ライフサイエンスコーパス: magnetization

1 re iridate Ho2Ir2O7, leading to a fragmented magnetization.

2 modify the sense of rotation of the average magnetization.

3 is observed which is antiparallel to the Fe magnetization.

4 ers have been used to efficiently manipulate magnetization.

5 needed to capture the extent of the induced magnetization.

6 y a detailed analysis of the field-dependent magnetization.

7 individual atoms and the resulting zero net magnetization.

8 estration that results in increased cellular magnetization.

9 irect measurements of the synthetic hemozoin magnetization.

10 ficant impact on the improvement of remanent magnetization.

11 aviours and a semi-reversible control of the magnetization.

12 allow electrical switching of perpendicular magnetization.

13 rp onset and the thickness dependence of the magnetization.

14 ficients and a large electric-field-reversed magnetization.

15 the spin polarization is rotating about the magnetization.

16 > 1.0 x 10(7) erg/cc), and large saturation magnetization (4piMs > 2.4 T).

17 nanostructures with high TC (700 K) and high magnetization (5.9 emu/g).

18 the process of selectively manipulating the magnetization alignment in magnetic layers in the Fe/GaA

19 By spin-locking the (1)H magnetization along the magic angle, the (1)H spin diffu

20 Dynamic optical control over both magnetization and chemical potential of a TI may be usef

21 sult in approximately 100% modulation of the magnetization and drives domain wall motion over approxi

22 en ferroelectrics featuring both spontaneous magnetization and electric polarization are still rare.

23 iral magnets with a simultaneous reversal of magnetization and electric polarization that is still li

24 pirals leads to the simultaneous reversal of magnetization and electric polarization.

25 Direct magnetization and electrical resistivity measurements de

26 excitation of coherent auto-oscillations of magnetization and for generation of tunable microwave si

27 itation of auto-oscillations of the Y3Fe5O12 magnetization and generation of coherent microwave radia

28 tandard MagLev (i.e., where the direction of magnetization and gravitational force are parallel) cann

29 rotated state (i.e., where the direction of magnetization and gravitational force are perpendicular)

30 r, electric-field control of ferromagnetism, magnetization and magnetic anisotropy has been explored

31 We show, through a combination of angular magnetization and magneto-optical domain imaging measure

32 i multilayered films with tunable saturation magnetization and perpendicular anisotropy grown directl

33 Meanwhile the remanent magnetization and polarization show opposite variation t

34 The detection in this instance of magnetization and scattering that are both local to the

35 nsformation temperatures, strain, saturation magnetization and strength) determine their prospects fo

36 a powerful way to build correlation between magnetization and T2 relaxivity of MNPs, especially magn

37 sample with x = 0.3 has the largest remanent magnetization and the smallest polarization.

38 gnetic structures, with arbitrarily oriented magnetization and tunable unidirectional anisotropy, are

39 smitted light was modified by modulating the magnetization, and a Q-switched pulse output with a puls

40 aterial to bear no crystalline dependence on magnetization, and application of a magnetic field cause

41 eutron diffraction, magnetic susceptibility, magnetization, and electrical resistivity are studied fo

42 Thermal expansion, electrical resistivity, magnetization, and specific heat measurements were perfo

43 We demonstrate that the polarity and magnetization are coupled in this system with a measured

44 Materials with high volume magnetization are perpetually needed for the generation

45 Oxygen migration and Co magnetization are quantitatively mapped with polarized n

46 ratio of anhysteretic to isothermal remanent magnetization, are insensitive to changing vegetation.

47 Voltage-induced switching of magnetization, as opposed to current-driven spin transfe

48 An abrupt increase of surface magnetization at around the same temperature suggests th

49 The MP are registered by their non-linear magnetization at combinatorial frequencies by a portable

50 angle to the director, yielding macroscopic magnetization at no external fields.

51 the Dy(III) complex enables a large remnant magnetization at temperatures up to 3.0 K in the magneti

52 Results show clear dual magnetization behavior with threefold enhancement betwee

53 ll as linear, isotropic, and hysteresis free magnetization behavior.

