ライフサイエンスコーパス: cuprate

1 the antinodal Fermi surface of an overdoped cuprate.

2 ed insulating state in an archetypal undoped cuprate.

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

4 e constant reaching 70% of that of a typical cuprate.

5 ing analogies to CDW phases in various other cuprates.

6 between charge and spin correlations in the cuprates.

7 rong electron-phonon coupling is realized in cuprates.

8 s with strong magnetic fluctuations, such as cuprates.

9 and the pseudogap phenomena exhibited by the cuprates.

10 ng tunneling microscopy (STM) experiments on cuprates.

11 orbital symmetry recently reported in other cuprates.

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

13 and charge density wave phases of underdoped cuprates.

14 ctural order parameter in underdoped striped cuprates.

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

16 the similarly subtle charge DW state in the cuprates.

17 erature superconductor families, such as the cuprates.

18 doping and temperature parallels that in the cuprates.

19 copic methods revealing extended iodo Gilman cuprates.

20 perconductivity across different families of cuprates.

21 n the CuO(2) sheets of doped superconducting cuprates.

22 limiting factor in the superconductivity of cuprates.

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

24 a useful model system for comparison to the cuprates.

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

26 cturing costs limit the applicability of the cuprates.

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

28 the newly found Ni-based superconductors and cuprates.

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

30 ch are antiferromagnetic insulators like the cuprates.

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

32 iparticle recombination and gap formation in cuprates.

33 challenging for layered manganites than for cuprates.

34 e similar 3d(9) orbital electrons as that in cuprates.

35 attice degrees of freedom in superconducting cuprates.

36 spin chirality(7) in the pseudogap phase of cuprates.

37 is consistent with the phase diagram (PD) of cuprates.

38 he superconducting transition temperature in cuprates.

39 igma of the high-temperature superconducting cuprates.

40 netic coupling that matches or surpasses the cuprates.

41 ncreasing n(f), as it follows from the PD of cuprates.

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

43 s studies of the pseudogap in the underdoped cuprates.

44 entum structure and dispersion to hole-doped cuprates.

45 ) state predicted to exist in copper oxides (cuprates)(3,4).

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

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

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

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

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

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

52 mmercial [Formula: see text] is an excellent cuprate analog with remarkably similar electronic parame

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

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

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

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

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

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

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

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

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

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

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

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

65 This study of charge localization in cuprates and interfacial hybridization provides importan

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

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

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

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

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

71 Cuprates and other high-temperature superconductors cons

72 tal lattice for the electronic properties of cuprates and other high-temperature superconductors rema

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

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

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

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

77 ector offset recently observed in a La-based cuprate, and possible origins of this effect in La(2)NiO

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

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

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

81 urprising result suggests that the overdoped cuprates are strongly influenced by electron correlation

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

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

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

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

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

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

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

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

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

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

92 strong Delta(r) modulations in the canonical cuprate Bi(2)Sr(2)CaCu(2)O(8+delta) that have eight-unit

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

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

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

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

97 ance as a basis to understand electron-doped cuprates, cannot be explained under the traditional sche

98 ressure-induced electronic transition in the cuprate compounds due to a charge transfer between the C

99 optimally doped YBa(2)Cu(3)O(7) as archetype cuprate compounds.

100 The three central phenomena of cuprate (copper oxide) superconductors are linked by a c

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

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

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

104 may be regarded as the canonical underdoped cuprate, displaying marked pseudogap behaviour and an as

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

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

107 We conclude that the pseudogap phase of cuprates ends at a quantum critical point, the associate

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

109 Here we measure the specific heat C of the cuprates Eu-LSCO and Nd-LSCO at low temperature in magne

110 Superconductivity in the cuprates exhibits many unusual features.

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

112 ey property that distinguishes the different cuprate families.

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

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

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

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

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

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

119 -resolved electronic Raman scattering in the cuprate [Formula: see text], we report the observation o

120 oy pulsed magnetic-field measurements on the cuprate [Formula: see text]Cu[Formula: see text] to iden

121 ity-wave (CDW/SDW) orders in superconducting cuprates has altered our perspective on the nature of hi

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

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

124 la: see text], in comparison with most other cuprates, has a stable stoichiometry, is largely free of

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

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

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

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

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

130 The tetragonal cuprate HgBa(2)CuO(4+delta), with only one CuO(2) layer

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

132 ntium titanate, strontium ruthenate, and the cuprate high-T(c) materials.

