ライフサイエンスコーパス: copper oxide

1 exchange reaction between sputtered tin and copper oxide.

2 through the use of sintering agents such as copper oxide.

3 am remarkably similar to that of the high-Tc copper oxides.

4 T magnetic field benchmark of the high-T(c) copper oxides.

5 like, originally designed for the high-T(c) copper oxides.

6 ity is the same for electron- and hole-doped copper oxides.

7 or high temperature superconductivity in the copper oxides.

8 s a general property of superconductivity in copper oxides.

9 cal doping that is observed in the high-T(c) copper oxides.

10 vy-fermion superconductors and the high-T(c) copper oxides.

11 tovoltaic hybrid iodides and superconducting copper oxides.

12 such as the waterfall dispersion observed in copper oxides.

13 een subject to strong controversy in high-Tc copper oxides.

14 is needed to elucidate the phase diagram of copper oxides.

15 t from outside the family of superconducting copper oxides.

16 8), in stark contrast to strongly correlated copper oxides(1,2) and nickelates(29-31), in which the C

17 ilt magnesium diboride and Rare-Earth-Barium-Copper-Oxide 100 kA class superconducting system.

18 late that is isostructural to infinite-layer copper oxides(11-13).

19 er than the charge-transfer insulator of the copper oxides(15,16).

20 This is phenomenologically similar to the copper oxides(2,12) despite key distinctions-namely, the

21 ly of nickelate superconductors analogous to copper oxides(24) and pnictides(25).

22 Here we used isotopically modified copper oxide ((65)CuO) NPs to characterize the processes

23 In underdoped high-T(c) superconducting copper oxides, a pseudogap (whose relation to the superc

24 the high-transition-temperature (high-T(c)) copper oxides-a set of anomalous physical properties bel

25 port zeolite-based copper catalysts in which copper oxide agglomerates formed after reaction can be r

26 gh electrochemical performance of nickel and copper oxide and hydroxide on a conductive template lead

27 old, both citrate stabilized), metal oxides (copper oxide and titanium dioxide), and CdSe/ZnS core/sh

28 for two disparate classes of materials--the copper oxides and a set of Ce- and U-based compounds.

29 xide structures, such as the superconducting copper oxides and ferroelectric titanates, as well as in

30 lity and unconventional superconductivity in copper oxides and heavy-electron systems such as CeRhIn5

31 of both the high transition-temperature (Tc) copper oxides and low-Tc material Sr2RuO4, where they ap

32 ental of those characteristics, for both the copper oxides and other superconductors, is the dependen

33 ilar to those of high-transition-temperature copper oxides and other unconventional superconductors(1

34 gin of high-temperature superconductivity in copper oxides and the nature of the 'normal' state above

35 e assumption that the pseudogap state in the copper oxides and the nodal-antinodal dichotomy are hall

36 fundamental property of the superconducting copper oxides and therefore must be essential in the mec

37 tivity can exist in an isolated monolayer of copper oxide, and if so, whether the two-dimensional sup

38 ests that they are a general property of the copper oxides, and a candidate for mediating the electro

39 es are high-temperature superconductivity in copper oxides, and colossal magnetoresistance in mangane

40 ion phenomena found extensively in low-doped copper oxides, and show that Cooper pair formation is co

41 quasiparticle states are well established in copper-oxide, and heavy-fermion superconductors, but not

42 The overdoped copper oxides are perceived as simpler, with strongly co

43 g transmission electron microscopy show that copper oxides are surprisingly resistant to reduction an

44 Transition metal catalysts, such as copper oxide, are more attractive alternatives to noble

45 High-temperature superconductivity in copper oxides arises when a parent insulator compound is

46 Our results establish monolayer copper oxides as a platform for studying high-temperatur

47 g macroporous frameworks of silver, gold and copper oxide, as well as composites of silver/copper oxi

48 ducting indium-gallium-zinc oxide (IGZO) and copper oxide, as well as conducting indium-tin oxide and

49 rsus wavevector) of electronic states in the copper oxides at binding energies of 50-80 meV, raising

50 magnetic field are found in these ruthenium copper oxides at low temperatures through coupling betwe

51 n the families of low- and high-temperature (copper oxide based) superconductors.

