281 a, and report the lightest system to exhibit superconductivity to date.

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

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

284 The spin-fluctuation mechanism of superconductivity usually results in the presence of gap

285 Superconductivity was discovered in the layered compound

286 No superconductivity was observed down to 4.3 K in (NH3)yCs

287 Unconventional superconductivity was predicted in single-layer graphene

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

289 ly identify non-equilibrium high-temperature superconductivity, we propose this as a possible explana

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

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

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

293 tstanding mechanical/elastic properties with superconductivity, which may be particularly attractive

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

295 find that C6CaC6 can support phonon-mediated superconductivity with a critical temperature Tc = 6.8-8

296 ntercalated Bi2Se3 has been reported to show superconductivity with a Tc ~ 3 K and a large shielding

297 We find that bulk MoTe2 exhibits superconductivity with a transition temperature of 0.10

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

299 ry phases, metal-insulator-metal transition, superconductivity with one of the highest elemental tran

300 Here, we report the observation of superconductivity with Tc above 100 K in the FeSe/STO sy