ライフサイエンスコーパス: charge order

1 er) and Cs(V(0.86)Ta(0.14))(3)Sb(5) (without charge order).

2 ncover an unexpected hidden magnetism of the charge order.

3 roscopic pathways, driven by the collapse of charge order.

4 nventional superconductivity and a competing charge order.

5 tures significantly higher than the onset of charge order.

6 an be attributed to the competition with the charge order.

7 t TRS breaking can occur prior to long-range charge order.

8 minutes, pointing to a glassy nature of the charge order.

9 ve vector magnitude of the well-known static charge order.

10 with 4a(0) unidirectional and 2a(0) x 2a(0) charge order.

11 ical interplay between superconductivity and charge order.

12 ormed in Pb films as modulated by the stripe charge order.

13 ductivity likely due to local lifting of the charge order.

14 surement of the critical fluctuations of the charge order.

15 ve role in the coupling between magnetic and charge orders.

16 n in a CDW gap could bridge spin physics and charge orders.

17 with 0.5 < x < 0.9 are antiferromagnetic and charge ordered.

18 dimerization, critical phase separation, or charge ordering.

19 he Neel transition is interpreted as a local charge ordering.

20 allowing for pressure/temperature tuning of charge ordering.

21 that determines the type and temperature of charge ordering.

22 idea of the Fermi surface reconstruction via charge ordering.

23 g and temperature dependence and the role of charge ordering.

24 Rb, Cs)(9-11) exhibit unconventional chiral charge order(12-19), which is analogous to the long-soug

25 flection spectrum, heralding the presence of charge order(13).

26 Here, based on a systematic search for bulk charge order above T(c) using resonant elastic X-ray sca

27 drally-coordinated Fe(2+)-Fe(3+)-Fe(2+) ions charge-ordering along the [110] direction in the inverse

28 It has been shown that charge order and charge disorder can coexist in the rela

29 We resolve the melting time of the charge order and directly observe its amplitude mode, im

30 14))(3)Sb(5), where the Ta-doping suppresses charge order and enhances superconductivity.

31 (3)O(4) in 1939 by Verwey, the nature of the charge order and its role in the transition have remaine

32 aints is an out-of-phase combination of bond charge order and loop currents that we dub a congruent C

33 mpeting with time-reversal symmetry-breaking charge order and offer unique insights into the nature o

34 rgence of an additional 4a(0) unidirectional charge order and strongly anisotropic scattering in diff

35 essitate a re-investigation of the nature of charge order and superconducting pairing in NbSe2 and re

36 Identifying high-temperature unconventional charge order and superconductivity in kagome systems is

37 use muon spin relaxation to probe the kagome charge order and superconductivity in KV(3)Sb(5).

38 The interplay between charge order and superconductivity remains one of the ce

39 survey of superconductivity, the pseudogap, charge order and the Mott state at various doping concen

40 The charge order and three-site distortions induce substanti

41 vations indicate a strong connection between charge order and TRS breaking and suggest that TRS break

42 minent in underdoped samples with coexisting charge order and vanishes with application of a small ma

43 ge order co-exists with short-range magnetic charge order and weak spin ice state.

44 We show that charge ordering and phase separation can be resolved in

45 onductors, including the pseudogap, spin and charge ordering and their relation to superconductivity,

46 ture conducting phase will shed light on how charge ordering and vibrational degrees of freedom deter

47 bilayer graphene(10-12), resonant excitons, charge ordering and Wigner crystallization in transition

48 tudies have led to proposals of a variety of charge-ordered and bond-dimerized ground-state models.

49 dicate that CuIr2S4 undergoes a simultaneous charge-ordering and spin-dimerization transition-a rare

50 epth in single crystals of RbV(3)Sb(5) (with charge order) and Cs(V(0.86)Ta(0.14))(3)Sb(5) (without c

51 ductivity proximate to conventional spin and charge order, and the crossover from long-range phase or

52 electronic nematicity of the Cu 3d orbitals, charge order, and the pseudogap phase as a function of d

53 ression mechanism: the development of broken charge ordering, and its influence on the electronic ban

54 ott insulating states, spontaneous spin- and charge-order, and high-temperature superconductivity.