52 or understanding the electronic structure of copper-oxide based high-temperature superconductors.

53 the common features and differences with the copper-oxide based superconductors.

54 higher critical temperatures are offered by copper oxide-based superconductors.

55 e out-of-equilibrium electronic structure of copper-oxide-based high-temperature superconductors by i

56 Copper-oxide-based high-temperature superconductors have

57 nthanide, marks the first discovery of a non-copper-oxide-based layered high-Tc superconductor.

58 f new classes of materials, with the layered copper oxides being a particularly impressive example.

59 port a photoemission study of the underdoped copper oxide Bi(2)Sr(2)CaCu(2)O(8+delta) that shows the

60 ghest known transition temperature for a non-copper-oxide bulk material.

61 ain field-induced magnetism in the high-T(c) copper oxides, but in which a clear delineation of quant

62 nsity for a water-based nanofluid containing copper oxide, calcium carbonate, and silicon dioxide in

63 Cable-like copper oxide/carbon-nitride core-shell nanostructures ac

64 ibromide (BTMA-Br3) followed by mixed copper-copper oxide-catalyzed amination of 4-bromophthalazin-1(

65 Copper oxide clusters synthesized via atomic layer depos

66 t a ternary mixed oxide catalyst composed of copper oxide, cobalt oxide, and ceria (dubbed CCC) that

67 the high-transition-temperature (high-T(c)) copper oxides competes with other possible ground states

68 Superconductivity in layered copper oxide compounds emerges when charge carriers are

69 a(2)Ca(4)Cu(5)O(10)(F,O)(2), which has inner copper oxide (CuO(2)) planes with extremely low disorder

70 agation rates for Al combined with nanoscale copper oxide (CuO) are in quantitative agreement with th

71 Here we report that copper oxide (CuO) can efficiently activate PDS under mi

72 Under copper oxide (CuO) nanoparticle exposure, polyploids exp

73 xposure to a potential nanoscale fertilizer: copper oxide (CuO) nanoparticles.

74 ed the aquatic toxicological implications of copper oxide (CuO) nanospheres relative to CuO nanorods

75 ochemically coated with zinc oxide (ZnO) and copper oxide (CuO) NPs.

76 ric acid biosensor has been realized using a copper oxide (CuO) thin film matrix grown onto platinum

77 aluminum layered hydroxides (Cu-Al LDHs) and copper oxide (CuO) were utilized as catalysts for hetero

78 nsity-wave (PDW) state predicted to exist in copper oxides (cuprates)(3,4).

79 The nature of the pseudogap phase of the copper oxides ('cuprates') remains a puzzle.

80 rstand high-temperature superconductivity in copper oxides, debate has been focused on the pseudogap-

81 In copper oxides, doping also gives rise to the pseudogap s

82 Copper-oxide electrocatalysts have been demonstrated to

83 Sputtering of nickel on the copper-oxide electrode nucleated an unexpected surface m

84 S) to study the dynamic restructuring of the copper (oxide) electrode surface and the adsorption of r

85 terplay between the dynamic restructuring of copper oxide electrodes and their activity and selectivi

86 Although the copper oxides exhibit very high transition temperatures,

87 When electrodepositing a copper oxide film on an achiral gold surface in the pres

88 Copper oxide films hold substantial promise as anti-stic

89 occurrence of electrons and holes in n-type copper oxides has been achieved by chemical doping, pres

90 to other correlated superconductors, such as copper oxides, has long inspired the study of the highly

91 onductivity, the high-transition-temperature copper oxides have an additional 'pseudogap'.

92 surements of spin fluctuations in hole-doped copper oxides have revealed an unusual 'hour-glass' feat

93 uch competition has been found in multilayer copper oxide high-temperature superconductors (HTSCs) th

94 Although the crystal structures of the copper oxide high-temperature superconductors are comple

95 Although copper oxide high-temperature superconductors constitute

96 A characteristic feature of the copper oxide high-temperature superconductors is the dic

97 Although crystals of the copper oxide high-transition-temperature (high-Tc) super

98 The parent compounds of the copper oxide high-transition-temperature (high-Tc) super

99 A remarkable mystery of the copper oxide high-transition-temperature (T(c)) supercon

100 In the copper-oxide high-temperature superconductors (HTSCs), a

101 Besides superconductivity, copper-oxide high-temperature superconductors are suscep

102 as been the main challenge in the physics of copper-oxide high-temperature superconductors.

