ライフサイエンスコーパス: Curie

1 Cambridge Biomedical Research Centre, Marie Curie Actions, Foundation for Development of Internal Me

2 Both Curie and anti-Curie temperature dependencies are observ

3 The Curie and the SIOPEN score were equally reliable and pre

4 als b-g, i, and j (histidine protons) follow Curie behavior (contact shift decreases with increasing

5 gnals a and h (cysteine protons) follow anti-Curie behavior (contact shift increases with increasing

6 e complexes show significant deviations from Curie behavior, and also evidence of extensive ligand ex

7 shows that the Cu(2+) center displays normal Curie behavior, indicating that the site is a mononuclea

8 Pauli-paramagnetic with an additional small Curie component.

9 The Curie constant indicates a large effective moment corres

10 cted from the hospital information system of Curie Institute-Paris.

11 effect connectivities, (b) prediction of the Curie intercepts from both one- and two-dimensional vari

12 nd International, European Commission (Marie Curie Intra-European Fellowship), Australian National He

13 Although Marie Curie is known primarily for her discovery of radium, he

14 ubstituted MoFe protein were found to follow Curie law 1/T dependence, consistent with a ground-state

15 with an axially symmetric structure, and the Curie law behavior confirms that the triplet state is th

16 ted state leads to strong deviation from the Curie law for the heme substituents experiencing primari

17 erence of the magnetic susceptibility to the Curie law in the range 30-300 K.

18 The EPR signal showed a Curie law temperature dependence similar to the resting

19 to be ferromagnetic as the signals exhibited Curie law temperature dependence.

20 and varied with temperature consistent with Curie-law dependence.

21 netic moments usually manifest themselves in Curie laws, where weak external magnetic fields produce

22 highly resistive, but its susceptibility is Curie-like at high temperatures and orders antiferromagn

23 The impurity spin susceptibility has a Curie-like divergence at the quantum-critical coupling,

24 arge intermolecular spacing, the solid shows Curie paramagnetism in the temperature range 100-400 K,

25 isorder by way of chemical substitution, the Curie point is suppressed, but no qualitatively new phen

26 only weakly temperature-dependent below the Curie point.

27 ve and sporulated biomasses were analyzed by Curie-point pyrolysis mass spectrometry (PyMS) and diffu

28 In this study Curie-Point pyrolysis-gas chromatography-mass spectromet

29 uent compositions having strategically tuned Curie points (T(C)) were designed and integrated with va

30 A Curie score </= 2 and a SIOPEN score </= 4 (best cutoff)

31 A semiquantitative mIBG score (Curie score [CS]) was assessed for utility as a prognost

32 lguanidine ((123)I-MIBG) scoring method (the Curie score, or CS) was previously examined in the Child

33 Neuroblastoma Group] score and the modified Curie score.

34 Curie scoring carries prognostic significance in the man

35 ere assessed according to the SIOPEN and the Curie scoring method.

36 3+)(4f(1)5d(0)).This oxidation state and the Curie shift are consistent with a weakly paramagnetic sy

37 (2700 Hz) with a small temperature-dependent Curie shift.

38 lity measurements indicate approximately 0.7 Curie spins per molecule from room temperature down to 5

39 m is shown for the first time to have a high Curie temperature ( approximately 545 K).

40 exhibiting high electrical conductivity and Curie temperature (Tc) above 300 K would dramatically im

41 12O19 nanoparticles trap electrons below the Curie temperature (TC) and release the trapped electrons

42 duced voltage under applied stress) and high Curie temperature (Tc) are crucial towards providing des

43 challenging to achieve a candidate with high Curie temperature (Tc), controllable ferromagnetism and

44 s C produces large and reversible changes in Curie temperature (up to 150 degrees C).

45 98) dilute magnetic quantum dots show a high Curie temperature above 400 K.

46 polarization switching with a ferroelectric Curie temperature above room temperature.

47 ring of the neighboring Nb ions, so that the Curie temperature and spontaneous polarization remain la

48 nal unmixing, we infer that the variation in Curie temperature arises from cation reordering, and Mos

49 ow that its depth and width enlarge when the Curie temperature decreases.

50 The His Hepsilon1 proton exhibited weak Curie temperature dependence from 283 to 303 K, contrary

51 In the reduced state, the Curie temperature dependence of the Hbeta protons corres

52 ence from 283 to 303 K, contrary to the anti-Curie temperature dependence predicted from the spin cou

53 Both Curie and anti-Curie temperature dependencies are observed for sets of

54 gap, unique ferromagnetic character and high Curie temperature has become a key driving force to deve

55 Here we demonstrate that Curie temperature in a set of natural titanomagnetites (

56 effect of particle size on the ferromagnetic Curie temperature in semiconducting EuS.

57 ic semiconductor, Mn(x)Ge(1-x), in which the Curie temperature is found to increase linearly with man

58 remanence requires fundamental revision when Curie temperature is itself a function of thermal histor

59 strong spin-fluctuation scattering above the Curie temperature is proposed here.

60 Curie temperature is therefore an inaccurate proxy for c

61 0.95)Ti(0.05)O3 films near the ferroelectric Curie temperature of 222 degrees C.

