ライフサイエンスコーパス: superconductor

1 tum anomalous Hall insulator and topological superconductor).

2 (phonons in the case of conventional s-wave superconductors).

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

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

5 h strong spin-orbit interaction to an s-wave superconductor.

6 f high pressure makes MnP the first Mn-based superconductor.

7 (6)Li gas but never observed directly in any superconductor.

8 lous Hall insulator thin film coupled with a superconductor.

9 ristine interfaces between semiconductor and superconductor.

10 arded motion of magnetic vortices inside the superconductor.

11 he cubic tunneling nonlinearity in a cuprate superconductor.

12 olved photoemission experiments on a cuprate superconductor.

13 n the surface of a spin-orbit coupled s-wave superconductor.

14 Lu5Rh6Sn18 which is a strong coupling s-wave superconductor.

15 rise to Majorana physics without invoking a superconductor.

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

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

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

19 ization of the Kitaev model of a topological superconductor.

20 rbit coupling is brought into contact with a superconductor.

21 cal magnetic field or a critical current for superconductors.

22 and resistance-free electric current flow in superconductors.

23 of light reflected from the surface of some superconductors.

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

25 ilon near zero (ENZ) core-shell metamaterial superconductors.

26 ontext of high-temperature and heavy Fermion superconductors.

27 es in metals, and Yu-Shiba-Rusinov states in superconductors.

28 nd tested against the specific case of Nb3Sn superconductors.

29 stic depinning transition occurring in dirty superconductors.

30 them as promising candidates of topological superconductors.

31 o probe paramagnons in doped high-Tc cuprate superconductors.

32 ssure is a powerful tool to study iron-based superconductors.

33 the shuttled charge quantum between the two superconductors.

34 of two-dimensional Rashba spin-orbit coupled superconductors.

35 al issue in high transition-temperature (Tc) superconductors.

36 ic potential, such as Josephson junctions in superconductors.

37 towards eventual realization of topological superconductors.

38 s identical to that of the "1111" iron-based superconductors.

39 raise both Tc and Jc together in iron-based superconductors.

40 opper oxide, iron pnictide and heavy fermion superconductors.

41 explored as candidate systems of topological superconductors.

42 r substitution gives rise to a new family of superconductors.

43 he normal state properties of the iron-based superconductors.

44 w classes of potential very high-temperature superconductors.

45 ties compared to the core-shell metamaterial superconductors.

46 i2O4 in a manner similar to high-temperature superconductors.

47 fermions is a promising path to topological superconductors.

48 ication of bulk aluminium-based metamaterial superconductors.

49 ison with those fabricated from conventional superconductors.

50 e of the pseudogap state in high-temperature superconductors.

51 record value of 56 K for known bulk Fe-based superconductors.

52 Rh2Ga9, and Ir2Ga9 are all previously known superconductors.

53 for theoretical understanding of iron-based superconductors.

54 rmion superconductors, but not in iron-based superconductors.

55 of considerable Tc increase in other simple superconductors.

56 the vortex state of high-temperature cuprate superconductors.

57 e been shown to universally exist in cuprate superconductors.

58 c relaxation and electromagnetic response of superconductors.

59 (1/2) and the S = (1/2) state of the cuprate superconductors.

60 al properties from semiconductors, metals to superconductors.

61 ise to pseudogap states and high-temperature superconductors.

62 son junction arrays, and certain narrow band superconductors.

63 remain the focus in the research of cuprate superconductors.

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

65 nickelate La4Ni3O10 compared to the cuprate superconductors.

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

67 determine key electromagnetic properties of superconductors.

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

69 netic nano-devices based on high temperature superconductors.

70 on materials, including the high-temperature superconductors.

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

72 the parent state of cuprate high-temperature superconductors.

73 ent properties in magnetic fields over other superconductors.

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

75 and practical guidelines for discovering new superconductors.