103 In the underdoped copper-oxides, high-temperature superconductivity conden

104 nalyzed for NPs of silver (Ag), copper (Cu), copper oxide/hydroxide (CuO, Cu(OH)(2)), zinc oxide (ZnO

105 It was found that the formation of monophase copper oxide II only occurred when copper acetate was us

106 of high-temperature superconductivity in the copper oxides in 1986 triggered a huge amount of innovat

107 A well-known example is the copper oxides, in which a charge density wave (CDW) is o

108 describes many of the features shared by the copper oxides, including an interaction-driven Mott insu

109 ture superconductivity is achieved by doping copper oxide insulators with charge carriers.

110 xcitation that appears in the unconventional copper oxide, iron pnictide and heavy fermion supercondu

111 ty of the T(c) versus A(1)( ) relation among copper oxides, iron-based and organic superconductors ma

112 ature (high-T(c)) superconductivity in doped copper oxides is an enduring problem.

113 ure of the resistivity in the electron-doped copper oxides is caused by spin-fluctuation scattering.

114 A central issue for copper oxides is the nature of the insulating ground sta

115 the anomalous normal state properties of the copper oxides--is correlated with the electron pairing.

116 In high-transition-temperature (high-T(c)) copper oxides, it is generally believed that magnetic ex

117 ransport in thin films of the electron-doped copper oxide La(2 - x)Ce(x)CuO(4).

118 ) and the doping level (x) in electron-doped copper oxide La(2-x)Ce(x)CuO(4) (LCCO).

119 gnetic field is applied perpendicular to the copper oxide layers, while an orthogonal elongated latti

120 een magnetism and superconductivity in these copper oxide materials has intrigued researchers from th

121 conductivity at elevated temperatures in the copper oxide materials there has been a considerable eff

122 as a competing ground state in the high-T(c) copper oxide materials, irrespective of electron or hole

123 d ammonia (30-300 muM) are sprayed through a copper oxide mesh with a 200 mum average pore size, resu

124 The antiferromagnetic ground state of copper oxide Mott insulators is achieved by localizing a

125 derived EQM image arrays from carrier-doped copper oxide Mott insulators.

126 electrode by drop casting using cerium oxide/copper oxide nanocomposite on the glassy carbon electrod

127 ement of the nonlinear optical refraction of copper oxide nanoellipsoids at the wavelength of 400 nm,

128 The optical limiting effect of copper oxide nanoellipsoids is analyzed.

129 ence of band gap of copper nanoparticles and copper oxide nanoellipsoids on their nonlinear optical r

130 study of the nonlinear optical properties of copper oxide nanoellipsoids using 800 nm and 400 nm, 60

131 near optical parameters of the suspension of copper oxide nanoellipsoids were measured to be gamma =

132 icient, commercially available, and reusable copper-oxide nanoparticle (CuO-NPs) and (R)-(-)-DTBM SEG

133 nt on the dissolution rate and solubility of copper oxide nanoparticles (CuO NPs) in soil, and to dev

134 In this study, the green synthesis of copper oxide nanoparticles (CuO NPs) mediated by Azadira

135 Transformation, dissolution, and sorption of copper oxide nanoparticles (CuO-NP) play an important ro

136 xtraction and analytical characterization of copper oxide nanoparticles (CuONPs) at trace levels on s

137 anocomposite based on Gum Arabic, silver and copper oxide nanoparticles (GA@Ag-CuO nanocomposite) was

138 was conducted to investigate the effects of copper oxide nanoparticles (nCuO, 0-100 mg/L), arsenic (

139 thesis of isotopically enriched (99% (65)Cu) copper oxide nanoparticles and its application in ecotox

140 form based on poly (crystal violet) film and copper oxide nanoparticles for the detection of brillian

141 For the first time, we report that copper oxide nanoparticles induce DNA damage in agricult

142 ism for the pH influence on the stability of copper oxide nanoparticles is described.

