ライフサイエンスコーパス: superconductor

1 ra near zero bias, consistent with a trivial superconductor.

2 ation is one of the defining properties of a superconductor.

3 t may accidentally occur at zero energy in a superconductor.

4 lous Hall insulator thin film coupled with a superconductor.

5 rise to Majorana physics without invoking a superconductor.

6 logical MZMs from trivial in-gap states of a superconductor.

7 oxygen, the layered Y2 O2 Bi phase becomes a superconductor.

8 alogous to a Bardeen-Cooper-Schrieffer (BCS) superconductor.

9 ization of the Kitaev model of a topological superconductor.

10 rbit coupling is brought into contact with a superconductor.

11 nano-structures proximity-coupled to a bulk superconductor.

12 three-dimensional (p-wave) non-conventional superconductor.

13 ns, the insulating (TaSe(4) )(2) I becomes a superconductor.

14 been identified as the parent phase of FeSe superconductor.

15 nd that the undoped bulk system is a trivial superconductor.

16 d to a magnetic flux vortex in a topological superconductor.

17 ered near-room-temperature lanthanum hydride superconductors.

18 m reminiscent of high-transition-temperature superconductors.

19 are believed to be very promising high-T(c) superconductors.

20 st-principles framework fails in the cuprate superconductors.

21 logy is a fundamental property of metals and superconductors.

22 etermining the sign change of unconventional superconductors.

23 elated materials, including high-temperature superconductors.

24 t the critical temperature in unconventional superconductors.

25 ise to pseudogap states and high-temperature superconductors.

26 cal magnetic field or a critical current for superconductors.

27 w classes of potential very high-temperature superconductors.

28 fermions is a promising path to topological superconductors.

29 son junction arrays, and certain narrow band superconductors.

30 remain the focus in the research of cuprate superconductors.

31 aterials, ranging from insulating magnets to superconductors.

32 the enhancement of Tc over other FeSe-based superconductors.

33 nickelate La4Ni3O10 compared to the cuprate superconductors.

34 conductors (MIECs), He-ion implantation, and superconductors.

35 determine key electromagnetic properties of superconductors.

36 CS) arguments indicate they might be high-Tc superconductors.

37 netic nano-devices based on high temperature superconductors.

38 on materials, including the high-temperature superconductors.

39 mistry to generate a library of e.g. cuprate superconductors.

40 the parent state of cuprate high-temperature superconductors.

41 ent properties in magnetic fields over other superconductors.

42 d it limits the current-carrying capacity of superconductors.

43 behavior is a universal one among iron based superconductors.

44 and practical guidelines for discovering new superconductors.

45 and resistance-free electric current flow in superconductors.

46 of light reflected from the surface of some superconductors.

47 a2-xSrxCoO4 and many hole-doped copper oxide superconductors.

48 of vortex bound states on FeTe(0.55)Se(0.45) superconductors.

49 uivalent of the intermediate state in type I superconductors.

50 ological materials, and putative topological superconductors.

51 h has a close analogy with high T(c) cuprate superconductors.

52 crystals, metal-dichalcogenides, magnets and superconductors.

53 a range of applications including lasers and superconductors.

54 ossible relation to high-[Formula: see text] superconductors.

55 ed to exist at the boundaries of topological superconductors.

56 ong spin-orbit coupling proximity coupled to superconductors.

57 s those believed to emerge in unconventional superconductors.

58 that is a common value for high-temperature superconductors.

59 theory or even observed in high-temperature superconductors.

60 metallic hydrogen state or high-temperature superconductors.

61 xperiments on spin injection in proximitized superconductors.

62 ature copper oxides and other unconventional superconductors(1-3), which suggests that MATBG may be a

63 to similar observations in high-temperature superconductors(15-21) provides new evidence of a deeper

64 tates, including correlated insulators(1-3), superconductors(2-4) and topological phases(3,5,6).

65 of the transition metal dichalcogenide (TMD) superconductor 2H-niobium disulfide (2H-NbS(2)) and a co

66 en electrons gives rise to Cooper pairing in superconductors(3).

