ライフサイエンスコーパス: charge order

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

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

3 ical interplay between superconductivity and charge order.

4 surement of the critical fluctuations of the charge order.

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

6 idea of the Fermi surface reconstruction via charge ordering.

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

8 dimerization, critical phase separation, or charge ordering.

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

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

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

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

13 The charge order and three-site distortions induce substanti

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

53 100 K, show no indication of low-temperature charge ordering in the racemic material at ambient press

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

81 eseen photoinduced phase fluctuations of the charge order parameter.

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

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

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

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

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

87 In charge-ordered phases, broken translational symmetry eme

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

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

90 Charge ordering phenomena can be induced in one dimensio

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

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

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

94 2Cu3(6+delta), despite the nonobservation of charge order signatures in the same spectroscopic techni

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

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

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

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

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

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

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

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

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

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

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

106 The charge ordered structure of ions and vacancies character

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

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

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

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

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

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

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

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

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

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

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

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