ライフサイエンスコーパス: magnetic anisotropy

1 diate layer showed an improved perpendicular magnetic anisotropy.

2 l increase and decrease of the perpendicular magnetic anisotropy.

3 eld of the azido ligand and its influence on magnetic anisotropy.

4 veal the presence of an interfacial uniaxial magnetic anisotropy.

5 uced surface charge doping that modifies the magnetic anisotropy.

6 at exchange coupling can strongly modify the magnetic anisotropy.

7 in inversion, achieved through a large axial magnetic anisotropy.

8 reases with increasing ground-state spin and magnetic anisotropy.

9 d antiferromagnetic films with perpendicular magnetic anisotropy.

10 e magnetic exchange coupling and introducing magnetic anisotropy.

11 n configurations are defined by altering the magnetic anisotropy.

12 erature as well as a stable and controllable magnetic anisotropy.

13 en the Eu(II) ions and a dominant easy-plane magnetic anisotropy.

14 tic order at finite temperatures without any magnetic anisotropy.

15 sed chiral SMM featuring a strong single-ion magnetic anisotropy.

16 ing alternative chemical routes toward large magnetic anisotropy.

17 s and ferromagnets (FM) with a vast range of magnetic anisotropy.

18 -plane easy axis of magnetization, and large magnetic anisotropy.

19 ns contribute to this type of superstructure magnetic anisotropy.

20 anisotropy contributing to the perpendicular magnetic anisotropy.

21 ole moment that is directly connected to its magnetic anisotropy.

22 e of the thermal Hall effect and that of the magnetic anisotropy.

23 re fundamental knowledge about the impact of magnetic anisotropy.

24 nhanced magnetism, with robust perpendicular magnetic anisotropy.

25 -based trilayer structures with out-of-plane magnetic anisotropy.

26 ich correlates with the stress dependence of magnetic anisotropy.

27 oated ferromagnetic layer with perpendicular magnetic anisotropy.

28 oxide tunes the disorder, exchange field and magnetic anisotropy.

29 thermal fluctuations can be counteracted by magnetic anisotropy.

30 film due to thermal effects that modify its magnetic anisotropy.

31 ey information for the full understanding of magnetic anisotropy.

32 40B20/MgO/TiO2 structures with perpendicular magnetic anisotropy.

33 sistent with voltage-induced modification of magnetic anisotropy.

34 e the BaFe12O19 layer exhibits perpendicular magnetic anisotropy.

35 nduced Dzyaloshinskii-Moriya interaction and magnetic anisotropy.

36 ombine large hyperfine NMR shifts with large magnetic anisotropies.

37 ss high-spin ground states, but insufficient magnetic anisotropies.

38 Ni, CoFeB and Terfenol-D with perpendicular magnetic anisotropies.

39 O(4) (MGO) substrates with: 1) perpendicular magnetic anisotropy; 2) low magnetic damping and 3) the

40 Magnetic anisotropy allows magnets to maintain their dir

41 relaxation is faster than expected based on magnetic anisotropy alone.

42 We report an observation of uniaxial magnetic anisotropy along the [100] crystallographic dir

43 rplay between antiferromagnetic exchange and magnetic anisotropy amplifies this canting by several or

44 The magnetic anisotropies and orientation of the magnetic ax

45 to the total NMR shift in systems with large magnetic anisotropies and small hyperfine shifts, (7)Li

46 tric shows robust 90 electrical switching of magnetic anisotropy and a converse magnetoelectric coeff

47 tunnel barrier, where a large perpendicular magnetic anisotropy and a sizable tunnelling magnetoresi

48 ps of R provide an experimental probe of the magnetic anisotropy and aromaticity of the C18 ring thro

49 Large magnetic anisotropy and coercivity are key properties of

50 ns, elucidates the significance of four-fold magnetic anisotropy and Dzyaloshinskii-Moriya symmetry b

51 athway can be used to in situ manipulate the magnetic anisotropy and enable non-volatile FMR tuning i

52 Magnetic anisotropy and highly anisotropic electrical tr

53 Strain-induced changes in perpendicular magnetic anisotropy and interfacial Dzyaloshinskii-Moriy

54 in-induced changes in both the perpendicular magnetic anisotropy and interfacial Dzyaloshinskii-Moriy

55 t film, leading to nonvolatile modulation of magnetic anisotropy and magnetization reversal character

56 order to produce different strengths of the magnetic anisotropy and magnetostriction constants.