67 gly correlated electrons in high-temperature superconductors(9).

68 idering a new class of quasi-one-dimensional superconductors A(2)Cr(3)As(3) (A = K, Rb, and Cs).

69 c modulus for ceramic and single crystalline superconductors alike.

70 est the possibility of a family of nickelate superconductors analogous to copper oxides(24) and pnict

71 provide a comprehensive treatment of how the superconductor and its properties are affected by the tr

72 Metallic hydrogen may be a room-temperature superconductor and metastable when the pressure is relea

73 identify a new extraordinary electron-phonon superconductor and pave the way for further exploration

74 SLG on an electron-doped (non-chiral) d-wave superconductor and performing local scanning tunnelling

75 icroscopy images of a Co-doped iron arsenide superconductor and prove that the application of the alg

76 eous and barrier-free interfaces between the superconductor and semiconductor.

77 ifferences in the pinning landscape when the superconductor and the ferromagnet are electron ically c

78 fect of stray magnetic fields from both, the superconductor and the ferromagnet in hybrid magnetic na

79 rolled and transparent interface between the superconductor and the QAH insulator.

80 cosmic microwave background polarization to superconductors and biological materials.

81 instability known to occur in hydrodynamics, superconductors and Bose-Einstein condensates.

82 nfined sheets and in thermodynamic phases of superconductors and chiral liquid crystals.

83 istinctions between the newly found Ni-based superconductors and cuprates.

84 tates have been reported in high-temperature superconductors and dilute magnetic semiconductors, they

85 ly analogous to the CuO(2) sheets in cuprate superconductors and hole doping (Ni(1+/2+) , Ru(2+) ) or

86 structurally compatible both with binary TMN superconductors and main-group nitride semiconductors al

87 sceptibility across the cuprates, iron-based superconductors and many heavy fermion materials.

88 en in tunnelling spectra in high temperature superconductors and that this feature arises from excita

89 sm in the parent compounds of unconventional superconductors and their superconducting phase is impor

90 tructure, with the aim of finding additional superconductors and understanding the origins of copper

91 From topological insulators to topological superconductors and Weyl semimetals, it is now understoo

92 logical superconductors, helical topological superconductors and Weyl semimetals.

93 the copper- and iron-based high-temperature superconductors, and their role in establishing supercon

94 measurements on commercial high-temperature superconductors are combined with large-scale time-depen

95 uantum materials such as antiferromagnets or superconductors are complex in that chemical, electronic

96 Spin-triplet superconductors are condensates of electron pairs with s

97 Superconductors are excellent testbeds for studying vort

98 The properties of cuprate high-temperature superconductors are largely shaped by competing phases w

99 central phenomena of cuprate (copper oxide) superconductors are linked by a common doping level p*-a

100 SOFCs) and oxygen-deficient high-temperature superconductors are poised for power transmission and ma

101 Chains of quantum dots coupled to superconductors are promising for the realization of the

102 Yet, topological superconductors are rare to date.

103 ications like sensors and detectors using 2D superconductors are still lacking.

104 s localized at the boundaries of topological superconductors-are expected to be ideal building blocks

105 y properties of the cuprate high-temperature superconductors arise from doping a strongly correlated

106 Co chalcogenides are ferromagnets instead of superconductors as in their iron analogues.

107 damental physics of dynamic vortex states of superconductors at high current densities, crucial for m

108 n of discovering new hydrogen-rich high-T(c) superconductors at lowest possible pressure, here we rep

109 served in heavy-fermion(6) and iron-based(7) superconductors at the point where their antiferromagnet

110 c quantum phenomena, having been realized in superconductors, atomic gases, and liquid helium.

111 c monolayer crystals of the high-temperature superconductor Bi(2)Sr(2)CaCu(2)O(8+delta) (Bi-2212; her

112 en freshly exfoliated flakes of the high-T c superconductor, Bi-2212, and the CDW-dominated TMD layer

113 e1+yTe, the parent compound of Fe1+ySe1-xTex superconductors, bulk-sensitive neutron diffraction reve

114 d the knowledge on this important commercial superconductor but also are helpful for a better underst

115 erfeld coefficient as for a disordered nodal superconductor, but occurring even in the pure case.

