ライフサイエンスコーパス: cuprate

1 the antinodal Fermi surface of an overdoped cuprate.

2 of LiCu(n-Bu)(2) to generate the cyclopropyl cuprate.

3 ve coupling of lithium (n-Bu)(2-pyrrolidinyl)cuprate.

4 es, which is reminiscent of that observed in cuprates.

5 , and along the same direction, as in p-type cuprates.

6 the similarly subtle charge DW state in the cuprates.

7 erature superconductor families, such as the cuprates.

8 doping and temperature parallels that in the cuprates.

9 copic methods revealing extended iodo Gilman cuprates.

10 perconductivity across different families of cuprates.

11 limiting factor in the superconductivity of cuprates.

12 gle, charged-hole doped into two-dimensional cuprates.

13 a useful model system for comparison to the cuprates.

14 ve been observed up to optimal doping in the cuprates.

15 cturing costs limit the applicability of the cuprates.

16 s studies of the pseudogap in the underdoped cuprates.

17 -like scenario of the pseudogap phase of the cuprates.

18 ayers lie at the heart of the mystery of the cuprates.

19 ch are antiferromagnetic insulators like the cuprates.

20 would be needed for applications, as in the cuprates.

21 iparticle recombination and gap formation in cuprates.

22 challenging for layered manganites than for cuprates.

23 entum structure and dispersion to hole-doped cuprates.

24 asted with the Mott-Hubbard insulator in the cuprates.

25 hat suppress superconductivity in underdoped cuprates.

26 are responsible for superconductivity in the cuprates.

27 oked for explaining the superconductivity in cuprates.

28 and the underlying antiferromagnetism of the cuprates.

29 doping increased, in both single and bilayer cuprates.

30 tanding the high-temperature-superconducting cuprates.

31 ns for other incommensurate phenomena in the cuprates.

32 example, in tuning superconductivity in the cuprates.

33 ing analogies to CDW phases in various other cuprates.

34 between charge and spin correlations in the cuprates.

35 rong electron-phonon coupling is realized in cuprates.

36 s with strong magnetic fluctuations, such as cuprates.

37 and the pseudogap phenomena exhibited by the cuprates.

38 ng tunneling microscopy (STM) experiments on cuprates.

39 orbital symmetry recently reported in other cuprates.

40 ut bears some resemblance to that of high-Tc cuprates.

41 and charge density wave phases of underdoped cuprates.

42 ctural order parameter in underdoped striped cuprates.

43 selective 1,4-addition of alpha-alkoxy vinyl cuprates 68 to steroid 17(20)-en-16-one 12E to introduce

44 In hole-doped (p-type) cuprates, a charge ordering (CO) instability competes wi

45 theoretical principles predict that, in the cuprates, a localized spin modulation of wavelength lamb

46 ping parameters, it is possible to drive the cuprates across a transition between Mott and Slater phy

47 of 3-methyl-3-buten-1-ol (5), a Z-selective cuprate addition of alkyl groups to an alpha,beta-alkyny

48 on alkynone 14 and a Feringa-Minnaard methyl cuprate addition on enoate 21.

49 symmetric alkynylation and a stereoselective cuprate addition to an alkynoate have been developed for

50 Cuprate addition to commercially available 1,4-dibromo-2

51 E-triene unit through a chelation-controlled cuprate addition with installation of the C11 stereochem

52 Tandem cuprate addition-Dieckmann condensation is featured in t

53 Removing electrons from the CuO2 plane of cuprates alters the electronic correlations sufficiently

54 Sr3Ir2O7 realizes a weak Mott state with no cuprate analogue by using ultrafast time-resolved optica

55 p, a diastereoselective addition of an ethyl cuprate and an unusual strategy to install two additiona

56 nd differences between BaTi(2)Sb(2)O and the cuprate and iron pnictide superconductors are discussed.

57 ga(-1+/-0.2) in the ground states of several cuprate and iron-based materials which undergo electroni

58 which have been observed experimentally, in cuprate and iron-based superconductors alike.

59 ese materials being intermediate between the cuprate and iron-pnictide high-temperature superconducti

60 The parent compounds of the cuprate and iron-pnictide superconductors exhibit Neel a

61 picture of the interfacial carrier doping in cuprate and manganite atomic layers, leading to the tran

62 to understand the buried interfaces between cuprate and manganite layers.

