ライフサイエンスコーパス: Curie

1 on through the Horizon 2020 Marie Sklodowska-Curie Actions (MSCA) COFUND scheme and the Welsh Europea

2 Horizon 2020 Marie Sklodowska-Curie Actions and European Society of Cardiology.

3 EU Marie Sklodowska-Curie Actions programme.

4 European Research Council, Marie Sklodowska-Curie Actions, and the Wellcome Trust.

5 Trond Mohn Foundation, Marie Sklodowska-Curie Actions, European Research Council, Royal Society,

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

7 dation, Wellcome Trust, and Marie Sklodowska-Curie Actions.

8 Both Curie and anti-Curie temperature dependencies are observ

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

10 n physics, together with her husband, Pierre Curie), and she was also the first person to win a secon

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

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

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

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

15 Pauli-paramagnetic with an additional small Curie component.

16 ed and delocalized character, with a maximum Curie constant and Li NMR paramagnetic shift near a comp

17 The Curie constant indicates a large effective moment corres

18 cial Research Council, EU Horizon 2020 Marie Curie Fellowship, and Leverhulme Trust Large Centre Gran

19 ovation programme under the Marie Sklodowska-Curie grant agreement No 701464".

20 ospective cohort study conducted at Institut Curie in Paris, France, among 381 consecutive patients d

21 Following the discovery of radium by the Curies in 1898, Amoros became interested in radiology an

22 rds "M.G.F. was funded by a Marie Sklodowska-Curie Individual Fellowship (No 701464)" should have rea

23 ean Commission Horizon 2020 Marie Sklodowska-Curie Individual Fellowship.

24 Swiss National Science Foundation and Marie Curie Individual Fellowship.

25 tific Research (NWO), H2020 Marie Sklodowska-Curie Innovative Training Network European Sepsis Academ

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

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

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

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

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

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

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

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

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

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

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

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

38 uoroborate for one-step radiofluorination at Curie levels of [(18)F] fluoride in good yields and high

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

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

41 on data collected from The Maria Sklodowska-Curie National Research Institute of Oncology in Warsaw.

42 d with palliative intent at Maria Sklodowska-Curie National Research Institute of Oncology, Gliwice B

43 25 (13) FM (AFM) candidates with a predicted Curie (Neel) temperature above 500K (100K) from the Mate

44 The regression models predict Curie (Neel) temperature with a coefficient of determina

45 on in Pennsylvania released about 22 million Curies of xenon-133 into the environment.

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

47 both after annealing near the ferromagnetic Curie point and in a thermally dynamic state.

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

49 t high temperatures ([Formula: see text]C of Curie point).

50 However, because of the low Curie point, the CuInP(2)S(6)-based memory devices suffe

51 only weakly temperature-dependent below the Curie point.

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

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

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

55 0 applications to three actions of the Marie Curie programme over a period of 12 years, we find that

56 musical shines a stylized spotlight on Marie Curie's extraordinary life.

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

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

59 The Curie score for (18)F-MFBG was higher, with an average o

60 core was higher in 50% of the cases, and the Curie score was higher in 70% of the cases.

61 an increased SIOPEN score, and an increased Curie score were seen on [(18)F]MFBG LAFOV PET/CT compar

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

63 Neuroblastoma Group] score and the modified Curie score.

64 The curie scores were also higher for (124)I-MIBG PET/CT tha

65 Modified Curie scores were assigned to both (123)I-MIBG scans, eq

66 esions, the number of total lesions, and the curie scores were recorded for the (123)I-MIBG and (124)

67 Curie scoring carries prognostic significance in the man

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

69 3+)(4f(1)5d(0)).This oxidation state and the Curie shift are consistent with a weakly paramagnetic sy

70 (2700 Hz) with a small temperature-dependent Curie shift.

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

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

73 ly large magnetic moment (0.5 mu(B) /Co) and Curie temperature (75 K), values larger than previously

74 xt] is an intermetallic compound with a bulk Curie temperature ([Formula: see text]) of 6-13 K.

75 ic Sr(2) FeReO(6) , an FMI state with a high Curie temperature (T(c) ~ 400 K) and a large saturation

76 pread application of 2D magnetism requires a Curie temperature (T(c)) above room temperature as well

77 g-range magnetic order in monolayer with the Curie temperature (T(c)) of 45 K.

78 rt and specific heat measurements indicate a Curie temperature (T(C)) of approximately 160 K, while m

79 Intrinsic ferromagnetism with a Curie temperature (T(C)) up to 300 K, an atomic magnetic

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

81 12O19 nanoparticles trap electrons below the Curie temperature (TC) and release the trapped electrons

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

83 c (at low temperatures) transition below the Curie temperature (Tc) in all the samples.

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

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

86 The reshaped Weyl states feature a doubled Curie temperature 50 K and a strong angular transport ch

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

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

89 in a barrierless charge transport below the Curie temperature and a large negative magnetoresistance

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

91 1 k(B) per charge carrier that begins at the Curie temperature and survives more than one order of ma

92 The material is shock-heated above the Curie temperature and therefore may efficiently record t

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

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

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

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

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

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

99 The magnetoresistance shows a peak at the Curie temperature due to the suppression of magnetic sca

100 ured transport energy gap is larger than the Curie temperature for magnetic ordering, and quantizatio

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

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

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

104 and magnetoresistance in the vicinity of the Curie temperature in the highly disordered dilute ferrom

105 The Curie temperature is calculated through spin-lattice dyn

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

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

108 The Curie temperature is negative, implying an analogy with

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

110 Curie temperature is therefore an inaccurate proxy for c

111 Here, motivated by the anomalously high Curie temperature observed in bulk diluted magnetic oxid

112 0.95)Ti(0.05)O3 films near the ferroelectric Curie temperature of 222 degrees C.