116 currents define eletromagnetic properties of superconductors, but it remains unexplored.

117 rmine the topological state of the resulting superconductor by measuring the tunnelling conductance a

118 ic sublattices in them and the tunability to superconductors by chemical doping or application of ext

119 vely, for the first time in an iron-pnictide superconductor, CaKFe(4)As(4).

120 First, we show that a topologically trivial superconductor can be driven into a chiral topological s

121 Under certain conditions, a fermion in a superconductor can separate in space into two parts know

122 ted for the layered cuprate high-temperature superconductors can be achieved by breaking away from th

123 Topological superconductors can support localized Majorana states at

124 ucting state in samples of the heavy-fermion superconductor CeIrIn(5) We pattern crystals by focused

125 tuating nematic character in a heavy-fermion superconductor, CeRhIn5 (ref.

126 ansitions of driven flux lines in high-T (c) superconductors, charged colloids, and grain transport i

127 Here we report a high-temperature superconductor coil that generates a magnetic field of 1

128 Here we report a high-temperature superconductor coil that generates a magnetic field of 1

129 ive magnet inside 11.4-tesla low-temperature superconductor coils(1), and such high-power resistive m

130 T(C) and the H(C2) among all the known alloy superconductors composed of only transition metal elemen

131 Although copper oxide high-temperature superconductors constitute a complex and diverse materia

132 , an insulating analogue of the copper oxide superconductors containing cobalt in place of copper.

133 can only exist on the surface of topological superconductors, Dirac and Weyl fermions can be realized

134 tructures comprised of a conventional s-wave superconductor (e.g. Nb, Al) and either strongly spin-po

135 However, iron-chalcogenide superconductors, especially Fe(Te,Se), suffer from stron

136 inhomogeneous superfluids in unconventional superconductors, excluding chemical disorder and inter-b

137 ant drive the moving vortex state in 2H-NbS2 superconductor exhibits a negative differential resistan

138 iring in the M(x)Bi(2)Se(3) (M = Cu, Sr, Nb) superconductor family.

139 eby spin supercurrents can be manipulated in superconductor/ferromagnet proximity systems via nonequi

140 phase in iron-based high-[Formula: see text] superconductors (FeSC), as in other unconventional super

141 between competing interactions in iron-based superconductors (FeSCs) can be tipped by additional inte

142 is signature is absent in DWs in the related superconductor, FeSe, which is not in the topological ph

143 at the interface between Bi(2)Te(3) and non-superconductor FeTe is one such candidate.

144 y inhomogeneous superfluid in the iron-based superconductor FeTe(0.55)Se(0.45).

145 tical current density J e because of the low superconductor fill factor in a complicated layered stru

146 Electron pairing in the vast majority of superconductors follows the Bardeen-Cooper-Schrieffer th

147 show a transition from a Mott insulator to a superconductor for the first time in three-dimensional m

148 trast with the behavior expected of a d-wave superconductor, for which both magnetic and nonmagnetic

149 tabilization of a weak-coupling type-II-like superconductor ([Formula: see text] [Formula: see text]

150 The cuprate superconductor [Formula: see text], in comparison with m

151 ermal conductivity of graphene, we develop a superconductor-graphene-superconductor Josephson junctio

152 g spin-valve effect with a T c change 1 K in superconductor/half-metal structures, in which case our

153 fluid of unconventional, strongly correlated superconductors has been suggested(1-7), it is not known

154 The rise of two-dimensional (2D) crystalline superconductors has opened a new frontier of investigati

155 In addition, some iron-pnictide superconductors have been demonstrated to have topologic

156 Iron-chalcogenide superconductors have emerged as a promising Majorana pla

157 waves (CDWs) in the cuprate high-temperature superconductors have evoked much interest, yet their typ

158 Edge supercurrents in superconductors have long been an elusive target.

159 ensional time-reversal-invariant topological superconductors, have evaded discovery in bulk intrinsic