57 This allows the magnetic anisotropy and microwave resonant frequency to

58 , that a 90 degrees in-plane rotation of the magnetic anisotropy and propagation of magnetic domains

59 monstrate the role of hydrogen and oxygen on magnetic anisotropy and skyrmion deletion on other magne

60 ctions arising from the combination of large magnetic anisotropy and spin-delocalization from metal t

61 ntacts, which lead to a combination of large magnetic anisotropy and spin-delocalization.

62 effect of this substitution on the intrinsic magnetic anisotropy and the anisotropy fields that deter

63 Here we show an extreme, uniaxial magnetic anisotropy and the emergence of magnetic hyster

64 tic free energy that includes the effects of magnetic anisotropy and the SOI field.

65 intense terahertz pulses abruptly change the magnetic anisotropy and trigger a large-amplitude ballis

66 ron paramagnetic resonance, the influence of magnetic anisotropy and zero-field splitting on the para

67 interactions had a significant impact on the magnetic anisotropy and, consequently, the paramagnetic

68 ntil now, it has proved very hard to predict magnetic anisotropy, and as a consequence, most syntheti

69 Comparison of iron spin relaxivity, magnetic anisotropy, and magnetic susceptibilities argue

70 roton chemical shifts, deltaOrn delta-proton magnetic anisotropy, and NOE cross-peaks that establish

71 ng, we can mechanically manipulate the local magnetic anisotropy, and thereby write and erase functio

72 The effects of surface and bulk magnetic anisotropies are corroborated with those of the

73 Ferromagnetic films with perpendicular magnetic anisotropy are of interest in spintronics and s

74 agnetic moments with an easy-axis single-ion magnetic anisotropy are strongly coupled by the unpaired

75 hich have proven their capability to predict magnetic anisotropy, are described.

76 Numerical calculations identify magnetic anisotropy as the main Co-Fe NCs' feature to ge

77 lane compressive strain and shows a stronger magnetic anisotropy as well as cation site-exchange.

78 This review of the magnetic anisotropies associated with a pentagonal bipyr

79 The magnetic anisotropy associated with a pentagonal bipyram

80 We find that the magnetic anisotropy axes of U(DOTA)(H(2)O) (5f(2)) close

81 Experimental and theoretical magnetic anisotropy axes perfectly match and lie along t

82 The magnetic anisotropy axis of 14 low-symmetry monometallic

83 been synthesized to probe the origin of the magnetic anisotropy barrier in the one-dimensional coord

84 n the basis of these shapes, the size of the magnetic anisotropy barrier in the polyradical, originat

85 erations, with an emphasis on increasing the magnetic anisotropy barrier.

86 using this, we show that voltage controlled magnetic anisotropy based switching mediated by an inter

87 ncentration we achieved arbitrary control of magnetic anisotropy between out-of-plane and in-plane wi

88 pling and crystal field induce a significant magnetic anisotropy, breaking the rotation symmetry of q

89 Reaction of the high-magnetic anisotropy building unit [ReCl(4)(CN)(2)](2-) w

90 Sr(5)Co(4)O(12) exhibits strong magnetic anisotropy but no long-range magnetic order.

91 Lanthanide SMMs exhibit large magnetic anisotropies, but building high-spin ground sta

92 nto Hopfions by adapting their perpendicular magnetic anisotropy, but their experimental verification

