ライフサイエンスコーパス: magnetic moment

1 ells is confirmed by a quenching of the spin magnetic moment.

2 single-ion crystal field and the size of the magnetic moment.

3 of the spin only contribution to the overall magnetic moment.

4 o probe the location of the particle and its magnetic moment.

5 nificant orbital contribution to the overall magnetic moment.

6 port, ferroelectric domain walls can carry a magnetic moment.

7 magnetic probes with a controllable low/high magnetic moment.

8 molecules, oxygen is the only one to carry a magnetic moment.

9 cle Kondo resonance, which arises from their magnetic moment.

10 nge of 39-52 K attributed to the [MnSb4](9-) magnetic moment.

11 art of the Co film has the usual density and magnetic moment.

12 (001) induces Kondo screening of the central magnetic moment.

13 extremely small average value of the ordered magnetic moment.

14 d to come from the interfacial uncompensated magnetic moment.

15 didate magnetoreceptive cells based on their magnetic moment.

16 between conducting electron spins and local magnetic moments.

17 nduction band carriers and a high density of magnetic moments.

18 t we can also recognize cells with different magnetic moments.

19 al model of Hall devices to verify the probe magnetic moments.

20 re are no known examples featuring localized magnetic moments.

21 = Gd to Tm, Y), six of which bear localized magnetic moments.

22 ensation of the different Fe(II) and Fe(III) magnetic moments.

23 within the nanocrystal that exhibit coupled magnetic moments.

24 anoparticles are strongly dependent on their magnetic moments.

25 ow the formation of materials with modulated magnetic moments.

26 cooling accompanied by the loss of localized magnetic moments.

27 actions between conduction electrons and the magnetic moments.

28 rized neutron reflectometry to measure their magnetic moments.

29 mind's eye, to yield transition electric and magnetic moments.

30 of magnetic materials with inherently larger magnetic moments.

31 ly predict the experimental room temperature magnetic moments.

32 switching and permits canting of the ordered magnetic moments.

33 ry of reflectivity shows a very small static magnetic moment ( 2 emu/cm(3)).

34 ity measurements, which indicate a very high magnetic moment (5.16muB) likely due to a high degree of

35 ll number of cells (1 in 476,000) with large magnetic moments (8-106 fAm(2)) from various tissues.

36 se of FePc a 10-fold increase of the orbital magnetic moment accompanies charge transfer and a transi

37 ered magnetic moments intensifies, and these magnetic moments align in parallel.

38 rgy per particle responsible for holding the magnetic moment along certain directions becomes compara

39 electrons an additional unbounded quantized magnetic moment along their propagation direction.

40 hat lead to magnetoelectric coupling, namely magnetic moment and a conducting channel, does not neces

41 egenerate ground state gives rise to a large magnetic moment and a remarkably large internal hyperfin

42 The magnetic moment and anisotropy of magnetite nanoparticle

43 ars is predicted to be a spin 1/2 fermion of magnetic moment and charge 0 and lifetime infinity.

44 microscopy because electrons possess both a magnetic moment and charge.

45 ctively mediate the interaction of molecular magnetic moment and electronic spin in underlying metall

46 The intrinsic Fe local magnetic moment and Fe orbital occupations of iron-based

47 nd to be crucial for reproducing the correct magnetic moment and geometry of the isolated manganese p

48 orrelates with the magnitude of the local Fe magnetic moment and its non-monotonic dependence on Co c

49 rganic pi-conjugated polymer with very large magnetic moment and magnetic order at low temperatures.

50 conductor showing a large hysteresis in both magnetic moment and magnetoresistance associated with a

51 ctural stability during the disappearance of magnetic moment and occurrence of axial alternative comp

52 envelopes is determined by the lanthanide's magnetic moment and was found to be a sensitive probe of

53 on the increasing trend to exploit the large magnetic moments and anisotropies of f-element ions.

54 A novel system featuring local magnetic moments and extended 2D electrons is the interf

55 l properties such as atomic spin and orbital magnetic moments and local magnetocrystalline anisotropy

56 tiferromagnetic domains show no net external magnetic moment, and so are difficult to manipulate or p

57 ine the average rotational drag coefficient, magnetic moment, and the frequency and amplitude of the

58 vided into two classes: those with localised magnetic moments, and those with itinerant charge carrie

59 he magnitude of both the orthorhombicity and magnetic moment are suppressed in the superconducting st

60 The ordered magnetic moments are 3.65(5) mu(B)/Mn for Pn = As, and 3

61 agnetic traps confine atoms whose electronic magnetic moments are aligned anti-parallel to the magnet

62 urthermore, quantitative values of the probe magnetic moments are obtained by determining their real

63 and magnetic entropy (SM) indicate that the magnetic moments are randomly distributed within the equ

64 ant and can be controlled by doping, so that magnetic moments are switched on and off.