133 Cuprate high-Tc superconductors exhibit enigmatic behavi

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

135 wisdom, the extraordinary properties of the cuprate high-temperature superconductors arise from dopi

136 an those previously reported for the layered cuprate high-temperature superconductors can be achieved

137 The cuprate high-temperature superconductors have been the f

138 Charge density waves (CDWs) in the cuprate high-temperature superconductors have evoked muc

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

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

141 In cuprate high-temperature superconductors, an antiferroma

142 -density waves (CDWs) in most members of the cuprate high-temperature superconductors, the interplay

143 In the cuprate high-temperature superconductors, the metallic s

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

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

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

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

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

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

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

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

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

153 -induced state in underdoped superconducting cuprates is a PDW, with approximately eight CuO(2) unit-

154 of high-[Formula: see text] superconducting cuprates is a unique Mott insulator consisting of layers

155 The pseudogap phenomenon in the cuprates is arguably the most mysterious puzzle in the f

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

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

158 ft X-ray scattering, we study the archetypal cuprate La(2-x)Sr(x)CuO(4) (LSCO) over a broad doping ra

159 a(xy)) in the normal state of four different cuprates-La(1.6-x)Nd(0.4)Sr(x)CuO(4), La(1.8-x)Eu(0.2)Sr

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

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

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

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

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

165 h has been the basis of much of the existing cuprate literature.

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

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

168 order have been discussed in iron-based and cuprate materials.

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

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

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

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

173 In electron-doped cuprate Nd(2-x) Ce (x) CuO(4) (NCCO), an unexpected FS r

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

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

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

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

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

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

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

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

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

183 Although the signature of a cuprate PDW has been detected in Cooper-pair tunnelling(

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

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

186 ns inconclusive and its broader relevance to cuprate physics is an open question.

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

188 Some experiments in cuprates point toward a CDW state competing with superco

189 rprisingly small Fermi surface in underdoped cuprates, possibly resulting from Fermi-surface reconstr

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

191 This cuprate 'pseudogap' manifests as a partial gap in the el

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

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

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

195 The pairing mechanism in cuprates remains as one of the most challenging issues i

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

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

198 f the pseudogap phase of the copper oxides ('cuprates') remains a puzzle.

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

200 unsaturated carbonyl compounds to form alpha-cuprated species has been extensively investigated, we r

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

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

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

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

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

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

207 High magnetic fields suppress cuprate superconductivity to reveal an unusual density w

208 The cuprate superconductor [Formula: see text], in compariso

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

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

211 -state thermopower (S) of the electron-doped cuprate superconductor La(2-x) Ce (x) CuO(4) (LCCO) from

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

213 hrough the cubic tunneling nonlinearity in a cuprate superconductor.

214 ular-resolved photoemission experiments on a cuprate superconductor.

215 infrared photoexcitation in high-temperature cuprate superconductor.

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

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

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

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

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

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

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

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

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

225 High-temperature cuprate superconductors display unexpected nanoscale inh

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

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

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 uitous in correlated materials, ranging from cuprate superconductors to bilayer graphene, and may ari

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

235 In cuprate superconductors with high critical transition te

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

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

238 In underdoped cuprate superconductors, a rich competition occurs betwe

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

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

241 In cuprate superconductors, it has been well established th

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 In cuprate superconductors, superconductivity is accompanie

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

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

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

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

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

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

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

255 yl, which has a close analogy with high T(c) cuprate superconductors.

256 an inherent characteristic of the enigmatic cuprate superconductors.

257 spin excitations are marginal to pairing in cuprate superconductors.

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

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

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

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

262 ased first-principles framework fails in the cuprate superconductors.

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

264 trilayer nickelate La4Ni3O10 compared to the cuprate superconductors.

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

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

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

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

269 In underdoped cuprates, the interplay of the pseudogap, superconductiv

270 In electron-doped cuprates, the low critical field (H(C2)) allows one to s

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 a ubiquitous feature of the superconducting cuprates, their disparate properties suggest a crucial r

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

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

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

279 sociated to a quantum critical point, in the cuprates they remain undetected until now.

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

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

289 on coupling in nickelates apart from that in cuprates where breathing phonons are not overdamped and

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

291 The highly overdoped cuprates-whose doping lies beyond the dome of supercondu

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

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

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

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

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

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

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

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

300 erest, due to its similarities to the parent cuprates, yet the intrinsic behaviour of Sr(2)IrO(4) upo