93 he digital laser writing on selective areas, magnetic anisotropies can be encoded in the composite fi

94 ts shows that compounds with record-breaking magnetic anisotropy can also be achieved with coordinati

95 Perpendicular magnetic anisotropy can be achieved in thin ferromagneti

96 Morphological and magnetic anisotropy can be combined in colloidal assembl

97 ted Cr(2)Te(3) thin films with perpendicular magnetic anisotropy can be grown on c-plane sapphire sub

98 Molecules that exhibit a high degree of magnetic anisotropy can behave as individual nanomagnets

99 strain-induced changes in the perpendicular magnetic anisotropy can modify the coercive field and do

100 The magnetic anisotropy change as response to the gating vol

101 lation is attributed to the hydrogen-induced magnetic anisotropy change on ferromagnetic surfaces.

102 n resonances is largely accounted for by the magnetic anisotropy changes.

103 ultrathin magnetic films with perpendicular magnetic anisotropy combined with ferroelectric substrat

104 More than 100 compounds exhibit magnetic anisotropy comparable to or larger than leading

105 in para-tolanes, whereas in ortho-analogues magnetic anisotropy complicates the analysis making (13)

106 phase transitions into a state with striking magnetic anisotropy, consistent with the breaking of the

107 ively characterise saturation magnetization, magnetic anisotropy constants, and magnetic phase transi

108 tic antiferromagnets with high perpendicular magnetic anisotropy could prove useful for high performa

109 (2) ground state with significantly enhanced magnetic anisotropy (D = -0.33 cm(-1) and E = -0.018 cm(

110 zation measurements reveal a strong uniaxial magnetic anisotropy (D = -39.6 cm(-1)) acting on the S =

111 the quantitative determination of the axial magnetic anisotropy, Deltachi(ax) = -2.50 x 10(-8) m(3)/

112 these stable states minimizes the sum of the magnetic anisotropy, demagnetization, Dzyaloshinskii-Mor

113 pectroscopy, showing easy-axis or easy-plane magnetic anisotropy depending on the choice of Ln ion.

114 ferromagnetic films possessing perpendicular magnetic anisotropy derived from the crystal lattice can

115 is change is easily detected in the observed magnetic anisotropy despite thermal population of more t

116 s has been made in the electrical control of magnetic anisotropy, domain structure, spin polarization

117 According to solvent-induced isotope and magnetic anisotropy effects, the two duplex conformers a

118 A model including a strong magnetic anisotropy, elastic, Zeeman, Heisenberg exchang

119 In solution, a giant magnetic anisotropy enables the alignment of PNRs at sub

120 The clusters are marked by low magnetic anisotropy energy (MAE) of 2.72 meV and a large

121 ayer, which we use to toggle the interfacial magnetic anisotropy energy by >0.75 erg cm(-2) at just 2

122 nterfaces are analyzed through resolving the magnetic anisotropy energy by layer and orbital.

123 An interfacial perpendicular magnetic anisotropy energy density of 1.85 mJ/m(2) was o

124 es which are the primary contributors to the magnetic anisotropy energy in the low temperature struct

125 wards of 0.6 T combined with a perpendicular magnetic anisotropy energy of 0.95 MJ/m(3) and a low Gil

126 t existing methods rely on locally modifying magnetic anisotropy energy or saturation magnetization,

127 Thus far, the magnetic anisotropy energy per atom in single-molecule m

128 However, with decreasing particle size the magnetic anisotropy energy per particle responsible for

129 opy (VCMA) efficiency (change of interfacial magnetic anisotropy energy per unit electric field) lead

130 d by the exchange field resulting in a large magnetic anisotropy energy via the Dzyaloshinskii-Moriya

131 f two Tb excitations, which are split by the magnetic anisotropy energy, indicates an effective two-s

132 terfaces results in such an increased of the magnetic anisotropy energy, that onion-type nanoparticle

133 ism is attributed to the sensitive change of magnetic anisotropy energy.