65 crucial to account for the reduction of the magnetic moment as observed in the experiments.

66 Sources with equivalent magnetic moments as large as 1.3 x 10(17) ampere-meter2

67 found to have similar unpaired electrons and magnetic moments as their isovalent REs (namely Nd and E

68 properties originate from the large in-plane magnetic moment associated with the interlayer optical t

69 Rare-earth elements can be used to introduce magnetic moments associated with the uncompensated spin

70 Whereas the cobalt cores lose their magnetic moment at 10 K in the first system, they remain

71 The induced magnetic moment at 60 T might suggest that only one subs

72 ctric-field control and manipulation of this magnetic moment at room temperature is also shown.

73 ed that the in-plane component of the canted magnetic moment at the CoFe/BiFeO3 interface can be reve

74 e band energetics, morphology, and even spin magnetic moment at the metal-organic interface by interf

75 characterized, in which the disorder of the magnetic moments at low temperatures is precisely analog

76 rdinations at the surface result in enhanced magnetic moments at Mn sites that may play a role in cat

77 multiple locations, with the upper specific magnetic moment being <3.1 x 10(-5) ampere-square meters

78 imensional noncovalent networks exert on the magnetic moments between 2 and 300 K of 1-D (4), 2-D (5)

79 peting interactions between nearest-neighbor magnetic moments can be directly controlled, thus allowi

80 The collective behaviour of interacting magnetic moments can be strongly influenced by the topol

81 s in terms of blocking temperature (TB), net magnetic moment, coercivity, and remnance.

82 The magnetic moment collapse process didn't induce volume an

83 Evolutions of magnetic moment collapse with pressure are confirmed by

84 this device due to the increasing degree of magnetic moment compensation in the superlattice.

85 he highly cross-linked polymer, an effective magnetic moment corresponding to an average S of about 5

86 The behavior of the net magnetic moment DeltamAFM in the antiferromagnet is dire

87 nd is attributed to suppression of the local magnetic moments, destabilizing the initial fcc structur

88 Electron paramagnetic resonance and solution magnetic moment determination confirm the high-spin stat

89 While in all cases the preferred magnetic moment direction is (010) at low temperatures,

90 tron, which modifies their energy levels and magnetic moments, effectively distinguishing them from t

91 The prospect of controlling magnetic moments electrically or optically will lead to

92 ant magnetoresistive sensor and uniform high-magnetic-moment FeCo nanoparticles (12.8 nm)-based detec

93 In contrast, the total magnetic moment for Dy2Mn4 MCs is much larger than the s

94 s parallel alignment of the orbital and spin magnetic moments for electrons and antiparallel alignmen

95 directly proportional to the squares of the magnetic moments for the solvated metal complexes for tw

96 density of states, and Millikan populations (magnetic moment) for each atom, as well as calculate the

97 In this new state of matter, the magnetic moment fragments into an ordered part and a per

98 d by a spin reorientation of the [MnSb4](9-) magnetic moments from the ab-plane to c-axis.

99 t 60 T might suggest that only one subset of magnetic moments has aligned along the field direction.

100 ions with lanthanides of different effective magnetic moments have been examined by 31P magic angle s

101 t accurate quantification of the size of the magnetic moment in a 5d(2) system of 0.60(2) muB -a sign

102 The results show the enhanced net magnetic moment in BFO from the LSMO/BFO interface exten

103 lattice and dopant ions, rendering a higher magnetic moment in bixbyite relative to corundum Mn-dope

104 ss-doped, superconducting LSCO films show no magnetic moment in neutron reflectivity, both above and

105 the vicinity of the Fermi surface and local magnetic moment in pristine TMDs has greatly hampered th

106 A toroidal magnetic moment in the absence of conventional total mag

107 nonmagnetic systems, the ferromagnet-induced magnetic moment in the adjacent nonmagnetic material sig

108 The residual magnetic moment in the aluminum-bearing perovskite is si

109 f magnetic impurities establishes a distinct magnetic moment in the graphene lattice, where the inter

110 lent rare-earth ions, Eu(3+) ions possess no magnetic moment in the ground state.