54 gnetic anisotropy, spin-orbit-torque-induced magnetization behaviour has attracted attention because

55 are known to play a significant role in the magnetization behaviour of thin-film ferromagnets by thr

56 Most of the magnetization behaviours microscopically originate from

57 We show that the switching of magnetization between the easy axes in a GaMnAs film dep

58 tric (ME) effect, the phenomenon of inducing magnetization by application of an electric field or vic

59 t and voltage-induced magnetization generate magnetization by applied electric fields, but only in sp

60 The manipulation of magnetization by spin-current occurs through the spin-tr

61 rate of incoherent quantum tunneling of the magnetization by two orders of magnitude.

62 ards zero in the applied magnetic field, the magnetization can reliably freeze about a higher anisotr

63 articles with a strong temperature-dependent magnetization, can be used to produce temperature-depend

64 Remarkably, giant controllable magnetization changes (measured to be as high has ~25%)

65 These magnetization changes are the largest seen to date to be

66 urrent simply by use of a FM/NM bilayer with magnetization collinear to the charge current.

67 ds to torques that can be used to switch the magnetization completely in out-of-plane magnetized ferr

68 It can be generalized to different magnetization configurations and yield multiple spin wav

69 netic simulations, and identify two possible magnetization configurations: a circulating magnetizatio

70 Remarkably, our magnetization curves reveal a crossover field [Formula:

71 = -1.29 cm(-)(1)) extracted from the reduced magnetization data.

72 The spin Seebeck effect also produces magnetization-dependent transverse electric fields.

73 conversion is shown to be spin-helicity- and magnetization-dependent.

74 The direction of the magnetization depends on the handedness of the adsorbed

75 and the current direction, regardless of the magnetization direction in the domain wall.

76 inistic switching is highly dependent on the magnetization direction in the domain wall.

77 /Ni junction can be switched by flipping the magnetization direction of the ferromagnetic electrode.

78 rate that manipulation of the AFM Neel-order magnetization direction via purely E-field means can pav

79 tions can be controlled as a function of the magnetization direction.

80 Two groups of characteristic remanent magnetization directions were defined with nearly antipo

81 The in-situ characterization of magnetization during the Li-ion intercalation/deintercal

82 evel coupled simulation framework, including magnetization dynamics and electron transport model, has

83 Low-loss magnetization dynamics and strong magnetoelastic couplin

84 f different coordination environments on the magnetization dynamics and the quantum coherence of two

85 serve as a test bed for studies of nonlinear magnetization dynamics at the nanometer length scale.

86 or could allow efficient manipulation of the magnetization dynamics by an electric field, providing a

87 we analytically and micromagnetically study magnetization dynamics excited in an SHO with oblique ma

88 spin currents can be used to excite coherent magnetization dynamics in magnetic nanostructures.

89 The magnetization dynamics in such cases shows preference fo

90 For this we have studied the magnetization dynamics of a ferromagnetic cobalt/palladi

91 Here we report the investigation of the magnetization dynamics of a vanadyl complex with diethyl

92 use time-resolved-vectorial measurements of magnetization dynamics of thin layers of Fe, Ni and Co d

93 We also determine the regime of magnetization dynamics that leads to the greatest perfor

94 e film plane, and is enabled by manipulating magnetization dynamics with fast, local piezostrains (ri

95 enological parameter that dictates real-time magnetization dynamics.

96 , TB , is 14 K, defined by zero-field-cooled magnetization experiments, and is the largest for any mo

97 3 single crystal in which the induced Dy(3+) magnetization (FDy) has a natural tendency to be antipar

98 udy in the Ba2-x Sr x Mg2Fe12O22 family with magnetization, ferroelectricity and neutron diffraction

99 ency to be antiparallel to Fe(3+) sublattice magnetization (FFe) within a large temperature window.

100 -3D regions with a single orientation of the magnetization field.

101 ormation, and highlighting the importance of magnetization fluctuations on carrier spin dynamics in n

102 dentifying a 25 nm central region of uniform magnetization followed by a larger region characterized

103 0) content from 5.9% to 55.6%, and increases magnetization from 4.7 to 65.5 emu/g.