113 lly (as verified by Landau theory) above the Curie temperature of 290 kelvin by electric fields of 29

114 A higher Curie temperature of 45 K than that for Li(1+y)(Zn,Mn)P

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

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

117 e in the kagome ferromagnet Fe(3)Sn with the Curie temperature of 760 kelvin.

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

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

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

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

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

123 can be removed by heating samples above the Curie temperature of BaTiO(3).

124 cal insulator Bi(2)Te(3) not only raises the Curie temperature of Fe(3)GeTe(2) (FGT) through interfac

125 ge crystals allowed the determination of the Curie temperature of few-layer SnSe van der Waals ferroe

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

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

128 Furthermore, the Curie temperature of the assemblies is about 40 degrees

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

130 twisted CrI(3), we explicitly show that the Curie temperature of the ferromagnetic state is higher t

131 osheets exhibit robust ferromagnetism with a Curie temperature of ~100 K and remarkably, host a spin-

132 ectric polarization of 70 muC/cm(2) and high Curie temperature of ~1213 K, which are ~2.8 times large

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

134 xt] of ~1098 picometers per volt with a high Curie temperature of ~450 degrees C.

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

136 (2- x)Sn (x)Se(4) FMSs, the magnitude of the Curie temperature strongly depends on the spatial separa

137 developed, rapidly heating the media to the Curie temperature T(c) before writing, followed by rapid

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

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

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

141 fully depoled through annealing above their Curie temperature to revive piezoelectric performances.

142 ))(95)Mo(5) bulk metallic glasses around the Curie temperature to understand the Invar effect they ex

143 le per moire unit cell with a widely tunable Curie temperature up to 14 K.

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

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

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

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

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

149 robust ferromagnetism, but with a suppressed Curie temperature, due to the drastic drop in the densit

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

151 further gap hardening is observed below the Curie temperature, indicating the establishment of an ef

152 rt measurements that are seen well below the Curie temperature, leading to speculation that a "hidden

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

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

155 temperature magnetic moment and a suppressed Curie temperature, T(c) = 27 K (refs.

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

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

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

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

160 By photoemission spectroscopy below the Curie temperature, we observe topological Fermi arcs tha

161 obility in ferromagnetic systems with a high Curie temperature, which is advantageous for topological

162 change in magnetization at the ferroelectric Curie temperature.

163 se magnitude reaches a peak value around the Curie temperature.

164 cted totally symmetric distortions above its Curie temperature.

165 ion and the correlations above and below the Curie temperature.

166 ntally affecting uniformity, scalability, or Curie temperature.

167 operated at a temperature slightly above the Curie temperature.

168 more dominant at all temperatures below the Curie temperature.

169 duction with no significant influence on the Curie temperature.

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

171 history at temperatures just above or below Curie temperature.

172 the exchange interactions and increases the Curie temperature.

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

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

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

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

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

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

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

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

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

182 ture, which are in-plane ferroelectrics with Curie temperatures of 320 to 420 degrees C.

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

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

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

186 ctrics or enhance electric polarizations and Curie temperatures.

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

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

189 d from three centers (training set: Institut Curie; test set: Institut Godinot and Institut Oscar Lam

190 l fluctuations in magnetite emerge below the Curie transition at T(C) ~ 850 K, through X-ray pair dis

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

192 In conventional ferroelectrics, the Curie transition is caused by a change in crystal symmet

193 netic semiconductors (FMSs) featuring a high Curie transition temperature ( T(c)) and a strong correl

194 oethylene (P(VDF-TrFE)) strongly affects its Curie transition, as not only a change in crystal symmet

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

196 ric state driven by temperature - called the Curie transition.

197 Marie Curie was born in Warsaw in1867.

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

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

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

201 etic measurements of these assemblies reveal Curie-Weiss behavior at high temperatures, without pairi

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

203 DC SQUID magnetometry reveals Curie-Weiss behavior for T > 20 K (C = 0.376 emu K mol(-

204 We observe Curie-Weiss behavior in the obtained octupolar susceptib

205 The Curie-Weiss behavior provides a pathway to an ideal glas

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

207 Mott insulating state with antiferromagnetic Curie-Weiss behaviour, as expected for a Hubbard model i

208 Curie-Weiss fitting applied to magnetization data sugges

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

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

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

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

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

214 he structure function, S(Q) - 1, follows the Curie-Weiss law.

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

216 We show that the Curie-Weiss model with molecule structures exhibits a fi

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

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

219 viour, other features-including its negative Curie-Weiss temperature and a lack of long-range orderin

220 The CrSbSe(3) nanowires display reduced Curie-Weiss temperature but higher coercivity and remane

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

222 long-range magnetic order down to ~5% of the Curie-Weiss temperature.

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

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

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

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