134 Herein, we show that pairing the axial magnetic anisotropy enforced by tetramethylcyclopentadie

135 e slower relaxation derives from the greater magnetic anisotropy enforced within the strongly donatin

136 ible functionalization that will boost their magnetic anisotropy even further.

137 cationic nickel cluster also possesses large magnetic anisotropy exemplified by a large, positive axi

138 e-earth iron garnet films with perpendicular magnetic anisotropy exhibit homochiral Neel domain walls

139 The ferroelectric switching of magnetic anisotropy exhibits extensive applications in e

140 ) displays paramagnetic property with strong magnetic anisotropy facilitated by large spin-orbit coup

141 otropy field (H K) and surface perpendicular magnetic anisotropy field (H KS) in the same Pt/YIG syst

142 An extrapolated, magnetic anisotropy field of 220 T and a coercivity fiel

143 ilms on amorphous substrates, with very high magnetic anisotropy fields exceeding 7 T, making them te

144 We realized the maximum magnetic anisotropy for a 3d transition metal atom by co

145 of antiferromagnetic materials with biaxial magnetic anisotropy for electrical manipulation.

146 ates the direction of the arrangement of its magnetic anisotropy for the purposes of generating contr

147 hin-film magnetic samples with perpendicular magnetic anisotropy, for which the Kerr rotation is seco

148 t spin-torque oscillators with perpendicular magnetic anisotropy free layers.

149 the metal centers appears to increase axial magnetic anisotropy, giving rise to larger magnetic rela

150 rromagnetic domain wall in the presence of a magnetic anisotropy gradient mimics a biological neuron

151 h weak Dzyaloshinskii-Moriya interaction and magnetic anisotropy gradient.

152 sfers to the CoFeB thin film and changes its magnetic anisotropy H(k).

153 We argue that strong magnetic anisotropy has a key role in this process, inje

154 Bleaney's long-standing theory of magnetic anisotropy has been employed with some success

155 control of ferromagnetism, magnetization and magnetic anisotropy has been explored in various magneti

156 magnetic field in GaMnAs film with in-plane magnetic anisotropy has been investigated by planar Hall

157 ferromagnetic insulators with perpendicular magnetic anisotropy have been identified as critical to

158 ar chemical design strategies for maximising magnetic anisotropy have come, but have also highlighted

159 Magnetic thin films with perpendicular magnetic anisotropy have localized excitations that corr

160 vs. low frequency conditions with respect to magnetic anisotropy, (ii) EPR spectra of non-integer (Kr

161 1), respectively, a consequence of the large magnetic anisotropies imparted by these ions.

162 elected because its characteristically large magnetic anisotropy imparts significant dipolar shifts w

163 gnetic resonance spectroscopy to measure the magnetic anisotropies in different strains of Magnetospr

164 This work focuses on the nature of magnetic anisotropy in 2.5-16 micron thick films of nick

165 is achieved with the voltage-control of the magnetic anisotropy in a nanosized region where the symm

166 he latter of which were used to quantify the magnetic anisotropy in both the ferric high-spin aquo an

167 position, bonding, electronic structure, and magnetic anisotropy in each case study.

168 ling macroscopic properties such as expected magnetic anisotropy in elongated shaped macromolecules c

169 ionic cyclic ligands, to ultimately maximize magnetic anisotropy in f-block-based SMMs.

170 rough interfacial strain-induced rotation of magnetic anisotropy in magnetostrictive/piezoelectric mu

171 entum and spin-orbit coupling from Bi impart magnetic anisotropy in MnBi(2).