104 minority electron spins alters the interface magnetization from C-type to A-type AFM state.

105 f sufficient polarization from h-LFO and net magnetization from o-LFO.

106 magneto-electric effect and voltage-induced magnetization generate magnetization by applied electric

107 obable cause for the ferromagnetism and weak magnetization hysteresis in Fe-doped hexagonal ZnO and Z

108 rly to the in-plane projection of the static magnetization; (ii) skyrmions generation by pure spin-cu

109 CrEr6 } analogues display slow relaxation of magnetization in a 3000 Oe static magnetic field.

110 ropagate, but current-induced control of the magnetization in a MI has so far remained elusive.

111 roduces a torque on and thereby switches the magnetization in a neighbouring ferromagnetic metal film

112 ace via surface receptors, followed by their magnetization in any desired direction.

113 s as dominating mechanisms for the large net magnetization in BFO.

114 (SOT) has been widely used to manipulate the magnetization in metallic ferromagnets.

115 ayers provides an opportunity to control the magnetization in one layer (in the presence case in GaMn

116 ontrol the up and down states of the remnant magnetization in the BaFe12O19 film when the film is mag

117 dians per square meter), we infer negligible magnetization in the circum-burst plasma and constrain t

118 We show here that by forcing the magnetization in the ferromagnet to precess at resonance

119 ng to our ability to selectively control the magnetization in the GaMnAs layer, we are able to manipu

120 ence case in GaMnAs) by a current, while the magnetization in the other layer (i.e., Fe) remains fixe

121 ce observed for two opposite currents as the magnetization in the structure switches directions.

122 ted the pure electrical generation of valley magnetization in this material, and its direct imaging b

123 omes entangled with kinetic instabilities as magnetization increases.

124 a function of current direction and detector magnetization indicate that hole spin-momentum locking f

125 All-optical switching (AOS) of magnetization induced by ultrafast laser pulses is funda

126 tly probe both the in-plane and out-of-plane magnetizations induced at the interface between the ferr

127 It shows that magnetization-induced electromagnetic spin-orbit couplin

128 we observe that vortex clusters appear near magnetization inhomogeneities in the ferromagnet, called

129 We decompose the torques that drive the magnetization into field-like and spin-transfer componen

130 es up to around 200 nanometres, in which the magnetization is accessible with current transmission im

131 The observed out-of-plane magnetization is independent of in-plane magnetic field,

132 ane (in-plane) MA in the FM (AFM) phase, its magnetization is more rigid to external E-field.

133 etween BiFeO3 antiferromagnetic order and Co magnetization is observed, with 90 degrees in-plane Co

134 The observed magnetization is significantly greater than both doped a

135 erromagnetic materials, the smoothly varying magnetization leads to the formation of fundamental patt

136 ential at the junction and allow probing the magnetization locally.

137 te fields, MDM is high throughout the entire magnetization loop.

138 Temperature-dependent magnetization M measurements reveal a ferromagnetic-like

139 Saturation magnetization (M S ) and coercivity (H C ) increase from

140 reover, for the first time, it is shown that magnetization measurements can be used to investigate se

141 omprehensive phase diagram based on detailed magnetization measurements of a high quality single crys

142 Temperature-dependent DC magnetization measurements of Yb14-xPrxMnSb11 (0.44 </=

143 Here we report on magnetization measurements on the dimerized quantum magn

144 Our bulk magnetization measurements reveal that most densely popu

145 s characterized by Mssbauer spectroscopy and magnetization measurements, showing that SAMNs resulted

146 ar the critical composition through detailed magnetization measurements.

147 s, first-principles calculations, as well as magnetization measurements.

148 These results present a simple low-power magnetization mechanism when operating at ambient condit

149 Ag@PDA nanocomposite shows a high saturation magnetization (Ms) of 48.9 emu/g, which allows it to be

150 u on the surface leads to an increase in the magnetization near the surface.