111 scover for the first time a reduction of the magnetic moment in the plane of rotation at the metamagn

112 erature, the linear 1 displayed an effective magnetic moment in the range 7.0-7.50 mu(B), consistent

113 whose existence indicates that Ni retains a magnetic moment in the superconducting state.

114 ess the issue of toroidal arrangement of the magnetic moment in these systems.

115 copy supports the existence of large orbital magnetic moments in 1 and 2, and DFT calculations provid

116 The depth dependence of magnetic moments in BFO/LSMO superlattices as a function

117 law fits of the high-temperature data yield magnetic moments in close agreement with those expected

118 The overall results indicate that magnetic moments in graphite oxide slowly interact and d

119 is shown that self-damage creates localized magnetic moments in previously nonmagnetic plutonium.

120 idence that these electrons localize to form magnetic moments in pure Pu.

121 f these walls causes statistical flipping of magnetic moments in randomly oriented grains of the hard

122 Furthermore, diluted magnetic moments in semiconductors can be strongly coupl

123 in, and not caused by long-range ordering of magnetic moments in the bulk.

124 ty of the ferromagnetic to form dilute local magnetic moments in the NM.

125 antiferromagnetic ordering of the manganese magnetic moments in the outer layers of the perovskite s

126 Ab initio calculations predict toroidal magnetic moments in the two Ln3 triangles, which are fou

127 In fact, the interacting magnetic moments in these systems do not order, but are

128 We observe that the total Pd magnetic moments induced at the top Co/Pd interface are

129 s, the weak magnetism displayed by unordered magnetic moments intensifies, and these magnetic moments

130 xtremes: an instability in a liquid of local magnetic moments interacting through conduction electron

131 ehicle to stroboscopically transduce a local magnetic moment into an electrical signal while retainin

132 eV, the branching ratio is 0.722(4), and the magnetic moment is 1.9(4) mu(B).

133 chiral spin torque and the proximity-induced magnetic moment is demonstrated by interface engineering

134 uctivity to arise, the local, fluctuating Fe magnetic moment is enhanced near optimal superconductivi

135 0.7)Sr(0.3)MnO(3) (LSMO), we find that a net magnetic moment is induced in the first few unit planes

136 tion metal ferrimagnetic compounds where net magnetic moment is nonzero at TA, the field-driven DW mo

137 moment in the absence of conventional total magnetic moment is observed in a {Dy(6)} ring.

138 A small uncompensated Mn magnetic moment is observed which is antiparallel to the

139 between the second-order rate constants and magnetic moments is consistent with Wigner's theory, the

140 the distribution of iron dopants with frozen magnetic moments is found to be non-uniform.

141 rent-induced switching in the orientation of magnetic moments is observed in cobalt/copper/cobalt san

142 or the net toroidal arrangement of the local magnetic moments is the high symmetry of the complex in

143 nal, indicative of the presence of localized magnetic moments, is observed only for M = Cu and Mn com

144 ne decorated by -COOH groups exhibit ordered magnetic moments, leading to a multiferroic organometall

145 FePt has high Curie temperature, saturation magnetic moment, magneto-crystalline anisotropy, and che

146 her magnetotactic bacteria, to combine their magnetic moments, magnetosomes align along filaments for

147 The resulting zero net magnetic moment makes magnetism in antiferromagnets exte

148 The magnetic moments measured at room temperature support th

149 iffraction, cyclic voltammetry, UV-vis, EPR, magnetic moment measurements, and DFT to confirm the pre

150 outermost Cu2O layer induces a considerable magnetic moment, mostly contributed by 2p orbitals of th

151 results of the NPD along with the saturation magnetic moment (MS) and magnetic entropy (SM) indicate

152 tosomes (radius rmag approximately 10(-7) m, magnetic moment mu approximately 2 x 10(-15) A m2) and t

153 noncentrosymmetric uniaxial magnetic ion of magnetic moment mu at a site of local electric dipole mo

154 eveal an asymmetric doping dependence of the magnetic moments mu bare in electron- and hole-doped BaF

155 energy gap are predicted to have an orbital magnetic moment, mu(orb), that is much larger than the B

156 etely quenched although CrBz has the highest magnetic moment, namely 6 mu(B), in the 3d metal-benzene

157 etailed information about the arrangement of magnetic moments near interfaces.

158 In contrast, the magnetic moment of (1-MeIm)(2)Fe(III)(OEPO) drops with t

159 The magnetic moment of (2,6-xylylNC)(2)Fe(II)(OEPO(*)) is te

160 , Cu(II)) is a copper spin-1/2 system with a magnetic moment of 1.05 +/- 0.04 muB/molecule, slightly

161 temperature-independent paramagnetism with a magnetic moment of 1.36 mu(B) at room temperature.