63 d strict lowest upper bounds for T(c) in the cuprate and pnictide families.

64 romagnet, in sharp contrast to the high-T(C) cuprates and a previous report in the literature.

65 mergence of high-Tc superconductivity in the cuprates and colossal magnetoresistance in the manganite

66 ly underdoped samples, its behavior in other cuprates and different doping regions is still unclear.

67 period as those found in Y-based or La-based cuprates and displays the analogous competition with sup

68 cenario being widely postulated in high T(c) cuprates and invoked to explain non-Fermi liquid transpo

69 ill valid in high-Tc superconductors such as cuprates and iron-based superconductors remains an open

70 ectronic symmetry breaking in the underdoped cuprates and its disappearance with increased hole densi

71 tous in correlated solids such as pnictides, cuprates and manganites.

72 ese materials share many properties with the cuprates and offer the hope of finally unveiling the sec

73 Cuprates and other high-temperature superconductors cons

74 This includes the cuprates and other transition metal oxide perovskites, w

75 ing the complex electronic properties of the cuprates and places strong constraints on theoretical mo

76 de-Ferrel-Larkin-Ovchinnikov (FFLO) state in cuprates and studying the competing quantum orders in hi

77 heir structural similarity to the 3d9 Cu(II) cuprates and the covalence associated with this unusual

78 Like the high-T(c) cuprates and the iron pnictides, the superconductivity i

79 uctural equivalence of iodo and cyano Gilman cuprates and their subsequential intermediates.

80 h are observed at lower temperatures in some cuprates, and find that the upper limit of the energy re

81 n several condensed matter systems including cuprate- and iron arsenic-based high-temperature superco

82 nducting transition temperatures for certain cuprates are found in samples that display simultaneous

83 ts in the pseudogap regime of the hole-doped cuprates are readily interpreted in light of these resul

84 The high-temperature superconducting oxides (cuprates) are the most studied class of superconductors,

85 High-temperature superconductivity in cuprates arises from an electronic state that remains po

86 physics similar to high T C superconducting cuprates as they have similar crystal structures and the

87 elations, finding strong resemblances to the cuprates as well as a few key differences.

88 ds light on the nature of charge ordering in cuprates as well as a reported long-range proximity effe

89 Such a hybrid state is most likely found in cuprates as well while our results point to the importan

90 rch for broken symmetry electronic states in cuprates, as well as in other materials.

91 del for the metallic state of the hole-doped cuprates at low hole density, p.

92 est values ever reported from any lengths of cuprate-based HTS wire or conductor.

93 d to the underdoped regime of the hole-doped cuprates because of its proximity to a complex Mott insu

94 Sandwiching a non-superconducting cuprate between two manganese oxide layers, we find a no

95 nteraction in the unoccupied spectrum of the cuprate Bi2Sr2CaCu2O8+x characterized by an excited popu

96 In cuprate bilayers, the critical temperature (Tc) can be s

97 isite broken-symmetry phase in the high-T(c) cuprates, but the impact of such a phase on the ground-s

98 ction of hole concentration in bismuth-based cuprates by measuring the voltage induced by vortex flow

99 her avenue for the study and manipulation of cuprates, bypassing the complexities inherent to convent

100 dentical phenomena in two lightly hole-doped cuprates: Ca(1.88)Na(0.12)CuO(2)Cl2 and Bi2Sr2Dy(0.2)Ca(

101 to create one quaternary stereocenter and a cuprate conjugate addition for the establishment of the

102 t, cuprate reagent, transferable ligand, and cuprate counterion (e.g., Li(+) vs MgX(+)).

103 alpha-(N-Carbamoylalkyl)cuprates couple with enol triflates derived from carbocy

104 f spin-polarized electrons from manganite to cuprate differently.

105 Although all superconducting cuprates display charge-ordering tendencies, their low-t

106 alkyl copper in iodo but not in cyano Gilman cuprates during the reaction.