151 An enhanced magnetization of 1.83 +/- 0.16 muB /Fe in BFO layers is

152 of low-dissipation protocols that invert the magnetization of a 2D Ising model and explore how the di

153 we report on the relaxation dynamics of the magnetization of artificial assemblies of mesoscopic spi

154 ibutes the temperature dependence of the net magnetization of BFO to strong orbital hybridization bet

155 Moreover, the splitting follows the magnetization of EuS, a hallmark of the MEF.

156 ort properties is further discussed, and the magnetization of five alloys containing three or more el

157 n the barrier, and a large proximity-induced magnetization of GdOx, both the magnitude and the sign o

158 e PMN-PT without a magnetic field, the local magnetization of NiFe can be repetitively reversed throu

159 Here we selectively probe the interface magnetization of SrTiO3/La0.5Ca0.5MnO3/La0.7Sr0.3MnO3 he

160 The staggered magnetization of the 5 nm thick CuMnAs layer is rotatabl

161 gnetic states, i.e. skyrmion states with the magnetization of the core pointing down/up and periphery

162 he circum-burst plasma and constrain the net magnetization of the cosmic web along this sightline to

163 The magnetization of the device is accompanied with large av

164 treatment, both the coercivity and remanent magnetization of the Dy-Cu press injected magnets increa

165 operty of small magnetic particles where the magnetization of the particle flips randomly in time, du

166 the direction perpendicular to the in-plane magnetization of yttrium iron garnet.

167 ials seem to crucially depend on whether the magnetizations of the R and Fe ions' weak ferromagnetic

168 s coupling can be utilized to manipulate the magnetization (or polarization) with an electric (or mag

169 bulk acoustic waves in ME antennas stimulate magnetization oscillations of the ferromagnetic thin fil

170 ed, and a reversible variation of saturation magnetization over 10% was observed in both these materi

171 oscopic patterns, specified by a sequence of magnetization plateaus.

172 nting up/down, and ferromagnetic states with magnetization pointing up/down, by sequential increase a

173 Magnetization prepared rapid acquisition gradient-echo T

174 that the collective rotation of the average magnetization proceeds in a unique sense during thermal

175 ls, which incorporate precessionally limited magnetization processes, are needed to understand domain

176 ross-correlating speckle patterns throughout magnetization processes.

177 Its zero-field magnetization produces distinctive magnetic self-interac

178 that can automatically generate the required magnetization profile and actuating fields for soft matt

179 human intuition to approximate the required magnetization profile and actuating magnetic fields for

180 provides the details of the composition and magnetization profiles and shows that an accumulation of

181 The static and dynamic magnetization properties are characterized by a hysteres

182 pproximately 69 K and displayed a saturation magnetization reaching 1.09 emu/g.

183 anoparticles that have significantly reduced magnetization, relative to the bulk.

184 In contrast, the bulk magnetization remains unchanged.

185 nons, and achieve coherent dynamic states of magnetization reminiscent of the Bose-Einstein condensat

186 The magnetization represents the magnetic quantum values of

187 Does the excitation of ultrafast magnetization require direct interaction between the pho

188 tions of proton-coupled redox potentials and magnetizations reveal that the Ni-only system features o

189 d the IDMI from the heavy metal layer on the magnetization reversal and provide a route to controllin

190 Using phase field simulations we interpret magnetization reversal as a synergistic effect of the me

191 across this interface lead to deterministic magnetization reversal at low current densities, paving

192 e state in the film, as well as to lower the magnetization reversal barrier, showing a promising rout

193 Magnetization reversal characteristics captured by angul

194 latile modulation of magnetic anisotropy and magnetization reversal characteristics.

195 Voltage controlled 180 degrees magnetization reversal has been achieved in BiFeO3-based

196 reversal showing that the energy barrier for magnetization reversal is drastically lowered.

197 estricted to be two-fold, the one-step sharp magnetization reversal is realized and giant magnetoelec

198 (SMM) behavior, with an effective barrier to magnetization reversal of up to 268 cm(-1).

199 Additionally, we find that unlike the magnetization reversal process for periodic artificial s

200 Purely voltage-driven, repeatable magnetization reversal provides a tantalizing potential

201 hat the measurement of magnetic field-driven magnetization reversal, mediated by domain wall (DW) mot

202 nd its consequences on the angular dependent magnetization reversal.

203 electrons per cm(2) are sufficient to induce magnetization reversal.