62 Its Curie temperature of 45 kelvin is only slightly lower th

63 ynthesized at high pressure which has a high Curie temperature of 520 K and magnetizations of up to 5

64 A carrier-density-dependent high Curie temperature of 850-930 K has been measured, in add

65 ured magnetic response is singular above the Curie temperature of a model, disordered magnet, and tha

66 opological insulators (with x = 0.05) show a Curie temperature of about 52 K, and the carrier concent

67 excellent ferroelectric properties, but its Curie temperature of approximately 130 degrees C is too

68 Strain has been used to enhance the Curie temperature of BaTiO(3) and SrTiO(3) films, but on

69 veral fundamental challenges such as the low Curie temperature of group III-V and II-VI semiconductor

70 Here, we increase the Curie temperature of micrometre-thick films of BaTiO(3)

71 are and kagome lattices by heating above the Curie temperature of the constituent material.

72 A high ferromagnetic state with a Curie temperature of ~45 K is observed in these nanoplat

73 ly, of ferromagnetism with modulation of the Curie temperature spanning 36 K.

74 states has direct and crucial bearing on its Curie temperature T(C).

75 p2(+))3] shows ferromagnetic ordering with a Curie temperature TC = 20 K.

76 s polarization Ps=13 muC cm(-2) and a higher Curie temperature Tc=438 K with a band gap of 3.65 eV.

77 titution results in ferromagnetic order with Curie temperature up to 30 K and demonstrates that the f

78 onductor, (Ba,K)(Zn,Mn)2As2 (BZA), with high Curie temperature was discovered, showing an independent

79 the three magnetic cations lead to the high Curie temperature, a large saturation magnetization of 8

80 The Curie temperature, based on Arrott plots, is depressed b

81 A magnetic semiconductor having a high Curie temperature, capable of independently controlled c

82 netic susceptibility data exhibit a negative Curie temperature, field irreversibility, and slow relax

83 FePt has high Curie temperature, saturation magnetic moment, magneto-c

84 al ordering in a temperature range above the Curie temperature, T C < T < T*, where a first-order tra

85 mple system is a ferromagnet approaching its Curie temperature, T(C), where all of the spins associat

86 At temperatures T well above the Curie temperature, Tc (where the transition from paramag

87 A simple empirical equation correlated Curie temperature, TC, with the values of ionic radii of

88 perties, we determined that the paramagnetic Curie temperature, Thetap, varies with doping level, in

89 operated at a temperature slightly above the Curie temperature.

90 more dominant at all temperatures below the Curie temperature.

91 duction with no significant influence on the Curie temperature.

92 rcive field (Hc > 1.0 T) and a relative high Curie temperature.

93 history at temperatures just above or below Curie temperature.

94 change in magnetization at the ferroelectric Curie temperature.

95 face greatly enhances the magnetic ordering (Curie) temperature of this bilayer system.

96 aramagnetic nanocrystals exhibit robust high-Curie-temperature (T(C)) ferromagnetism (M(s)(300 K) = 0

97 o find other spin-polarized oxides with high Curie temperatures (well above room temperature) and lar

98 of how, or even whether, properties such as Curie temperatures and bandgaps are related in magnetic

99 for this new technology, and although their Curie temperatures are rising towards room temperature,

100 ll conductance of (GaMn)As, while displaying Curie temperatures as high as 53 K.

101 Estimated Curie temperatures can be up to 376 and 425 K for TiCl3

102 found to be weak itinerant ferromagnets with Curie temperatures close to 10 K.

103 al compounds Co2TiX (X = Si, Ge, or Sn) with Curie temperatures higher than 350 K.

104 We show that the Curie temperatures of the constituent materials can be s

105 Sixteen layers of LaFeMnSiH having different Curie temperatures were employed as magnetocaloric mater

106 scalar physical properties such as bandgaps, Curie temperatures, equation-of-state parameters and den

107 ctrics or enhance electric polarizations and Curie temperatures.

108 However, dominance of high Curie-temperatures due to cluster formation or inhomogen

109 Monte Carlo simulations illustrate very high Curie-temperatures of 292, 472, and 553 K for VS2, VSe2,

110 This is analogous to the Curie transition in simple and frustrated ferro- and ant

111 that appear at high temperatures beyond the Curie transition, form nuclei for the field-induced long

112 terProSurf web server is available at http://curie.utmb.edu/

113 ane exchange coupling that may result in non-Curie Weiss behavior above TN.

114 a, where antiferromagnetic (AFM) exchange, a Curie-Weiss (C-W) temperature of theta = -125 K, and a n

115 eptibility measurements on alpha-1b indicate Curie-Weiss behavior (with Theta = -14.9 K), while the d

116 Deviations from Curie-Weiss behavior begin at 100 K; variation in field-

117 ouplings of the d(1) centers whereas 3 shows Curie-Weiss behavior.

118 The model reproduces the Curie-Weiss law at high temperatures, but the classical

119 Curie-Weiss law fits of the high-temperature data yield

120 urs), classical mean-field theory yields the Curie-Weiss law for the magnetic susceptibility: X(T) in

121 alue of gamma, along with a deviation from a Curie-Weiss law observed in the low-temperature magnetic

122 molar magnetic susceptibility of 3 obeys the Curie-Weiss law with mu(eff) = 2.78 muB and theta = -1.0

123 (chi) data for Y(3)MnAu(5) were fitted by a Curie-Weiss law.

124 Compound 2 exhibits Curie-Weiss paramagnetism, and an antiferromagnetic orde

125 ed picture for both the critical-scaling and Curie-Weiss regimes.

126 metal unpaired electrons on the basis of the Curie-Weiss temperature dependence of the shift.

127 ads to a two-component model consisting of a Curie-Weiss term and a short-ranged interaction term con

128 a high-temperature paramagnetic metal with a Curie-Weiss-like susceptibility.

129 A Curie-Weiss-like temperature dependence for the hyperfin

130 y and functionality was pinpointed by Pierre Curie who stated that it is the symmetry breaking that c