76 e using a device comprised of a conventional superconductor, a ferromagnetic insulator, and semicondu

77 In the high-temperature (T(c)) cuprate superconductors, a growing body of evidence suggests tha

78 In underdoped cuprate superconductors, a rich competition occurs between super

79 ed experimentally, in cuprate and iron-based superconductors alike.

80 c modulus for ceramic and single crystalline superconductors alike.

81 In cuprate high-temperature superconductors, an antiferromagnetic Mott insulating st

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

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

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

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

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

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

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

89 cosmic microwave background polarization to superconductors and biological materials.

90 er is generic to the hole-doped copper oxide superconductors and competes with superconductivity.

91 the critical current density, Jc, of type II superconductors and its anisotropy with respect to magne

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

93 sm of a new class of plutonium-based high-Tc superconductors and predict the presence of a nodal s(+/

94 Finally, we apply this model to the Nb3Sn superconductors and propose approaches to control their

95 condensed matter systems such as topological superconductors and semimetals, in which they arise as l

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

97 ted electronic states of the high-Tc cuprate superconductors and the heavy-fermion intermetallics and

98 ial for understanding unconventional high-Tc superconductors and the non-Fermi liquid properties of h

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

100 logical superconductors, helical topological superconductors and Weyl semimetals.

101 oxide field-effect transistors, the cuprate superconductors, and conducting oxide interfaces (e.g.,

102 nature of the normal state of iron-pnictide superconductors, and the role played by correlations ari

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

104 ubic (BCC) Ta-Nb-Hf-Zr-Ti high-entropy alloy superconductor appears to display properties of both sim

105 nsity Jc determine the limits to large-scale superconductor applications.

106 We show that these superconductors are all strongly correlated, with an orb

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

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

109 Superconductors are excellent testbeds for studying vort

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

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

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

113 Yet, topological superconductors are rare to date.

114 Conventional superconductors are robust diamagnets that expel magneti

115 The properties of one-dimensional superconductors are strongly influenced by topological f

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

117 Our study unravels that CrH is a superconductor at atmospheric pressure with an estimated

118 uantum critical paradigm in that it is not a superconductor at temperature T >/= 10 millikelvin (mK).

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

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

121 nique to image vortices in the iron pnictide superconductor BaFe2(As0.7P0.3)2 with critical temperatu

122 of new energetic solids and high-temperature superconductors based on hydrogen-rich materials.

123 ial thin films are classified as dirty-limit superconductors because their mean-free paths, which are

124 n particular, we show that the heavy-fermion superconductor beta-YbAlB4 forms a possible phase with s

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

126 structed from single crystals of the high-Tc superconductor Bi2Sr2CaCu2O8+delta, we performed three p

127 ting microscope tip to the condensate of the superconductor Bi2Sr2CaCu2O8+x.

128 Recently, noncentrosymmetric superconductor BiPd has attracted considerable research

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

130 hts unique features of FeSe among iron-based superconductors, but bears some resemblance to that of h

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

132 tablished in copper-oxide, and heavy-fermion superconductors, but not in iron-based superconductors.

133 ic states such as topological insulators and superconductors, but the combination of strong spin-orbi

134 hout the underdoped high-temperature cuprate superconductors, but the underlying symmetry breaking an

135 have been suggested for the high-temperature superconductors, but their identification remains experi

136 ficantly to the zero resistance current in a superconductor by enhancing the probability that scatter

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

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

139 hich odd-frequency pairing in a Zeeman-split superconductor can be unambiguously detected via the app

140 rate that the resonance in the heavy fermion superconductor Ce1-xYbxCoIn5 with x=0, 0.05 and 0.3 has

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

142 in single crystals of Na2-deltaMo6Se6, a q1D superconductor comprising MoSe chains weakly coupled by

143 s in liquid crystals and Abrikosov phases in superconductors, contain arrays of topological defects i

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

145 that the pseudogap phase of the copper oxide superconductors contains such a 'pair density wave' stat