107 llic behaviour and superconductivity in many cuprates, electron doping alone is insufficient in mater

108 elate physics, with the differences from the cuprate electronic structure potentially shedding light

109 electivities appear to be more a function of cuprate-electrophile reactivities than of the reaction t

110 ism by which d wave superconductivity in the cuprates emerges and is optimized by doping the Mott ins

111 ctive oxidative biaryl coupling and a double cuprate epoxide opening, allowing the selective synthese

112 Superconductivity in the cuprates exhibits many unusual features.

113 ht on the origin of superconductivity in the cuprates.Exploration of the electronic structure of nick

114 ey property that distinguishes the different cuprate families.

115 angle-resolved photoemission data for every cuprate family precludes an agreement as to its structur

116 erence pattern within a single bismuth-based cuprate family, we observed a Fermi surface reconstructi

117 e in the unconventional superconductivity of cuprates, Fe-based and heavy-fermion systems, yet even f

118 ium iridate (Sr2IrO4), in which the distinct cuprate fermiology is largely reproduced.

119 This connects Fe pnictides to cuprates, for which, in spite of fundamental electronic

120 An amido cuprate formed from CuCN and LDA allows a general deconj

121 vation of quantum oscillations in underdoped cuprates has generated intense debate about the nature o

122 ucture of the normal state of the underdoped cuprates has thus far remained mysterious, with neither

123 Although high-temperature superconductor cuprates have been discovered for more than 25 years, su

124 scattering (RIXS) experiments in hole-doped cuprates have purported to measure high-energy collectiv

125 h temperature (high-Tc) superconductors like cuprates have superior critical current properties in ma

126 uctors, without most of the drawbacks of the cuprates, have a superior high-field performance over lo

127 Later, a variety of systems, such as cuprates, heavy fermions, and Fe pnictides, showed super

128 ion measurements on the structurally simpler cuprate HgBa2CuO4+delta (Hg1201), which features one CuO

129 e randomness of dopant atom distributions in cuprate high-critical temperature superconductors has lo

130 Cuprate high-Tc superconductors exhibit enigmatic behavi

131 The properties of cuprate high-temperature superconductors are largely sha

132 observables across the phase diagram of the cuprate high-temperature superconductors has remained a

133 The cuprate high-temperature superconductors have been the f

134 The nature of the pseudogap phase of cuprate high-temperature superconductors is a major unso

135 The pseudogap in the cuprate high-temperature superconductors was discovered

136 In cuprate high-temperature superconductors, an antiferroma

137 erstanding of complex materials, such as the cuprate high-temperature superconductors.

138 bit coupled analogues of the parent state of cuprate high-temperature superconductors.

139 oduct yields are higher with the alkyl(cyano)cuprates [i.e., RCu(CN)Li, 56-93%] than with the dialkyl

140 pi, pi) are analogous to those of hole-doped cuprates in several aspects, thus implying that such spi

141 ion, as well as many other properties of the cuprates in the vicinity of the instability toward "stri

142 nderstand the origin of the pseudogap in the cuprates, in terms of bosonic entropy.

143 es the Fermi surface of optimally hole-doped cuprates, including its [Formula: see text] orbital char

144 a cuprate metal (La(1.65)Sr(0.45)CuO4) and a cuprate insulator (La2CuO4) in which each layer is just

145 High-T(c) cuprates, iron pnictides, organic BEDT and TMTSF, alkali

146 onance in the spin susceptibility across the cuprates, iron-based superconductors and many heavy ferm

147 ts suggest that the superfluid in underdoped cuprates is a condensate of coherently-mixed particle-pa

148 standing the role of competing states in the cuprates is essential for developing a theory for high-t

149 that the k-space topology transformation in cuprates is linked intimately with the disappearance of

150 A key unresolved issue in cuprates is the relationship between superconductivity a

151 correlations in the canonical stripe-ordered cuprate La1.875Ba0.125CuO4 across its ordering transitio

152 However, in contrast to cuprates, La4Ni3O10 has no pseudogap in the [Formula: se

153 ercalating molecule electron transfer on the cuprate layer may be important, quite apart from this sp

154 The question of how thin cuprate layers can be while still retaining high-tempera

155 The pseudogap in underdoped cuprates leads to significant changes in the electronic

156 In pursuit of creating cuprate-like electronic and orbital structures, artifici

157 from Co to Ir, the charge transfers from the cuprate-like Zhang-Rice state on Cu to the t(2g) orbital

158 confirms that this effect is general to all cuprate/manganite heterostructures and the presence of d

159 antum critical scaling in the electron-doped cuprate material La(2-x)Ce(x)CuO(4) with a line of quant

160 it was found that a large family of ceramic cuprate materials exhibited superconductivity at tempera

161 the dc (omega = 0) resistivity of different cuprate materials.