143 chemical properties of poly (crystal) violet/copper oxide nanoparticles modified carbon paste electro

144 the pH effect on the colloidal stability of copper oxide nanoparticles showed that the sample was st

145 to the photon correlation spectroscopy data, copper oxide nanoparticles synthesized in an aqueous med

146 thod for the synthesis of gelatin-stabilized copper oxide nanoparticles was developed.

147 The synthesized copper oxide nanoparticles were investigated with Fourie

148 g the decomposition of ammonium perchlorate, copper oxide nanoparticles, and sodium azotetrazolate.

149 d exposing them to varying concentrations of copper oxide nanoparticles, we experimentally explored h

150 of the carbon paste electrode modified with copper oxide nanoparticles.

151 f spray-dried alumina granules modified with copper (oxide) nanoparticles and critically assess the e

152 Subsequently, copper (oxide) nanoparticles provided a large number of

153 e anodes is achieved via oxidative growth of copper oxide nanowires onto copper substrates followed b

154 In the high-temperature superconducting copper oxides, only one spatial arrangement of the elect

155 paste electrode (CPE) and modified CPE with copper oxide or copper yttrium oxide were prepared for d

156 opper oxide, as well as composites of silver/copper oxide or silver/titania can be routinely prepared

157 ose static form occurs in only one family of copper oxides over a narrow range of the phase diagram.

158 In the copper oxide parent compounds of the high-transition-tem

159 ion temperature superconductor with a single copper oxide plane per unit cell.

160 cused on the high-symmetry directions of the copper oxide plane.

161 n anomalous increase of the distance between copper oxide planes on cooling, which results in negativ

162 ntiferromagnetic (insulating) regions within copper oxide planes, which would necessitate an unconven

163 The copper oxide quasiparticles therefore apparently exhibit

164 Rare-earth-barium-copper-oxide (ReBCO) superconducting tapes are pivotal f

165 of high-temperature superconductivity in the copper oxides remains elusive.

166 the high-transition-temperature (high-T(c)) copper oxides remains the subject of active inquiry; sev

167 the Nickel oxide (rGO-NiO), Silver (rGO-Ag), Copper oxide (rGO-CuO) doped Graphene Oxide are reported

168 e-to-ammonia conversion over nickel-modified copper oxide single-atom alloy oxide nanowires.

169 llmark of the complex chemistry that governs copper oxide superconductivity as manifested in the cele

170 ng state are central issues in understanding copper oxide superconductivity.

171 thought to describe the essential details of copper oxide superconductivity.

172 rconductors and understanding the origins of copper oxide superconductivity.

173 In both the iron arsenides and the copper oxides, superconductivity arises when an antiferr

174 net validates predictions(11) for high-field copper oxide superconductor magnets by achieving a field

175 r this material resembles a high-temperature copper oxide superconductor or a low-temperature metalli

176 ke charge order is generic to the hole-doped copper oxide superconductors and competes with supercond

177 s for the putative vortex-glass state in the copper oxide superconductors are examined.

178 The high-temperature copper oxide superconductors are of fundamental and endu

179 evidence that the hour-glass spectrum in the copper oxide superconductors arises from fluctuating str

180 a5/3Sr1/3CoO4, an insulating analogue of the copper oxide superconductors containing cobalt in place

181 hypothesized that the pseudogap phase of the copper oxide superconductors contains such a 'pair densi

182 h transition temperatures (high-T(c)) of the copper oxide superconductors has led to collective spin

183 The normal state in the hole underdoped copper oxide superconductors has proven to be a source o

184 s been seen in hole-doped crystals; only the copper oxide superconductors have higher transition temp

185 s on high-transition-temperature (high-T(c)) copper oxide superconductors have revealed the existence

186 The high-transition-temperature (high-T(c)) copper oxide superconductors have unusual, highly two-di

187 of the high-transition-temperature (high-Tc) copper oxide superconductors is that they are convention

188 A universal feature of the copper oxide superconductors is the existence of a reson

189 Close to optimal doping, the copper oxide superconductors show 'strange metal' behavi

190 as a central feature in the normal state of copper oxide superconductors(5-9).