172 ty and approaches to create "patterned" high magnetic anisotropy in nanoparticle superstructures/asse

173 he use of PBP complexes to impart controlled magnetic anisotropy in polynuclear species such as SMMs

174 which has been widely employed to manipulate magnetic anisotropy in spintronic devices and artificial

175 gand vibrations being of equal importance to magnetic anisotropy in the design of high-temperature SM

176 eraction, open pathways to active control of magnetic anisotropy in the emerging dissipation-free sup

177 n oriented single crystals, and a very large magnetic anisotropy in the magnetic susceptibility was o

178 Maintaining strong magnetic anisotropy in the presence of collective spin i

179 pounds of Co(II) in particular exhibit large magnetic anisotropy in the presence of low-coordination

180 or magnetic fields to visualize directly the magnetic anisotropy in the uniaxial ferromagnet CeRu2Ga2

181 are based on nanomagnets with perpendicular magnetic anisotropy, initialized to their hard axes by t

182 mplex patterns with continuous variations in magnetic anisotropy, interlayer exchange coupling, and f

183 Magnetic anisotropy is a crucial characteristic for enha

184 Magnetic anisotropy is also affected by the electric fie

185 The magnetic anisotropy is axial and oriented by the axial F

186 ar u(3)-oxo-bridged Mn(III)-based SMM, whose magnetic anisotropy is closely related to the Jahn-Telle

187 Designing systems with large magnetic anisotropy is critical to realize nanoscopic ma

188 The massive magnetic anisotropy is due to bis-trans-disposed tert-bu

189 Furthermore, we show that the magnetic anisotropy is equally well predicted in a selec

190 Magnetic anisotropy is essential for many applications o

191 garnet (YIG) system and its association with magnetic anisotropy is essential towards optimization of

192 blished understanding that strong Ising-type magnetic anisotropy is essential.

193 r [Formula: see text] crystal structure, the magnetic anisotropy is perpendicular to the [100] plane,

194 Moreover, the electrical switching of magnetic anisotropy is repeatable and non-volatile.

195 Magnetic anisotropy is the property that confers to the

196 The perpendicular magnetic anisotropy K(eff), magnetization reversal, and

197 (3)O(4) chain arrays possess a high uniaxial magnetic anisotropy (K(eff) ~ 2.9x10(5 )J/m3) and signif

198 opatterns by crafting, at the nanoscale, the magnetic anisotropy landscape of a ferromagnetic layer e

199 A strong out-of-plane magnetic anisotropy, linear magnetoresistance, and robus

200 Magnetic anisotropy (MA) is one of the most important ma

201 of-plane piezoelectricity and strain-tunable magnetic anisotropy make the 1T'-CrCoS(4) monolayer a st

202 etic-dipole-induced aggregation, while their magnetic anisotropy makes them responsive to an external

203 We explain these effects with a detailed magnetic anisotropy model and first-principles calculati

204 drogenation drives pronounced changes in its magnetic anisotropy, Neel vector orientation and canted

205 aracterize the intrinsic exchange fields and magnetic anisotropies of the AFM.

206 cal quantity depends on the magnitude of the magnetic anisotropy of a complex and the size of its spi

207 tic skyrmion by modulating the perpendicular magnetic anisotropy of a nanomagnet with an electric fie

208 cantilever torque magnetometry to probe the magnetic anisotropy of a single crystal of U(DOTA)(H(2)O

209 rovides a powerful route to characterize the magnetic anisotropy of actinide complexes and offers a v

210 cation-specific coordination environment and magnetic anisotropy of Co(II), with axial zero-field spl

211 el systems with which to harness the maximum magnetic anisotropy of Dy(III) ions.

212 ctrostatic method, capable of predicting the magnetic anisotropy of dysprosium(III) complexes, even i

213 te disorder as well as variations of the net magnetic anisotropy of FM nuclei.

214 enable a better estimation of the effective magnetic anisotropy of highly crystalline magnetite nano

215 he way toward a reliable predictivity of the magnetic anisotropy of lanthanide complexes with a conse

216 La0.08Zr0.52Ti0.48O3 (PLZT) films, where the magnetic anisotropy of NiFe can be electrically modified

217 The shape of the magnetic anisotropy of some couples of ions differing by

218 The results show how synergizing the strong magnetic anisotropy of terbium(III) with the effective e

219 le for the strong positive axial and rhombic magnetic anisotropy of the high-spin Co(II) ion (D = +98

220 and 1-Er arise from differences in the local magnetic anisotropy of the lanthanide centers.