162 nickelates with similar crystal structure to cuprates may shed a light on the origin of high T c supe

163 ization substrate 11 was treated with Gilman cuprate Me(2)CuLi to afford anthracene 12.

164 of the current mechanistic understanding of cuprate-mediated allylic substitution reactions.

165 lar beam epitaxy to synthesize bilayers of a cuprate metal (La(1.65)Sr(0.45)CuO4) and a cuprate insul

166 he presence of charge ordering in the n-type cuprate Nd(2-x)Ce(x)CuO4 near optimal doping.

167 r unconventional superconductors such as the cuprates, neighbors a magnetically ordered one in the ph

168 However, unlike the bilayer cuprates, no electronic instabilities have been reported

169 on the intertwined orders emerging from the cuprates' normal state.

170 hat the near-nodal excitations of underdoped cuprates obey Fermi liquid behavior.

171 Lanthanide cuprates of formula Ln(2)CuO(4) exist in two principal f

172 rface via quantum oscillations in hole-doped cuprates opened a path towards identifying broken symmet

173 eoselectively, by 1,6-addition of a tertiary cuprate or a tertiary carbon radical to beta-vinylbuteno

174 Tellurium-derived cuprate organometallics offered an efficient and highly

175 EDL) gating experiments with superconducting cuprates, our work shows that interfacing correlated oxi

176 operties in two isostructural A-site ordered cuprate perovskites, CaCu(3)Co(4)O(12) and CaCu(3)Cr(4)O

177 In the layered cuprate perovskites, the occurrence of high-temperature

178 e in shaping the anomalous properties of the cuprate phase diagram.

179 g order as the root of the complexity of the cuprate phase diagram.

180 Optimally doped ceramic superconductors (cuprates, pnictides, etc.) exhibit transition temperatur

181 Ceramic superconductors (cuprates, pnictides, etc.) exhibit universal features in

182 he origin of the weak ferromagnetism of bulk cuprates, propagates the magnetisation from the interfac

183 ossible explanation for the existence of the cuprate "pseudogap" state is that it is a d-wave superco

184 energy features previously observed in doped cuprates-pseudogaps, Fermi arcs and marginal-Fermi-liqui

185 n situ generated enantioenriched stereogenic cuprate reagent with (E)-4-bromo-1-iodo-1-trimethylsilyl

186 of Cu(I) salt (i.e., CuCN, CuCN.2LiCl, CuI), cuprate reagent, sec-butyllithium quality, solvent, and

187 E-isomer 17 varied as a function of solvent, cuprate reagent, transferable ligand, and cuprate counte

188 C4 upon treatment with a higher order cyano cuprate reagent.

189 Mixed lithium dialkyl- or alkyl(aryl)cuprate reagents containing one alpha-(heteroatom)alkyl

190 itued piperidinones stereoselectively, while cuprate reagents give either the trans or cis diastereom

191 ith various nucleophiles, i.e., Grignard and cuprate reagents, azide ion, and amines.

192 ive importance of quantum criticality in the cuprates remains uncertain.

193 ve spin excitations of doped superconducting cuprates remains under debate.

194 In low dimensional cuprates several interesting phenomena, including high T

195 x), with x=0-0.30 that shows that, as in the cuprates, static magnetism persists well into the superc

196 oncentrated on the existence of higher-order cuprate structures.

197 In bulk cuprates such as La(2)CuO(4), the presence of a weak cou

198 discovery of high T(c) superconductivity in cuprates suggests that the highest T(c)s occur when pres

199 rthorhombic structural distortion across the cuprate superconducting Bi(2)Sr(2)Ca(n-1)Cu(n)O(2n+4+x)

200 The unclear relationship between cuprate superconductivity and the pseudogap state remain

201 l a strong, nonrandom out-of-plane effect on cuprate superconductivity at atomic scale.

202 dged that electron-phonon interactions cause cuprate superconductivity with T(c) values approximately

203 ng tunneling microscopy in the lightly doped cuprate superconductor Ca2-xNaxCuO2Cl2.