55 red phase, which, in turn, possesses unusual charge ordering, anti-ferromagnetic ordering, and low, g

56 Charge orders are usually suppressed by chemical doping

57 etal phase, which exhibits antiferroelectric charge order arising from a thermally activated, orbital

58 measured spectra also identifies a non-polar charge ordering arrangement in the LuFe(2)O(4) layer.

59 emical doping and site selective doping of a charge ordered array has not previously been demonstrate

60 Our discovery suggests that similar complex charge ordered arrays could be used to provide surface s

61 tter phase is characterized by Fe(2+)/Fe(3+) charge ordering as well as orbital ordering of the doubl

62 s predicted to support states with monopolar charge order at entropies below that of the previously o

63 uperconducting fluctuations by the competing charge order at low temperatures provides a new perspect

64 to identify a 3-dimensional precursor of the charge order at the L point that condenses into a CDW th

65 Electronically, exotic charge orders at both integer and fractional fillings ha

66 ong served as a prototype of two-dimensional charge ordering, believed to arise from an instability o

67 we observed time-reversal symmetry breaking charge order below [Formula: see text] 110 K in RbV(3)Sb

68 l magnetite, Fe(3)O(4), exhibiting a complex charge-ordering below the Verwey transition, whose natur

69 y visualizes the chiral nature of the Kagome charge order, but also highlights the nonlinear photogal

70 ts superconductivity with suppression of the charge order by doping, analogously to cuprates, these r

71 Here we report an unprecedented charge-ordering cascade in IrTe2 without the loss of met

72 Furthermore, the symmetry of the charge-ordered class-I MV phase is reduced from Pmma to

73 A charge order (CO) with a wavevector [Formula: see text]

74 A charge ordered (CO) insulating state, analogous to a cry

75 In hole-doped (p-type) cuprates, a charge ordering (CO) instability competes with supercond

76 o far the nature of the two-dimensional (2D) charge ordering (CO) state is not clear and no observati

77 Charge ordering (CO), characterized by a periodic modula

78 nds, this transition is often accompanied by charge ordering (CO), resulting in the emergence of comp

79 nables the magnetic ordering to lock in to a charge-ordered commensurate state at lower temperatures.

80 t scattering experiments have suggested that charge ordering competes with superconductivity.

81 rements, our experiments reveal a picture of charge order competing with superconductivity where shor

82 The Mg(2+) and ClO4(-) ions appear charge-ordered, confining the water on length scales of

83 is also naturally accompanied by a period-4 charge order, consistent with recent nuclear magnetic re

84 rrent-voltage spectroscopy data we find that charge order correlates with both structural order and t

85 e finite size and temperature scaling of the charge-ordering correlation.

86 c x-ray scattering (RIXS) studies of dynamic charge order correlations in the cuprates have focused o

87 help understand, for example, the origin of charge order correlations or the isotropic scattering re

88 der evidencing two-dimensional Ce(3+)/Ce(4+) charge ordering correlations.

89 Charge ordering creates a spontaneous array of different

90 Charge ordered defect pyrochlores AM(2+)M(3+)F(6) offer

91 Both the pseudogap and the stripe charge order disappear when the band is either empty or

92 pedance microscopy, enhanced conductivity of charge-order domain walls in the layered manganite Pr(Sr

93 In both phases, charge-order domains occur with domain walls showing enh

94 c screening enables us to observe electronic charge order even in the absence of a moire potential or

95 fraction and dark-field imaging to show that charge order exists in regions with no net magnetization

96 We show that an incipient charge order exists in the antiferromagnetic regime down

97 ore the intricate interplay between the spin-charge order, flat band structures, interlayer coupling,

98 n phase transitions and the role of spin and charge order fluctuations in high-temperature supercondu

99 in the one-dimensional density of states and charge-order fluctuations below 150 K.

100 rmation collectively enhance and stabilize a charge-ordered ground state.

101 onductors but instead have striped spin- and charge-ordered ground states.

