ライフサイエンスコーパス: copper oxide

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

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

3 or high temperature superconductivity in the copper oxides.

4 s a general property of superconductivity in copper oxides.

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

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

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

8 t from outside the family of superconducting copper oxides.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

38 Copper-oxide-based high-temperature superconductors have

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

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

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

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

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

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

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

46 Copper oxide clusters synthesized via atomic layer depos

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

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

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

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

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

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

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

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

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

56 Although the copper oxides exhibit very high transition temperatures,

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

96 The copper oxide quasiparticles therefore apparently exhibit

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

125 chemical and structural relationships to the copper oxide superconductors.

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

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

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

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

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

131 viour and therefore superconductivity in the copper oxide superconductors.

132 dichotomous behaviour observed in underdoped copper oxide superconductors.

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

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

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

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

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

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

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

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

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

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

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

144 In copper-oxides that show high-temperature superconductivi

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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