204 harge-density-wave correlations in the model cuprate superconductor HgBa2CuO(4+delta) (T(c)=72 K) via

205 particle population in a Bi2Sr2CaCu2O8+delta cuprate superconductor induced by an ultrashort laser pu

206 i-particles in a high-transition-temperature cuprate superconductor using the transient grating techn

207 e-amplitude apical oxygen distortions in the cuprate superconductor YBa2Cu3O6.5 promotes highly uncon

208 infrared photoexcitation in high-temperature cuprate superconductor.

209 such a nonequilibrium phase transition in a cuprate superconductor.

210 hrough the cubic tunneling nonlinearity in a cuprate superconductor.

211 ular-resolved photoemission experiments on a cuprate superconductor.

212 ctive conductors out of the high-temperature cuprate superconductors (HTSs) has proved difficult beca

213 nic superconductors and underdoped high-T(c) cuprate superconductors a fluctuating superconducting st

214 c systems such as the strange metal phase of cuprate superconductors and heavy fermion materials near

215 Many exotic compounds, such as cuprate superconductors and heavy fermion materials, exh

216 resolving similarly longstanding debates in cuprate superconductors and other strongly correlated ma

217 es are the high critical temperatures of the cuprate superconductors and the colossal magnetoresistan

218 correlated electronic states of the high-Tc cuprate superconductors and the heavy-fermion intermetal

219 transition temperatures of the highest T(c) cuprate superconductors are facilitated by enhanced CuO(

220 The nature of the pseudogap regime of cuprate superconductors at low hole density remains unre

221 fied picture of the oxygen isotope effect in cuprate superconductors based on a phonon-mediated d-wav

222 on spectroscopy applied to deeply underdoped cuprate superconductors Bi2Sr2Ca(1-x)YxCu2O8 (Bi2212) to

223 ments of quasi-particle dynamics not only in cuprate superconductors but in other electronic systems

224 High-temperature cuprate superconductors display unexpected nanoscale inh

225 This result poses a new challenge to theory--cuprate superconductors have not run out of surprises.

226 of the bulk value of the pairing strength in cuprate superconductors in magnetic field.

227 of superconductivity in the high-temperature cuprate superconductors is one of the major outstanding

228 ase which opens in the under-doped regime of cuprate superconductors is one of the most enduring chal

229 A major challenge in understanding the cuprate superconductors is to clarify the nature of the

230 bital symmetry of CDW order in the canonical cuprate superconductors La1.875Ba0.125CuO4 (LBCO) and YB

231 s observation in the iron-pnictide and doped cuprate superconductors places it at the forefront of cu

232 High-critical temperature cuprate superconductors set the present record of ~100 K

233 om scanning tunnelling microscopy studies of cuprate superconductors to identify the fundamental phys

234 Ca(x)CuO2 (the parent phase of the high-T(c) cuprate superconductors), but with a d(2) electron count

235 his restricts choice to two high-temperature cuprate superconductors, (Bi,Pb)2Sr2Ca2Cu3Ox and YBa2Cu3

236 In the high-temperature (T(c)) cuprate superconductors, a growing body of evidence sugg

237 In underdoped cuprate superconductors, a rich competition occurs betwe

238 candidate for electronic phase separation in cuprate superconductors, and a key to understanding seem

239 ty metal oxide field-effect transistors, the cuprate superconductors, and conducting oxide interfaces

240 als share a similar pairing mechanism to the cuprate superconductors, as both families exhibit superc

241 s throughout the underdoped high-temperature cuprate superconductors, but the underlying symmetry bre

242 t to increase the critical temperature Tc of cuprate superconductors, it is essential to identify the

243 For high-transition temperature cuprate superconductors, stripes are widely suspected to

244 tic modes that propagate along the planes of cuprate superconductors, sustained by interlayer tunnell

245 In underdoped cuprate superconductors, the Fermi surface undergoes a r

246 ts show that as for many other properties of cuprate superconductors, the important underlying micros

247 In the high-temperature cuprate superconductors, the pervasiveness of anomalous

248 In many cases, such as in d-wave cuprate superconductors, the position and topology of no

249 However, in the pseudogap regime of the cuprate superconductors, where parts of the Fermi surfac

250 fullerides but reminiscent of the atom-based cuprate superconductors--to the role of strong electroni

251 in many charge-ordered materials, including cuprate superconductors.