102 out fluctuations of short-range directional charge order (i.e., centered around [q(x) = +/-q(CO), q(

103 wavelength with features in common with the charge order identified recently by complementary spectr

104 By directly measuring the associated charge order in a diamond anvil cell at low temperatures

105 , we use ultrashort laser pulses to melt the charge order in CsV[Formula: see text]Sb[Formula: see te

106 These findings strengthen the role of charge order in explaining strange metal phenomenology a

107 The coexisting stripe charge order in IrTe(2) nanoflakes significantly increas

108 report a highly correlated three-dimensional charge order in Pr-substituted YBa(2)Cu(3)O(7), where th

109 of pressure effectively suppresses the spin-charge order in trilayer nickelate La(4)Ni(3)O(10-delta)

110 The recent discovery of a charge order in underdoped YBa2Cu3Oy raised the question

111 ctors, point to a nodal electron pocket from charge order in YBa2Cu3(6+delta).

112 ray diffraction, that revealed signatures of charge order in YBa2Cu3(6+delta).

113 Here, we photoinduce the melting of the charge ordering in a complex three-dimensional solid and

114 Our finding sheds light on the nature of charge ordering in cuprates as well as a reported long-r

115 ide a microscopic explanation of the complex charge ordering in Fe(4)O(5) which "unifies" it with the

116 tors (varistors), oxide tunnel junctions and charge ordering in mixed-valence compounds.

117 g measurements to establish the formation of charge ordering in the high-temperature superconductor B

118 easurements that demonstrate the presence of charge ordering in the n-type cuprate Nd(2-x)Ce(x)CuO4 n

119 100 K, show no indication of low-temperature charge ordering in the racemic material at ambient press

120 Depending on the hole concentration, the charge ordering in this system occurs with the same peri

121 roscopic study on the competing spin-lattice-charge orders in strongly correlated systems.

122 y-dependent photocurrent associated with the charge order, indicating broken inversion and mirror sym

123 Since the proposal of charge order-induced MIT in magnetite Fe(3)O(4) in 1939

124 The charge order induces an intensity anomaly in the bond-bu

125 s generally accompanied by both magnetic and charge-order instabilities, it remains unclear if a cont

126 ed tuning of La2/3Ca1/3MnO3 into an emergent charge-ordered insulating phase with extreme photo-susce

127 suggest that the Cooper pairs grow out of a charge-ordered insulating state, and then condense accom

128 lts point to time-reversal symmetry-breaking charge order intertwining with unconventional supercondu

129 nt MV Fe(2.5+) ions, through a "premonitory" charge ordering into a class-II MV compound, and finally

130 experiments indicate that static stripe-like charge order is generic to the hole-doped copper oxide s

131 Here we show that a similar type of charge order is present in La5/3Sr1/3CoO4, an insulating

132 Charge order is universal to all hole-doped cuprates.

133 The data imply that charge ordering is driven by polaron crystallization int

134 e real- and momentum-space probes, for which charge ordering is emphasized in the tunneling measureme

135 This 'charge order within a charge order' is attributed to the relative instability

136 -edge, which was argued to be a probe of the charge order, is theoretically modelled within the Dynam

137 Charge ordered kagome lattices have been demonstrated to

138 ubiqitous time-reversal symmetry-breaking in charge ordered kagome lattices.

139 The recently discovered charge ordered kagome material ScV(6)Sn(6) does not feat

140 d resonant X-ray diffraction measurements on charge ordered La(1.75)Sr(0.25)NiO(4) to reveal unforese

141 The short-range charge order likely originates from enhanced electron co

142 Ru(3)Si(2) hosts an exceptional interplay of charge order, magnetism, and superconductivity, revealed

143 of strongly correlated materials such as the charge-ordering manganese perovskites, the multiferroic

144 idual atomic columns in the room temperature charge-ordered manganite Bi0.35Sr0.18Ca0.47MnO3 using ab

145 NbSe2 is typical in this sense, and that any charge-ordered material in more than one dimension will

146 The consequences will be observable in many charge-ordered materials, including cuprate superconduct

147 of spins on the V cations, indicating that a charge ordering mechanism drives the structural phase tr

148 ustrates how a collective phenomenon such as charge ordering might be exploited in nanoelectronic dev

149 ions indicate that the insulator consists of charge-ordered Mn(4+) and Mn(3+) with staggered strain-e

150 he cations, distinct from existing manganite charge-order models.