160 um anomalous Hall effect, chiral topological superconductors, helical topological superconductors and

161 ic behaviour in a prototypical heavy-fermion superconductor highlights the interrelation of nematicit

162 One-dimensional topological superconductors host Majorana zero modes (MZMs), the non

163 epsilon) measurements on a high temperature superconductor (HTS), a (Rare-Earth)Ba(2)Cu(3)O(7-delta)

164 High-temperature superconductors (HTS) could enable high-field magnets st

165 rconducting proximity effect observed in QAH-superconductor hybrid devices and shows that the half-qu

166 The nematic phase in iron based superconductors (IBSs) has attracted attention with a no

167 shorter than the one predicted for the same superconductor in a uniform magnetic field equal to the

168 All superconductors in high field magnets operating above 12

169 gnetic adatoms on the surface of a thin-film superconductor, in which the control over an externally

170 e short coherence length in high-temperature superconductors, in the model of free charge carriers th

171 2 is different from that of other iron-based superconductors, including Co-doped or P-doped BaFe2As2.

172 nductor-normal metal transition (SMT) to the superconductor-insulator transition (SIT) via the interm

173 terlayer resonant conditions, resulting in a superconductor-insulator transition at magic twist angle

174 range from criticality of quantum metal- and superconductor-insulator transitions to the effects of c

175 inhomogeneity at a ferromagnet/spin-singlet-superconductor interface.

176 of an unusually large zero-energy peak in a superconductor interfaced with a half-metal, which even

177 The superconductor iron selenide (FeSe) is of intense intere

178 Topological superconductor is attracting growing interest for its po

179 us Hall (QAH) insulator coupled to an s-wave superconductor is predicted to harbor chiral Majorana mo

180 The chiral p-wave superconductor is the archetypal example of a state of m

181 of the Ising-like nematic phase in Fe-based superconductors is also presented.

182 h opens in the under-doped regime of cuprate superconductors is one of the most enduring challenges o

183 A pivotal challenge posed by unconventional superconductors is to unravel how superconductivity emer

184 al, which is a '122' parent of iron arsenide superconductors, is found through synthesis to have orde

185 In cuprate superconductors, it has been well established that the g

186 to most previous works, we focus on how the superconductor itself is influenced by the proximity eff

187 aphene, we develop a superconductor-graphene-superconductor Josephson junction(8-13) bolometer embedd

188 roaches to THz-frequency generation based on superconductor Josephson junctions (JJ), free electron l

189 ed supercurrents in ferromagnet/spin-triplet-superconductor junctions can be controlled by the angle

190 hermopower (S) of the electron-doped cuprate superconductor La(2-x) Ce (x) CuO(4) (LCCO) from x = 0.1

191 resonant x-ray scattering in stripe-ordered superconductors (La,M)2CuO4 to probe the relationship be

192 High temperature (high-Tc) superconductors like cuprates have superior critical cur

193 nergy dissipation limitation in conventional superconductor logic families such as rapid-single-flux-

194 Flux-Parametron (AQFP) logic is an adiabatic superconductor logic family that has been proposed as a

195 BCO) coated conductor, and a low temperature superconductor (LTS), a Nb(3)Sn wire, that include the v

196 ndamental to classical and quantum vortices, superconductors, magnetic flux tubes, liquid crystals, c

197 re the essential physics of high-temperature superconductors, magnetic insulators and other complex q

198 predictions(11) for high-field copper oxide superconductor magnets by achieving a field twice as hig

199 ve method for altering the properties of the superconductor material Bi2Sr2CaCu2O8+delta (Bi2212).

200 copolymer-directed metal, semiconductor, and superconductor materials.

201 second class of high-Tc materials, Fe-based superconductors, may provide another option for high-fie

202 emission of coherent terahertz radiation5,6, superconductor-metal oscillations7 and soliton formation

203 d how quantum phase coherence evolves across superconductor-metal-insulator transitions through magne

204 The anti-perovskite superconductor MgC0.93Ni2.85 was studied using high-reso

205 ce of a robust edge supercurrent in the Weyl superconductor molybdenum ditelluride (MoTe(2)).