252 an inherent characteristic of the enigmatic cuprate superconductors.

253 spin excitations are marginal to pairing in cuprate superconductors.

254 breaking remain the focus in the research of cuprate superconductors.

255 trilayer nickelate La4Ni3O10 compared to the cuprate superconductors.

256 nt on its magnitude and doping dependence in cuprate superconductors.

257 nd may shed important light on the high-T(c) cuprate superconductors.

258 g besides Kondo-lattice metals, Fe-based and cuprate superconductors.

259 structure that is reminiscent of the high-Tc cuprate superconductors.

260 l as well as the variation between different cuprate superconductors.

261 rial chemistry to generate a library of e.g. cuprate superconductors.

262 rmi liquid, the normal metallic state of the cuprate superconductors.

263 e used to probe paramagnons in doped high-Tc cuprate superconductors.

264 ield in the vortex state of high-temperature cuprate superconductors.

265 ions have been shown to universally exist in cuprate superconductors.

266 J eff = (1/2) and the S = (1/2) state of the cuprate superconductors.

267 he application of magnetic fields to layered cuprates suppresses their high-temperature superconducti

268 symmetry between the electron and hole-doped cuprates than previously thought.

269 conducting critical temperature, T(c), among cuprates that have identical hole density but are crysta

270 pper-oxygen sheets of the enigmatic lamellar cuprates, the ground state evolves from an insulator to

271 In cuprates, the pattern formation is associated with the p

272 very of high-Tc superconductivity in layered cuprates, the roles that individual layers play have bee

273 like regime that is ubiquitous in underdoped cuprates, the spectrum consists of holes on the Fermi ar

274 s of the magnetic excitation spectrum of the cuprates: the X-shaped 'hourglass' response and the reso

275 iferromagnetic (AFM) ground state to that of cuprates, therefore, it receives much more attention on

276 Trailing behind the cuprates, these iron-based compounds are the second-high

277 f the charge order by doping, analogously to cuprates, these results provide a new electronic paradig

278 In cuprates, this technique has been used to remove charge

279 an enantioselective addition of isopropenyl cuprate to 2-methylcyclopentenone (see compound 99).

280 stereoselective conjugate addition of vinyl cuprate to enone.

281 xysuccinimide via an unusual syn-addition of cuprate to the alpha,beta-unsaturated lactam.

282 t extends the similarity between Sr2IrO4 and cuprates to a new dimension of electron-phonon coupling

283 many electronic properties of the underdoped cuprates to be understood.

284 uctivity highlight a generic tendency of the cuprates to develop competing electronic (charge) superm

285 posed in some of these superconductors, from cuprates to iron-based compounds.

286 erconductors - ranging from high-temperature cuprates to ultrathin superconducting films - that exper

287 Field-effect experiments on cuprates using ionic liquids have enabled the exploratio

288 The lithium-copper transmetalation and cuprate vinylation reactions proceed with retention of c

289 High-temperature superconductivity in cuprates was discovered almost exactly 20 years ago, but

290 Superconductivity appears in the cuprates when a spin order is destroyed, while the role

291 RPES) is ideally suited for this task in the cuprates, where emergent phases, particularly supercondu

292 t test for various ordering scenarios in the cuprates, which have been central in the debate on the n

293 disorder in HgBa2CuO4 + y, the single-layer cuprate with the highest Tc, 95 kelvin.

294 tafluoroethane, C2F5H (HFC-125), is smoothly cuprated with preisolated or in situ-generated [K(DMF)][

295 In the example of cuprates with a highly soluble substituent (R = Me3SiCH2

296 static vs. electrochemical, of the doping of cuprates with ionic liquids.

297 access the underlying metallic state of the cuprate YBa2Cu3O(6+delta) over a wide range of doping, a

298 pic structure of the CDWs in an archetypical cuprate YBa2Cu3O6.54 at its superconducting transition t

299 y correlation in the underdoped phase of the cuprate YBa2Cu3Oy was obtained by NMR and resonant X-ray

300 ty can be used to directly detect Hc2 in the cuprates YBa2Cu3Oy, YBa2Cu4O8 and Tl2Ba2CuO6+delta, allo