146 In most unconventional superconductors, Coulomb repulsion is minimized through

147 ty, consisting of the surface of an ordinary superconductor decorated with a two-dimensional lattice

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

149 ial route to a new class of high temperature superconductor due to the formal analogy between J eff =

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

151 e motivation of discovering high-temperature superconductors, evolutionary algorithm USPEX is employe

152 Iron selenide superconductors exhibit a number of unique characteristi

153 t compounds of the cuprate and iron-pnictide superconductors exhibit Neel and stripe magnetic order,

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

155 ile some candidate materials for bulk chiral superconductors exist, they are subject of an ongoing de

156 Fe-based superconductors (FBS) present a large variety of compoun

157 gap structure in iron-based high-temperature superconductors (Fe-HTSs) is non-universal.

158 spatial modulation of the magnetic field in superconductor/ferromagnet (S/F) hybrids.

159 It is now well established that at a superconductor/ferromagnet (S/F) interface an unconventi

160 It is found that superconductor FeS (tetragonal) partly transforms to a h

161 al characterizations of the newly discovered superconductor FeS.

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

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

164 Unlike other iron-based superconductors, FeSe exhibits nematic ordering without

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

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

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

168 t predicting the optimal defect landscape in superconductors for targeted applications by elucidating

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

170 le the normalized excess current through the superconductor-graphene interface decreases sharply.

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

172 tion of topological phases in insulators and superconductors has advanced the search for robust quant

173 rent absence of such nodes in the iron-based superconductors has led to a belief they form an s-wave

174 al state in the hole underdoped copper oxide superconductors has proven to be a source of mystery for

175 Iron-based superconductors have been found to exhibit an intimate i

176 density-wave (CDW) order in high-temperature superconductors have predicted a primarily d CDW orbital

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

178 Studies to date on ferromagnet/d-wave superconductor heterostructures focus mainly on the effe

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

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

181 Topological superconductors host new states of quantum matter which

182 Since the discovery of high-temperature superconductors (HTSs), most efforts of researchers have

183 discovery of the high-transition-temperature superconductors (HTSs), researchers have explored many m

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

185 superconductivity in some of the iron based superconductors in the vicinity of a Lifshitz point wher

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

187 In contrast to other unconventional superconductors, in the Fe-HTSs both d-wave and extended

188 2 is different from that of other iron-based superconductors, including Co-doped or P-doped BaFe2As2.

189 The physics of underdoped copper oxide superconductors, including the pseudogap, spin and charg

190 population in a Bi2Sr2CaCu2O8+delta cuprate superconductor induced by an ultrashort laser pulse.

191 conducting films in the critical vicinity of superconductor-insulator transition where a giant dielec

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

193 Nonlinear charge transport in superconductor-insulator-superconductor (SIS) Josephson

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

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

196 ature of the magnetism of a high-temperature superconductor is crucial for establishing its pairing m

197 the superconducting nature of a topological superconductor is found to be robust against Anderson di

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

199 Simultaneous increase of Tc and Jc in superconductors is desirable but very difficult to reali

200 tanding the normal state of high-temperature superconductors is now an essential step towards the des

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

202 A hallmark of the iron-based superconductors is the strong coupling between magnetic,

203 is a prototypical example of a heavy-fermion superconductor: it orders anti-ferromagnetically below 3

204 avevector QC = QP coexists with a d-symmetry superconductor; it is also predicted by several contempo

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

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

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

208 mmetry of CDW order in the canonical cuprate superconductors La1.875Ba0.125CuO4 (LBCO) and YBa2Cu3O6.

209 In the family of iron-based superconductors, LaFeAsO-type materials possess the simp

210 In stark contrast to usual superconductors, large non-linear diamagnetism by far ex

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

212 g for the first time in a noncentrosymmetric superconductor macroscopic characterization, atomic-scal

213 s with quenched disorder such as vortices in superconductors, magnetic domain walls, and charge densi

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

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

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

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

218 m of superconductivity in high-Tc iron-based superconductors more generally.