206 Hybrid semiconductor-superconductor nanowires have emerged as a promising pla

207 a smooth crossover from the disorder-driven superconductor-normal metal transition (SMT) to the supe

208 id evidences exist in several unconventional superconductors of ubiquitous critical fluctuations asso

209 he recently discovered 'two-dimensional (2D) superconductor' of single-layer FeSe also exhibits 1D to

210 This result places iron-based superconductors on equal footing with copper oxide super

211 p possibilities for manipulating topological superconductors on the device-friendly platform of monol

212 agnetic ground states relevant to iron-based superconductors-one single-Q and two double-Q phases.

213 hile many materials are found to be either a superconductor or a topological insulator, it is very ra

214 havior has been observed in other iron based superconductors, our observation confirms that the behav

215 ogenide (TMD)s as candidates for topological superconductors out of such momentum-space-split spinles

216 behaves as a strong-coupled orbital-limited superconductor over the entire range of temperatures and

217 Spin-triplet superconductors potentially host topological excitations

218 dal compounds to high-transition-temperature superconductors, proteins, ultrathin magnetic films, liq

219 he magnetic properties of K(2-x)Fe(4+y)Se(5) superconductors, providing deeper insight into the elect

220 a lattice, gauge theories, high-temperature superconductors, quantum spin liquids, and systems with

221 The discovery of high-temperature superconductors raised the question of whether such stro

222 ure dependence, is omnipresent in disordered superconductors - ranging from high-temperature cuprates

223 Since superconductors rarely exhibit strong photoresponses, an

224 he upper critical field Hc2 of the fulleride superconductors reaches values as high as approximately

225 nductor nanowire networks in the topological superconductor regime.

226 The systems studied are high temperature superconductor-related materials, spin-orbit Mott insula

227 conductivity in electron-doped iron selenide superconductor remains unclear.

228 rties of cuprates and other high-temperature superconductors remains controversial despite decades of

229 t promotes nanoscale phase separation in the superconductor resulting in lower disparity and strong s

230 hat heavily overdoping a Bi2Sr2CaCu2O8+delta superconductor results in a decline of the conventional

231 Recent discoveries from superconductor (S)/ferromagnet (FM) heterostructures inc

232 te energy bands that is much larger than the superconductor's energy gap.

233 mising for the development of Ferromagnet(F)/Superconductor(S)/Ferromagnet(F) pseudo spin-valve devic

234 structure exhibits the synergic influence of superconductor (SC) - ferromagnetic (FM) stray fields, i

235 A superconducting hard gap in hybrid superconductor-semiconductor devices has been found to b

236 nanowire junctions, as well as an epitaxial superconductor-semiconductor interface.

237 mental indications of Majorana zero modes in superconductor-semiconductor nanowires(3-8).

238 conductance) is demonstrated in these hybrid superconductor-semiconductor nanowires, highlighting the

239 t the paramagnetic end of this ferromagnetic superconductor series.

240 nsity of states (PDOS) of the weakly coupled superconductor Sn were analyzed and correlated with the

241 ors, have evaded discovery in bulk intrinsic superconductors so far.

242 igh-quality thin films of the unconventional superconductor Sr(2)RuO(4) grown on various substrates.

243 O(3) epitaxially deposited on a spin-triplet superconductor Sr(2)RuO(4), without any electronic spin-

244 For high-transition temperature cuprate superconductors, stripes are widely suspected to exist i

245 behaviour in three distinct classes of oxide superconductors: strontium titanate, strontium ruthenate

246 temperature in conventional two-dimensional superconductors such as NbSe(2).

247 onductors (FeSC), as in other unconventional superconductors such as the cuprates, neighbors a magnet

248 sting density waves, which we demonstrate on superconductors such as the dichalcogenides and [Formula

249 ests that UTe(2) is related to ferromagnetic superconductors such as UGe(2), URhGe, and UCoGe.

250 ld approach when applied to other correlated superconductors, such as copper oxides, has long inspire

251 In cuprate superconductors, superconductivity is accompanied by a p

252 Some layered superconductors support Josephson plasma waves (JPWs)2,3

253 or the pairing mechanism in high temperature superconductors, supported by the common appearance of a

254 ound states (MBSs) of electronic topological superconductor systems.