191 seudogap, which is generic to all hole-doped copper oxide superconductors, and stripes, whose static

192 pre-formed in the normal state of underdoped copper oxide superconductors, awaiting transition to the

193 s of high-transition-temperature (high T(c)) copper oxide superconductors, but their possible role in

194 In the high-T(c) copper oxide superconductors, however, a pseudogap exten

195 lication in other complex solids--notably in copper oxide superconductors, in which the role of Cu-O

196 The physics of underdoped copper oxide superconductors, including the pseudogap, s

197 However, in the copper oxide superconductors, neither of these descripti

198 roscopic measurements in the hole underdoped copper oxide superconductors, point to a nodal electron

199 -based superconductors on equal footing with copper oxide superconductors, where a similar relation h

200 d in gases of cold fermions and inferred for copper oxide superconductors.

201 d because of similarities with the high-T(c) copper oxide superconductors.

202 seem to hint at a strong similarity with the copper oxide superconductors.

203 from that of the pseudogap behaviour in the copper oxide superconductors.

204 response above T(c) in hole-doped high-T(c) copper oxide superconductors.

205 chemical and structural relationships to the copper oxide superconductors.

206 als, as observed in the phase diagram of the copper oxide superconductors.

207 and high-transition temperature (high-T(c)) copper oxide superconductors.

208 would represent a new view of the underdoped copper oxide superconductors.

209 ttering rate-for three different families of copper oxide superconductors.

210 e of spin-charge separation phenomena in the copper oxide superconductors.

211 urements of La2-xSrxCoO4 and many hole-doped copper oxide superconductors.

212 viour and therefore superconductivity in the copper oxide superconductors.

213 dichotomous behaviour observed in underdoped copper oxide superconductors.

214 able as doped antiferromagnets, of which the copper-oxide superconductors are the most prominent repr

215 optimal doping, high-transition-temperature copper-oxide superconductors exhibit 'strange metal' beh

216 have been observed in nearly all families of copper-oxide superconductors.

217 The three central phenomena of cuprate (copper oxide) superconductors are linked by a common dop

218 chlorophenol at 230 degrees C (2-MCP-230) on copper oxide supported by silica, 5% Cu(II)O/silica (3.9

219 show that a model NHC binds covalently to a copper oxide surface under UHV conditions.

220 on oil-infused heterogeneous nanostructured copper oxide surfaces, we demonstrated approximately 100

221 and acetate were used as precursors for the copper oxide synthesis.

222 ith magnesium diboride and Rare-Earth-Barium-Copper-Oxide technologies.

223 rmal volume expansion, for layered ruthenium copper oxides that have been doped to the boundary of an

224 In copper-oxides that show high-temperature superconductivi

225 By contrast, in copper oxides the carrier density is low whereas T(c) is

226 In electron-doped copper oxides, the absence of an anomalous pseudogap pha

227 ventional in the high-transition-temperature copper oxides, the relative importance of phenomena such

228 Therefore, like high-T(c) copper oxides, the superconducting regime in these iron-

229 g mechanisms in the simplest superconducting copper oxide-the infinite-layer compound ACuO2 (where A

230 s of high-transition-temperature (high-T(c)) copper oxides, there have been efforts to understand the

231 In underdoped copper oxides, there is strong evidence that an energy g

232 calculate the Hamakers constant of symmetric copper oxide thin films based on experimentally obtained

233 utilized to deposit conformal antibacterial copper oxide thin films on the hierarchical surface stru

234 But in the copper oxides this has been a long-standing technical ch

235 In underdoped copper oxides, this normal state hosts a pseudogap and o

236 ere, using the interfacial transformation of copper oxide to copper as an example, we demonstrate the

237 the high-transition-temperature (high-T(c)) copper oxides two decades ago, it has been firmly establ

238 ear excitation of certain phonons in bilayer copper oxides was recently shown to induce superconducti

239 bon dots stabilized silver nanoparticles and copper oxide, was used as an electrocatalyst and signal

240 gin of high-temperature superconductivity in copper oxides, we must understand the normal state from

241 tion-temperature superconductivity arises in copper oxides when holes or electrons are doped into the

242 semblance to the high-transition-temperature copper oxides, whereas the second approach emphasizes th

243 non of high-temperature superconductivity in copper oxides, which is intimately related to the two-di

244 A critical question in the study of copper oxides with high critical transition temperature

245 Many copper oxides without stripe order, however, also exhibi

246 m oscillation measurements in the underdoped copper oxide YBa2Cu3O6 + x.