162 expected solely on the basis of the smaller magnetic moment of 13C.

163 The magnetic moment of 2 (3.50 mu(B)) in solution is consist

164 Magnetic studies produced an effective magnetic moment of 2.60 mu(B) at 23 degrees C, which is

165 Mn2Hg5-type structure, exhibits a saturated magnetic moment of 2.71 muB per formula unit with T(C) a

166 12@Pb20, are designed, which combine a large magnetic moment of 28 microB, a moderate HOMO-LUMO gap,

167 g in a high-spin-polarized current and local magnetic moment of 2D Ti-based TMDs toward half-metallic

168 surements of Na4ZnU6F30 yielded an effective magnetic moment of 3.42 muB for the U(4+) (f(2)) cation

169 tent with an (N(2))(3-) ligand, but the high magnetic moment of 4f(9) Dy(3+) precluded definitive ide

170 tic superatom with a filled d-subshell and a magnetic moment of 5.0 muB.

171 The metallic core has a spin magnetic moment of 5.3 muB in agreement with experiment.

172 and the chemisorbed atom results in a large magnetic moment of 7 muB along with high in-plane magnet

173 t is much larger than the Bohr magneton (the magnetic moment of an electron due to its spin).

174 The ordered magnetic moment of Co(2+) in Sr(2)CoO(2)Cu(2)S(2) (x = 0

175 On the other hand, the magnetic moment of Cr(Bz)(2) is completely quenched alth

176 band calculations confirmed the existence of magnetic moment of Cr2TiAlC2 at 0 GPa and disappearance

177 Here we report the detection of an induced magnetic moment of Eu(3+) ions in GaN which is associate

178 Evolutions of magnetic moment of Fe2MnAl display distinct variation tr

179 Moreover, the total fluctuating magnetic moment of FeSe is approximately 60% larger than

180 combined effect of these changes is that the magnetic moment of high- and low-spin ions such as Cu an

181 The magnetic moment of Mn2FeAl shows an increasing tendency

182 e of ~2.29 MHz/T, corresponding to a nuclear magnetic moment of mu(n) approximately 0.15mu(N) (where

183 ing characteristics, stability, and the spin magnetic moment of neutral and cationic AgnV clusters ha

184 On that basis the magnetic moment of the cuboids can be explained.

185 ith a long-term average virtual axial dipole magnetic moment of the Earth of only 4.9 +/- 2.4 x 10(22

186 rovided the first evidence for the anomalous magnetic moment of the electron, inspired Schwinger's re

187 e Fe-Si/Al atomic planes does not change the magnetic moment of the film up to the very interface.

188 transition is accompanied by a change in the magnetic moment of the oxide and can be related to a val

189 t the temperature variation of the effective magnetic moment of the S2-state multiline EPR signal for

190 O(2) results in a reversible decrease in the magnetic moment of the system, as well as a reduction of

191 tead results in a reversible increase in the magnetic moment of the system, indicating a net ferromag

192 We determined the magnetic moment of this bacterium using a to our knowled

193 ly 0.05, 0.22, and 0.20 eV, all with integer magnetic moments of 1.0 muB.

194 Ni(2+), and Cu(2+)) yielded total effective magnetic moments of 10.2, 9.84, 8.87, and 8.52 muB for t

195 omplexes [Cp'3Dy](-) and [Cp'3Ho](-) exhibit magnetic moments of 11.3 and 11.4 muB, respectively, whi

196 and V{N(H)Ar(Me6)}2 have ambient temperature magnetic moments of 3.41 and 2.77 muB, respectively, whi

197 26 and 18 K, respectively, and with ordered magnetic moments of 3.61(6) and 2.3(1) muB per Mn cation

198 Magnetic moments of 8, 12, and 17 nm diameter CoFe2O4 na

199 n nearest-neighbour dopants, making the full magnetic moments of all dopants observable.

200 due to the exchange interaction between the magnetic moments of Eu-4f and of Ti-3d electrons.