219 ities near the Fermi level in the iron-based superconductors must be explicitly accounted for in any

220 uctor, using epitaxial InAs-Al semiconductor-superconductor nanowires.

221 We study the two-dimensional topological superconductors of spinless fermions in a checkerboard-l

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

223 elopment of highly transparent semiconductor-superconductor ohmic contacts.

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

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

226 onal (2D) semiconductor heterostructure to a superconductor opens new research and technology opportu

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

228 the geometric boundaries in mesoscopic-size superconductors or by the spatial modulation of the magn

229 as LnPtBi compounds are non-centrosymmetric superconductors, our discovery further highlights them a

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

231 ects determine electromagnetic properties of superconductors, particularly their ability to carry non

232 urements in the hole underdoped copper oxide superconductors, point to a nodal electron pocket from c

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

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

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

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

237 Moreover, the newly discovered epsilon-NbN superconductor remains stable at pressures up to approxi

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

239 erconductors such as cuprates and iron-based superconductors remains an open question.

240 Its elusive nature in iron-based superconductors resulted in a controversy not only as re

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

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

243 als with different ordered phases, such as a superconductor (S) and a ferromagnet (F), is driving new

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

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

246 f the intrinsic thermal Hall conductivity on superconductor's temperature, magnetic field and the amp

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

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

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

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

251 , FeSe, the structurally simplest iron-based superconductor, shows nematic order (Ts=90 K), but not m

252 charge transport in superconductor-insulator-superconductor (SIS) Josephson junctions has a unique si

253 electro-thermal properties of semiconductor-superconductor (Sm-S) electronic cooler junctions by a n

254 gigapascals--the highest Tc reported for any superconductor so far.

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

256 orm a uniform vortex lattice in bulk type-II superconductors, strong confinement potential profoundly

257 r this explanation is still valid in high-Tc superconductors such as cuprates and iron-based supercon

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

259 K, great interest has been attracted in hard superconductors such as transition-metal nitrides and ca

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

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

262 The hard-gap semiconductor-superconductor system demonstrated here is amenable to t

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

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

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

266 In iron-based superconductors the interactions driving the nematic ord

267 s similar challenge in many Fe-based layered superconductors, the newly-discovered Ca10(Pt4As8)(Fe2As

268 In the family of the iron-based superconductors, the REFeAsO-type compounds (with RE bei

269 exciting opportunity to study 2D topological superconductors through the proximity effect.

270 measured by Jc, is the ability of defects in superconductors to pin the magnetic vortices, and that m

271 rements from five optimally doped iron-based superconductors to show that divergent nematic susceptib

272 xide films to study the magnetic-field tuned superconductor-to-insulator transition (H-SIT) in the T

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

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

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

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

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

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

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

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

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

282 The heavy fermion superconductor URu2Si2 has a "hidden order" (HO) phase b

283 quantum condensate of Cooper pairs forming a superconductor was originally conceived as being transla

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

285 the in-plane Cu spins in YBa2Cu3O7-x (YBCO) superconductor when it is grown on top of ferromagnetic

286 vely affected by vortex penetration into the superconductor when the peak magnetic field at the cavit

287 ever, in the pseudogap regime of the cuprate superconductors, where parts of the Fermi surface are de

288 ling of fluctuation Cooper pairs between two superconductors which grow even sharper and more pronoun

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

290 [Formula: see text]), an [Formula: see text] superconductor with a nontrivial topology is formed.

291 rs in the recently discovered sulfur hydride superconductor with a superconducting transition tempera

292 gically analogous to the 2D topological p+ip superconductor with chiral Majorana edge states and zero

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

294 In the quest for superconductors with higher transition temperatures (T(c

295 Normal superconductors with Rashba spin-orbit coupling have bee

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 iments on the recently discovered caged type superconductor Y5Rh6Sn18 ( TC= 3.0 K).

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