151 any discrete symmetry-breaking aspect of the charge order--nematicity in the case of the unidirection

152 s in the vicinity) exhibits well-defined 1:3 charge order of Mn(4+) and Mn(3+) and orbital order of M

153 tion is described as a disproportionation or charge ordering of [Nb2](7+) dimers: (2[Nb2](7+) --> [Nb

154 in 1939 that this transition is driven by a charge ordering of Fe(2+) and Fe(3+) ions, but the groun

155 (2), (A = alkali metal) where a complete 1:1 charge ordering of Mn(2+) and Mn(3+) is observed along t

156 ical investigations reveal that the peculiar charge ordering of Pb generates two Fe(3+) magnetic subl

157 tructural transition also appears to involve charge ordering of Ru(V) and Ru(VI), causing all Ru(V) t

158 )(0.5)Pb(4+)(0.5)FeO(3) lead to a long range charge ordering of the -A-B-B- type of the layers with t

159 composition and placement, molecular weight, charge, ordering of the aromatic and aliphatic amino-aci

160 "site-selective" Mott scenario without real charge order on Ni sites.

161 lectron diffraction to unveil that a nematic charge order on particular Fe sites emerges in the high-

162 oms, and that the transition is the onset of charge ordering on cooling.

163 f distinct ground states, such as magnetism, charge order or superconductivity.

164 ty is strongly suppressed as static spin and charge orders or "stripes" develop near the doping level

165 presses the symmetry lowering and long-range charge order parameter.

166 eseen photoinduced phase fluctuations of the charge order parameter.

167 Understanding of this charge-ordered parent phase is crucial for deciphering t

168 The corresponding charge-ordered pattern has a fine structure associated w

169 Remarkably, the charge-ordering pattern consists of isomorphic octamers

170 ure magnetism in these superlattices and the charge-ordering pattern in the m = 3 member.

171 The observed Q is intriguingly near the charge-order periodicity required if fluctuating charge

172 is identified well inside the parent stripe charge ordering phase in the thickness-dependent phase d

173 s of periodic lattice displacements near the charge ordering phase transition, we directly visualize

174 Here, we report the realization of the charge-ordered phase in electron-doped (100) SrTiO(3) ep

175 The charge-ordered phase is known to occur in a doped system

176 major driving forces that stabilize various charge-ordered phases of matter.

177 In charge-ordered phases, broken translational symmetry eme

178 ns from a pure Ir(3+) phase to Ir(3+)-Ir(4+) charge-ordered phases, which originate from Ir 5d to Te

179 ize the thermal phase transition between two charge-ordered phases.

180 Charge ordering phenomena can be induced in one dimensio

181 This model provides new insights into charge-ordering phenomena in transition-metal oxides in

182 (REXS), we show that the structure factor of charge order previously identified by STM is absent in t

183 Ti substitution tunes the charge ordering property and reaction pathway, significa

184 wever, the emergence of superconductivity at charge-order QCPs remains shrouded in mystery, despite i

185 er's amplitude fluctuations, and thus limits charge order recovery.

186 wey transition mechanism and the question of charge ordering remain highly controversial.

187 r the time-reversal symmetry breaking of the charge order remains elusive.

188 2Cu3(6+delta), despite the nonobservation of charge order signatures in the same spectroscopic techni

189 sordered spin-ice-like regime to an emergent charge ordered state, in which emergent magnetic charge

190 muon ensemble, which takes place within the charge ordered state.

191 These changes destabilize the charge-ordered state and suppress the temperature at whi

192 tance at low temperature suggests it is in a charge-ordered state below T ~ 17 K.