204 ce plateaus are observed at the locations of magnetization reversals, giving a distinct signature of

205 Using a magnetization-sensitive scanning X-ray transmission micr

206 nt a simple analytical model to estimate the magnetization (sigma s) and intrinsic coercivity (H ci)

207 estigate magnetoresistance effects and track magnetization spatial distribution in L-shaped Py nanost

208 rents provide the possibility to control the magnetization state of conducting and insulating magneti

209 These include modifying the local magnetization state via an interfacial Dzyaloshinskii-Mo

210 By exploiting the magnetization states of nanomagnetic disks as state repr

211 E-SHEATH method, sustaining both singlet and magnetization states, thus offering a path to long-lived

212 magnetization configurations: a circulating magnetization structure and a twisted state that appears

213 In thicker samples, however, in which the magnetization structure varies throughout the thickness

214 Magnetization studies revealed nearly ideal paramagnetic

215 und spin state (ST =16) that is confirmed by magnetization studies up to 20 Tesla.

216 excites a non-uniform in time precession of magnetizations sublattices in the AFM, due to the presen

217 rt of a thicker BFO layer has a much smaller magnetization, suggesting it still keeps the small cante

218 er, hystereses are clearly observed when the magnetization switches direction in the GaMnAs layer, bu

219 torque coexist, hence jointly affecting the magnetization switching behavior.

220 new path towards achieving energy-efficient magnetization switching by controlling interlayer coupli

221 Furthermore, we demonstrate the magnetization switching by scanning gate voltage with co

222 Current induced magnetization switching by spin-orbit torques offers an

223 Here, we study perpendicular magnetization switching driven by the combination of the

224 the thin film, and realize the deterministic magnetization switching in a hybrid ferromagnetic/ferroe

225 achieve voltage-driven in-plane 180 degrees magnetization switching in a strain-mediated multiferroi

226 The electrical control of the magnetization switching in ferromagnets is highly desire

227 like torques and damping-like torques to the magnetization switching induced by the electrical curren

228 Local magnetization switching is achieved by adsorbing a chira

229 nts, thereby offering a promising low energy magnetization switching mechanism.

230 Here we demonstrate magnetization switching of ferromagnetic thin layers tha

231 Voltage-driven 180 degrees magnetization switching provides a low-power alternative

232 ge of planar Hall voltage is associated with magnetization switching through 90 degrees in the plane

233 es a low-power alternative to current-driven magnetization switching widely used in spintronic device

234 AFM Fe-terminated phase undergoes an E-field magnetization switching with large VCMA efficiency and a

235 ntronic applications such as current induced magnetization switching without any spin-polarized leads

236 ross the interface, and the mediation of the magnetization switching, with the flow of current throug

237 aller than that dissipated by current-driven magnetization switching.

238 in the spin structure factor and a staggered magnetization that is close to the ground-state value.

239 rect exchange coupling via proximity-induced magnetization through non-magnetic layers is typically i

240 l coupling between electric polarization and magnetization, through the exchange of elastic, electric

241 ounds may exhibit intramolecular spontaneous magnetization, thus offering promising prospects for sto

242 with spatial modulations of the density and magnetization, thus overcoming usual requirement for a s

243 the signal dependence on the applied field, magnetization time, and magnetic core size.

244 cts the pair condensate, we have used torque magnetization to 45 T and thermal conductivity [Formula:

245 ic particles, the current can also cause the magnetization to flip randomly in time, even at low temp

246 Magnetization transfer (MT) is a neuroimaging technique

247 Purpose To determine whether magnetization transfer (MT) magnetic resonance (MR) imag

248 Here, we used quantitative magnetization transfer (qMT) imaging, an advanced micros

249 proton transfer and semisolid macromolecular magnetization transfer effects, the IDEAL fitting reveal

250 etrics of diffusion tensor imaging (DTI) and magnetization transfer imaging (MTI) can detect diffuse

251 can affect both diffusion tensor imaging and magnetization transfer imaging in a non-specific manner.