221 rameter D (2.9 cm(-1)), which quantifies the magnetic anisotropy of the Mn(III) centers.

222 lar beam epitaxy and introduce perpendicular magnetic anisotropy of the octupole using an epitaxial i

223 In TbMn(6)Sn(6), the uniaxial magnetic anisotropy of the Tb(3+) ion is effective at ge

224 This changes the magnetic anisotropy of the Yb(III) ground state from eas

225 de ligands leads to a marked increase in the magnetic anisotropy of trans-[ReF(4) (CN)(2) ](2-) as co

226 ed by novel main group ligands in addressing magnetic anisotropy of transition metal and f-element co

227 ferromagnetic insulators with perpendicular magnetic anisotropy, opening new possibilities for spin

228 d pulse can be used to 'set' and 'reset' the magnetic anisotropy orientation and resistive state in t

229 ormula: see text] crystal structure, we find magnetic anisotropy perpendicular to the film plane.

230 scillator, with the energy of the easy-plane magnetic anisotropy playing the role of the Josephson en

231 agnetic layered structure with perpendicular magnetic anisotropy (PMA) and one piezoelectric substrat

232 .21 [Formula: see text]/Cr and perpendicular magnetic anisotropy (PMA) constant (K(u)) of 4.89 x 10(5

233 Perpendicular magnetic anisotropy (PMA) ferromagnetic CoFeB with dual

234 Controlling the perpendicular magnetic anisotropy (PMA) in thin films has received con

235 on in magnetic thin films with perpendicular magnetic anisotropy (PMA) requires the domain walls to h

236 excitations in a [Co/Pt]-based perpendicular magnetic anisotropy (PMA) synthetic antiferromagnet (p-S

237 field-free electric control of perpendicular magnetic anisotropy (PMA) vdW magnets at room temperatur

238 io as well as a large value of perpendicular magnetic anisotropy (PMA).

239 cularity on an underlayer with perpendicular magnetic anisotropy (PMA).

240 rove its thermal stability and perpendicular magnetic anisotropy (PMA).

241 icating the presence of a weak perpendicular magnetic anisotropy, PMA.

242 cess are lacking for MTJs with perpendicular magnetic anisotropy (pMTJs) required for scalable applic

243 tion between the exchange interaction and 4f magnetic anisotropy present in the system.

244 Magnetic anisotropy removes this restriction, however, a

245 and CrCl(3), with perpendicular and in-plane magnetic anisotropy, respectively.

246 his article, we report our discovery of high magnetic anisotropy resulted from Fe(3)O(4) nanoparticle

247 netic domain configuration due to an induced magnetic anisotropy resulting from the inverse magnetost

248 Significant magnetic anisotropy results from this orbital degeneracy

249 relaxation and a preliminary estimate of the magnetic anisotropy, reveal a chi that is axially anisot

250 conversion by correcting for the effects of magnetic anisotropy reveals a very substantial change in

251 ly, demonstrating that the strength of axial magnetic anisotropy scales with increasing ligand field

252 Magnetic anisotropy slows down magnetic relaxation and p

253 In materials with the gradient of magnetic anisotropy, spin-orbit-torque-induced magnetiza

254 oupling effects lead to non-negligible axial magnetic anisotropy, splitting the ground state multiple

255 polar interactions and the weak out-of-plane magnetic anisotropy stabilising a vortex core within a r

256 nteraction, spin-orbit coupling, and surface magnetic anisotropy stabilizes different types of spin a

257 The magnetic anisotropy symmetry reversibly switches from a

258 endipitous processes in the search for large magnetic anisotropy systems.

259 tio calculations allowed us to determine the magnetic anisotropy tensor of the uranium center.

