ライフサイエンスコーパス: magnetic moment

1 MWCNTs (change of magnetic state of blocked magnetic moments).

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

3 extremely small average value of the ordered magnetic moment.

4 d to come from the interfacial uncompensated magnetic moment.

5 didate magnetoreceptive cells based on their magnetic moment.

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

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

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

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

10 nificant orbital contribution to the overall magnetic moment.

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

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

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

14 netic properties, such as magnetic order and magnetic moment.

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

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

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

18 irectly by acting on the interaction between magnetic moments.

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

20 of magnetic materials with inherently larger magnetic moments.

21 ly predict the experimental room temperature magnetic moments.

22 switching and permits canting of the ordered magnetic moments.

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

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

25 re are no known examples featuring localized magnetic moments.

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

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

28 within the nanocrystal that exhibit coupled magnetic moments.

29 anoparticles are strongly dependent on their magnetic moments.

30 ow the formation of materials with modulated magnetic moments.

31 cooling accompanied by the loss of localized magnetic moments.

32 de complex carrying sizable spin and orbital magnetic moments.

33 es due to strong quantum fluctuations of the magnetic moments.

34 at 10.5 tesla from the precession of induced magnetic moments.

35 between conducting electron spins and local magnetic moments.

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

37 rized neutron reflectometry to measure their magnetic moments.

38 omically thin LCO layers, surprisingly large magnetic moment (0.5 mu(B) /Co) and Curie temperature (7

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

40 ptical band-gap (2.4 eV), and a large enough magnetic moment (~200 emu/cc), all of which can be tuned

41 n of this spin-valley index, which carries a magnetic moment(3), requires tuning its energy.

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

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

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

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

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

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

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

49 acancies in Co(3)Sn(2)S(2.) The SOPs carry a magnetic moment and a large diamagnetic orbital magnetiz

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

51 The magnetic moment and anisotropy of magnetite nanoparticle

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

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

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

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

56 is a strong correlation between the overall magnetic moment and free carrier spin in FeSb(2- x)Sn (x

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

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

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

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

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

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

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

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

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

66 rromagnets is challenging due to their small magnetic moments and the ambiguous role of local interac

67 r alloys, where high spin polarization, zero magnetic moment, and low magnetic damping can be achieve

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

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

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

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

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

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

74 ltilayered structures, FeNi nanoisland giant magnetic moments are interacting due to the indirect exc

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

76 ion between itinerant carriers and localized magnetic moments are of tremendous importance for the de

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

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

79 trated magnetic interactions with changes in magnetic moment as a function of temperature between 150

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

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

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

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

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

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

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

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

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

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

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

91 lishes the formation of robust perpendicular magnetic moments at the interface.

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

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

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

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

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

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

98 Evolutions of magnetic moment collapse with pressure are confirmed by

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

100 etic substrate or in the orientations of the magnetic moments concerning a given direction in space.

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

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

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

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

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

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

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

108 escribe the dynamics of large, Ising-like Yb magnetic moments, ensuring that the measured excitations

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

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

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

112 c-axis antiferromagnetic orientation of the magnetic moments for the bilayer, as in Sr(3)Ir(2)O(7).

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

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

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

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

117 he calculations show that a deviation of the magnetic moments from the c-axis leads to the breaking o

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

135 lain the formation of the very large ordered magnetic moments in [Formula: see text] and [Formula: se

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

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

138 Further, compensation of magnetic moments in ferrimagnetic materials can signific

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

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

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

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

143 s (ISHEs), enable the reading and control of magnetic moments in spintronics.

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

145 t are antiferromagnetically coupled to the V magnetic moments in the ground state.

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

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

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

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

150 llenging, due to its inherently weak nuclear magnetic moment, in contrast to other alkali ions such a

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

152 Internal magnetic moments induced by magnetic dopants in MoS(2) m

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

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

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

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

157 nds that upon dopant substitution, the local magnetic moment is decreased and its magnitude is depend

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

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

160 0.7)Sr(0.3)MnO(3) (LSMO), we find that a net magnetic moment is induced in the first few unit planes

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

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

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

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

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

166 een non-equilibrium thermal fluctuations and magnetic moments is illustrated using Lighthill's formul

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

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

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

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

171 rromagnetic NPs ever reported, and saturated magnetic moment (M(s) ) of 88.7 emu g(-1) , the highest

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

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

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

175 The magnetic moments measured at room temperature support th

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

177 troscopy, high-resolution mass spectrometry, magnetic moment measurements, and supporting CASSCF calc

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

193 12@Pb20, are designed, which combine a large magnetic moment of 28 microB, a moderate HOMO-LUMO gap,

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

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

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

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

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

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

200 materials combine the advantages of the low magnetic moment of an antiferromagnet and the ease of re

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

202 ples to the spin, atomic orbital, and valley magnetic moment of carriers from the conduction and vale

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

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

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

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

207 closely related to the decrease in the spin magnetic moment of Fe.

208 Evolutions of magnetic moment of Fe2MnAl display distinct variation tr

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

210 By tuning the net magnetic moment of Gd(x) (FeCo)(1-) (x) via changing the

211 The saturation magnetic moment of h-CBN reaches 0.033 emu g(-1) at 300

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

213 The magnetic moment of Mn2FeAl shows an increasing tendency

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

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

216 the weak ferromagnetic properties and excess magnetic moment of PFWO can be understood based on non-r

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

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

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

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

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

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

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

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

225 eutron diffraction measurements revealed the magnetic moments of 0.91(6)-1.97(3) mu(B) on the U atoms

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

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

228 re ferromagnetic FeNi nanoislands have giant magnetic moments of 10[Formula: see text]-10[Formula: se

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

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

231 26 and 18 K, respectively, and with ordered magnetic moments of 3.61(6) and 2.3(1) muB per Mn cation

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

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

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

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

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

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

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

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

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

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

242 The magnetic moments of the particles are calculated based o

243 ional interlayer space and possess their own magnetic moments of ~0.52 mu(B) per quasi-atomic IAE, wh

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

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

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

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

248 r geometrical frustration of the ordering of magnetic moments or orbital occupancies at low temperatu

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

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

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

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

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

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

255 tilizing spin-orbit torque (SOT) to switch a magnetic moment provides a promising route for low-power

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

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

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

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

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

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

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

263 bands give the Bloch electrons large orbital magnetic moments so that a small current can generate a

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

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

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

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

268 d with a pulsed heat spot, which induces the magnetic moments surrounding the Skyrmion to rotate by t

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

270 ure-dependent flipping of the nearest W-site magnetic moments that are antiferromagnetically coupled

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

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

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

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

275 Due to conservation of their magnetic moments, the electrons form a beam collimated a

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

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

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

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

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

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

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

283 covers the trends in the observed band gaps, magnetic moments, type of magnetic and crystallographic

284 d as a result of thermal fluctuations of the magnetic moments under non-equilibrium thermal interacti

285 sion spectroscopy, we find appreciable local magnetic moments until 30 GPa to 40 GPa in the high-pres

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

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

288 Free magnetic moments usually manifest themselves in Curie la

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

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

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

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

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

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

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

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

297 Tb magnetic moments with an easy-axis single-ion magnetic a

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

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

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