252 Purpose To test the utility of magnetization transfer imaging in detecting and monitori

253 We applied magnetization transfer imaging to examine the impact of

254 Conclusion Magnetization transfer imaging was used successfully to

255 hanges, such as diffusion tensor imaging and magnetization transfer imaging, show some correlation wi

256 etion) decreased diffusivities and increased magnetization transfer in cornea, whereas glyceraldehyde

257 ornea, whereas glyceraldehyde also increased magnetization transfer in sclera.

258 se course) underwent T1- and T2-weighted and magnetization transfer magnetic resonance imaging at bas

259 e forward reaction rate constant using (31)P magnetization transfer magnetic resonance spectroscopy a

260 fusion tensor MRI without apparent change in magnetization transfer MRI, suggestive of straightening

261 es, longer coherence lifetimes, and improved magnetization transfer offset the reduced sample size at

262 The magnetization transfer ratio (MTR) at 3.5ppm demonstrate

263 ys after implantation, with the asymmetrical magnetization transfer ratio (MTRasym) calculated from i

264 acromolecular proton fraction outperforms MT magnetization transfer ratio and R1 in detection of MS m

265 ion volume and normal-appearing white matter magnetization transfer ratio for all of the patients com

266 The magnetization transfer ratio gradient also correlated wi

267 An abnormal periventricular magnetization transfer ratio gradient occurs early in mu

268 definite multiple sclerosis within 2 years (magnetization transfer ratio gradient odds ratio 61.708,

269 The magnetization transfer ratio gradient over 1-5 mm differ

270 multivariate binary logistic regression the magnetization transfer ratio gradient was independently

271 The magnetization transfer ratio gradient was not significan

272 At 5 years, lesional measures overtook magnetization transfer ratio gradients as significant pr

273 In normal-appearing white matter, magnetization transfer ratio gradients were measured 1-5

274 macromolecular proton fraction , R1, and MT magnetization transfer ratio in normal-appearing white m

275 Compared with controls, magnetization transfer ratio in the normal-appearing whi

276 The 6-week magnetization transfer ratio map showed good correlation

277 Results In the stenotic kidney, the median magnetization transfer ratio showed progressive increase

278 In control subjects, magnetization transfer ratio was highest adjacent to the

279 ptic neuritis, normal-appearing white matter magnetization transfer ratio was lowest adjacent to the

280 .4-T magnetic resonance imaging examination, magnetization transfer ratio was measured as an index of

281 erosis, tissue abnormality-as assessed using magnetization transfer ratio-increases close to the late

282 the MDD group, MT studies demonstrated lower magnetization transfer ratios (MTR), a marker of abnorma

283 l advantages over (1)H NMR using traditional magnetization-transfer and/or two-dimensional methods.

284 ments could be hyperpolarized by spontaneous magnetization transfers from bound (13)C nuclei followin

285 in the GaMnAs layer, but are negligible when magnetization transitions occur in Fe.

286 Saturation magnetization value obtained for MMIP was 1.72emug(-1).

287 led study of the different components of the magnetization vector as a function of temperature, appli

288 A significant lowering of the magnetization was observed for the nitrogen-doped carbon

289 ckness and an in-plane easy axis (c-axis) of magnetization were grown on a-plane single-crystal sapph

290 tion dynamics excited in an SHO with oblique magnetization when the SHE and i-DMI act simultaneously.

291 gurable micron-scale optical control of both magnetization (which breaks time-reversal symmetry) and

292 d erase arbitrary patterns in their remanent magnetization, which we then image with Kerr microscopy.

293 s attributed to the H KS and M S (saturation magnetization) whose peaks also occur at the same temper

294 Remarkably, bilayer CrI3 displays suppressed magnetization with a metamagnetic effect, whereas in tri

295 arch on pathways to control the direction of magnetization with an electric field.

296 c superparamagnetic responses with saturated magnetization with circular contours, as observed for th

297 measurements reveals slow relaxation of the magnetization, with an effective thermal relaxation barr

298 We imaged the structure of the magnetization within a soft magnetic pillar of diameter

299 netic field needed to flip the ferromagnetic magnetization within femtosecond timescale is unphysical

300 cal deterministic switching of perpendicular magnetization without any assistance from an external ma