201 Based on the measured magnetic moments of hemoglobin and its compounds, and on

202 This dipolar sensor can determine the magnetic moments of individual adatoms with high accurac

203 Images of the magnetic moments of individual elements in this correlat

204 owever, collisional relaxation of the atomic magnetic moments of non-S-state atoms (non-spherical ato

205 harge carriers interact with large localised magnetic moments of Tb(4f) states, forming complex magne

206 The magnetic moments of the Cr- and Fe-ions are reduced from

207 atively observed a reduced but still sizable magnetic moments of the epitaxial Fe ML on graphene, whi

208 The magnetic moments of the particles are calculated based o

209 more localized Fe electrons and higher local magnetic moments on Fe ions.

210 lds because of the alternating directions of magnetic moments on individual atoms and the resulting z

211 magnetic ordering at T(C) = 180 K is due to magnetic moments on the Fe(13) clusters.

212 e states for cerium and possible presence of magnetic moments on the iron sites.

213 The other utilizes the collective motion of magnetic moments or spin waves with the quasi-particle e

214 ted magnets are materials in which localized magnetic moments, or spins, interact through competing e

215 energy splitting of the ion spins and enable magnetic moment orientation solely by changing either ph

216 tructure theory we find that the theoretical magnetic moments oscillate with cluster size in exact ag

217 A dramatic reduction in the magnetic moment per Fe(2+), approximately 0.40 micro(B),

218 riate bridging ligands enhances the toroidal magnetic moment per unit cell.

219 on between nested, itinerant spins and local magnetic moments provides the organizing principle for t

220 ygens in these facets are ferromagnetic with magnetic moments ranging from 0.2 to 0.5 mu(B).

221 layer V ions which can provide the localized magnetic moments required for scattering the conduction

222 The spatial gradient in magnetic moment results in an anharmonic magnetic force

223 ntrinsic phase separation, while the ordered magnetic moment retains its full value until it is sudde

224 ce, minimizing demagnetizing fields,and that magnetic moments should be configured into an overall cl

225 ignal, depending on their characteristics of magnetic moment, size, and surface-based binding ability

226 spin injection and transport, defect-induced magnetic moments, spin-orbit coupling and spin relaxatio

227 n material CeCoIn(5) is enhanced through the magnetic moments (spins) of individual electrons.

228 ti-layered probes with controllable high/low magnetic moment states.

229 ta with SQUID studies that measure the total magnetic moment suggests that Gd2Mn4 and Y2Mn4 have only

230 ngular momentum contribution that leads to a magnetic moment that is lower than their spin-only value

231 rconductivity develop out of quasi-localized magnetic moments that are generated by strong electron-e

232 rative interaction between individual atomic magnetic moments that results in a macroscopic magnetiza

233 Electron correlations tend to generate local magnetic moments that usually order if the lattices are

234 d with the experimentally determined orbital magnetic moment, the DFT results also demonstrate that b

235 larger contaminant particles with larger net magnetic moments, the pulse magnitudes could be only som

236 ization and gives rise to gradients in local magnetic moments; this is associated with a metal-insula

237 the TI surface, and its electrons gain a net magnetic moment through short-range exchange interaction

238 strange quark contributions to the proton's magnetic moment through the electron-proton weak interac

239 spatially mediating electronic access to the magnetic moment through the Kondo resonance.

240 time domain, we determined the motion of the magnetic moment throughout the process of spin-transfer-

241 ctricity and ferromagnetism, but also enable magnetic moments to be induced by an external electric f

242 utrons go through one beam path, while their magnetic moment travels along the other.

243 strate a very large quenching of the orbital magnetic moment upon bending the linear geometry.

244 tem, only tiny changes of the interfacial Fe magnetic moment upon reversal of the BaTiO(3) dielectric

245 Free magnetic moments usually manifest themselves in Curie la

246 ised by a collective observable (e.g., total magnetic moment), which is read out using a quantum nond

247 essential role of dopant as a carrier of the magnetic moment, which was directly confirmed by X-ray m

248 emically inert 4f electrons set up localized magnetic moments, which are coupled via an indirect exch

249 rrespond to reversed, dynamically precessing magnetic moments, which are known as magnetic droplet so

250 nt of the thermal barrier to reversal of the magnetic moment, while suppressing alternative relaxatio

251 rder is the most stable ground state and the magnetic moment will collapse at about 50 GPa.

252 l fluctuations induce random flipping of the magnetic moment with time, and the nanoparticles lose th

253 electronic structure consists of disordered magnetic moments with all relativistic effects and expli

254 repeated mutual control of ferroelectric and magnetic moments with differential ME coefficients on th

255 ons mediating interactions between localised magnetic moments with strong spin-orbit coupling is like

256 dients around the wires of a steel stent and magnetic moments within MNPs because of a uniform extern