255 he fault-tolerance threshold(6) have been in superconductor systems.

256 Gi is significantly lower in most iron-based superconductors than in YBa 2Cu3O7-delta.

257 Sr2RuO4 is an unconventional superconductor that has attracted widespread study becau

258 of HgBa(2)CuO(4+delta), a highly anisotropic superconductor that is a model system for studying the e

259 iconductors with spin-valley coupling, Ising superconductors that can be tuned into a quantum metal,

260 most members of the cuprate high-temperature superconductors, the interplay between superconductivity

261 In the cuprate high-temperature superconductors, the metallic state above the highest tr

262 as found in multigap or in strongly-coupled superconductors, thus deviating from conventional Wertha

263 e demonstrate transitions from the candidate superconductor to Mott insulator and metallic phases.

264 Therefore, we show these superconductors to be example systems where electron-pho

265 n correlated materials, ranging from cuprate superconductors to bilayer graphene, and may arise from

266 The ability of type II superconductors to carry large amounts of current at hig

267 e expected to form a new type of topological superconductors to host Majorana zero modes under the pr

268 The superconductor-to-insulator transition (SIT) induced by

269 served at the Cu K-edge concomitant with the superconductor-to-insulator transition, evidencing modif

270 thin superconducting films - that experience superconductor-to-insulator transition.

271 uperconducting samples and static beyond the superconductor-to-metal transition.

272 extended to generate a distinct family of 2D superconductors, topological insulators, and excitonic s

273 light of De Gennes' analogy with the normal-superconductor transition of a metal, we identify the 1d

274 find evidence of this being due to insulator-superconductor transition.

275 A promising device is a superconductor-two quantum dots Cooper pair splitter.

276 Black phosphorus is also known to be a superconductor under high pressure exceeding 10 GPa.

277 ctivated vortex motion (creep) in iron-based superconductors unveiled fast rates (S) comparable to me

278 ctor can be driven into a chiral topological superconductor upon diluted doping of isolated magnetic

279 ies of the recently discovered heavy-fermion superconductor UTe(2), which has a superconducting trans

280 as the normal state of some high-temperature superconductors, violate this scenario, and the complete

281 he pseudogap in the cuprate high-temperature superconductors was discovered as a suppression of the K

282 topographic and electronic properties of the superconductor, we find that this inhomogeneity in the s

283 ic phases including Mott-like insulators and superconductors were recently discovered(5-8) by using e

284 e present a model appropriate for iron-based superconductors where the topological transition associa

285 onductors on equal footing with copper oxide superconductors, where a similar relation has been obser

286 enide high-transition-temperature (high-T c) superconductors, which have no hole Fermi pockets, but h

287 absence of clean-limit two-dimensional (2D) superconductors, which presents an impediment to the pur

288 wisted bilayer graphene and high-temperature superconductors, which spurred intensive research into t

289 eptibility in materials such as the Fe-based superconductors will be as effective in the case of [For

290 nreciprocity is a viable approach toward the superconductors with chiral or noncentrosymmetric struct

291 nt tuning parameter for the many families of superconductors with coexisting density waves, which we

292 Here we show that multiband superconductors with dominant spin singlet, intraband pa

293 In cuprate superconductors with high critical transition temperatur

294 in H(3)S, attention returned to conventional superconductors with properties that can be described by

295 ing a new route for realizing 2D topological superconductors with proximity effect.

296 Interfacing superconductors with strongly spin-polarized magnetic ma

297 years have seen the rise of atomically thin superconductors, with a caveat that superconductivity is

298 charge density wave in the high-temperature superconductor YBa(2)Cu(3)O(7-x) (YBCO) has two differen

299 emely thin superlattices composed of high Tc superconductor YBa2Cu3O7 (YBCO) and colossal magnetoresi

300 the doping mechanism of the high-temperature superconductor YBa2Cu3O7-X (YBCO) by simultaneous ionic