193 oscopy experiments which probe the 4a0 x 4a0 charge-ordered state discovered by scanning tunneling mi

194 Here the charge-ordered state of stoichiometric CaFe(3)O(5) is pr

195 nd magnetic structure of the low-temperature charge-ordered state provide an unusual opportunity to f

196 We identify a high-temperature charge-ordered state with propagation vector (1/2,0,0) a

197 ion favors electron-lattice coupling for the charge-ordered state, and triggering the stabilization o

198 ong constraints on theoretical models of the charge-ordered state.

199 py, and the favored coulombic structure is a charge-ordered state.

200 in the internal magnetic field width in the charge-ordered state.

201 s, and support the picture that proximity to charge ordered states is a general property of supercond

202 /WS(2) heterobilayer detected incompressible charge ordered states that one can view as generalized W

203 pe CO competes with the "trimeron"/"dimeron" charge ordered states, allowing for pressure/temperature

204 We propose a series of charge-ordered states at commensurate filling fractions

205 tercalation alters the energetics of various charge-ordered states in 1T-TaS2 and produces a series o

206 ken symmetry effect of the antiferromagnetic charge-ordered states in manganites.

207 ntermediate phases in between incompressible charge-ordered states in the strong coupling limit.

208 ovide a new electronic paradigm of localized charge-ordered states interacting with itinerant electro

209 The role of the lattice in charge-ordered states remains particularly enigmatic, so

210 actors, below the melting temperature of the charge-ordered states, and for small sample-gate separat

211 on between electrons and phase mixing of the charge-ordered states.

212 ch set of possible phases upon melting these charge-ordered states.

213 The charge ordered structure of ions and vacancies character

214 superconductor whose Cooper pairs form spin-charge-ordered structures instead of becoming supercondu

215 in complexity with respect to all the known charge-ordered structures, which are typically based on

216 er at the intra-unit-cell level in the model charge-ordered system Nd(1/2)Sr(1/2)MnO(3).

217 n ensemble, which takes place just below the charge ordering temperature and persists into the superc

218 tly, the muon spin relaxation rate below the charge ordering temperature is substantially enhanced by

219 bly, the muon spin relaxation rate below the charge ordering temperature is substantially enhanced by

220 lthough all superconducting cuprates display charge-ordering tendencies, their low-temperature proper

221 eudogap phase accompanied by a global stripe charge order that breaks the rotational symmetry of the

222 to occur from magnetic field enhancement of charge order that is rendered fragile in zero magnetic f

223 We observed this charge ordering to leave a distinct electron-hole asymme

224 eezing of the first-order antiferromagnetic (charge ordered) to ferromagnetic transition.

225 more, the anisotropy drops sharply below the charge order transition, again similar to the electrical

226 decreases with increasing pressure while the charge-ordering transition occurs at ~8 GPa and room tem

227 ar 275 K, Fe(5) O(6) undergoes a Verwey-type charge-ordering transition that is concurrent with a dim

228 Upon applying pressure, the charge-order transitions are suppressed, the superfluid

229 Te2, which is a unique layered material with charge-order transitions into stripe phases.

230 cannot directly image phase coexistence and charge ordering, two key features of the manganites.

231 By resolving both the fluctuating spin and charge orders using DCA, we demonstrate that they surviv

232 ne with radius equal to the magnitude of the charge order wave vector, q(CO).

233 and lifetime shortening are found around the charge ordering wave vector.

234 on to imaging the prototypical site-centered charge order, we discover the nanoscale coexistence of a

235 raction, without the emergence of long-range charge order which sets in at a different propagation ve

236 Such a charge order, which is distinctly different from the wel

237 temperature T(c) ~ 2.5 K, a tri-directional charge order with a 2a(0) period that breaks the transla

238 ally explained as an intra-unit-cell nematic charge order with d-wave symmetry, pointing to the ubiqu

239 r-range couplings of the chargons leading to charge order with longer periods.

240 is state features intra-moire-cell irregular charge orders with spontaneous on-site ordering at the m

241 This 'charge order within a charge order' is attributed to the

242 xt] of the CuO2 planes at low temperature in charge-ordered YBa2Cu3O y We find that [Formula: see tex

243 In the latter, a charge-ordered yet spin-disordered topological phase, th