260 identify a new trend: the orientation of the magnetic anisotropy tensors of derivatives differing by

261 lbert-Slonczewski equation in the absence of magnetic anisotropy terms is described by a Mobius trans

262 the switching of magnets with perpendicular magnetic anisotropy that are demanded by the high-densit

263 quantum limit, signalling a reversal of the magnetic anisotropy that can be directly attributed to t

264 ion due to lithographic patterning induces a magnetic anisotropy that competes with the magnetocrysta

265 for the first time the exceptional uniaxial magnetic anisotropy that even the six equatorial donor a

266 se of the Tb and Dy variants, a strong axial magnetic anisotropy that gives rise to a large magnetic

267 th competing in-plane and out-of-plane (OOP) magnetic anisotropies, the SOC mediated interaction betw

268 Due to a weak uniaxial magnetic anisotropy, the domains are separated primarily

269 rder to optimize this system with respect to magnetic anisotropy, the triplesalophen ligand system ha

270 r is also the first molecule with easy-plane magnetic anisotropy to exhibit zero-field slow magnetic

271 e guests report their positions by imparting magnetic anisotropy to the capsule components.

272 s, the room temperature TC, and the in-plane magnetic anisotropy together in a single layer VX2, this

273 a magnetic half-plane and show how intrinsic magnetic anisotropies trigger bistable spin textures tha

274 A reversible change of magnetic anisotropy up to 219 Oe is achieved with a low

275 d, non-volatile manipulation of out-of-plane magnetic anisotropy up to 40 Oe is demonstrated and conf

276 utorial is dedicated to the investigation of magnetic anisotropy using both electron paramagnetic res

277 all motion in materials with the gradient of magnetic anisotropy using the CCM remains lack of invest

278 as been demonstrated that voltage-controlled magnetic anisotropy (VCMA) based writing is highly energ

279 The voltage-controlled magnetic anisotropy (VCMA) effect, which manifests itsel

280 MeRAM devices is the low voltage-controlled magnetic anisotropy (VCMA) efficiency (change of interfa

281 uctures which exhibit low voltage-controlled magnetic anisotropy (VCMA) efficiency.

282 titative determination of voltage-controlled magnetic anisotropy (VCMA) in Au/[DEME](+) [TFSI](-) /Co

283 recovery in ferrimagnets with perpendicular magnetic anisotropy via nonlinear magnon processes.

284 totype MRI contrast agents showed that their magnetic anisotropy was highly sensitive to changes in m

285 Remarkably, a substantial increase in magnetic anisotropy was observed, as manifested by the i

286 The molecule's spin states and magnetic anisotropy were manipulated in the absence of a

287 nel junctions with interfacial perpendicular magnetic anisotropy, where the coercivity, the magnetic

288 dentify a novel magnetic phase with enhanced magnetic anisotropy which is a candidate for rare-earth

289 ntiferromagnetic spin correlations and local magnetic anisotropy, which allows it to be indirectly ob

290 The barriers exhibit perpendicular magnetic anisotropy, which has the main advantage for po

291 gnetic frustration has a clear in-plane (ab) magnetic anisotropy, which is maintained up to temperatu

292 extreme total ionizing dose on perpendicular magnetic anisotropy, which plays a crucial role on therm

293 are very promising to enhance the effective magnetic anisotropy while preserving sizes below 20 nm.

294 a single crystal of 1 shows a giant uniaxial magnetic anisotropy with an experimental D(expt) value (

295 Combining Ising-type magnetic anisotropy with collinear magnetic interactions

296 if a nanoparticle assembly can possess high magnetic anisotropy with low anisotropic materials.

297 Significant magnetic anisotropy with the easy axis along the [101] d

298 We find that 1-Dy has large magnetic anisotropy, with U(eff) = 2191(33) K; this is c

299 evices in which piezoelectrically controlled magnetic anisotropy yields up to 500% mobility variation