ライフサイエンスコーパス: ferromagnet

1 peculiar kind of constrained two-dimensional ferromagnet.

2 governed by an antiferromagnet instead of a ferromagnet.

3 etal and spin transfer torque in an in-plane ferromagnet.

4 et resonating valence bonds into the ordered ferromagnet.

5 ed electrons from the La(0.66)Sr(0.33)MnO(3) ferromagnet.

6 metal or the Rashba-Edelstein effect in the ferromagnet.

7 ral exciton state remains insensitive to the ferromagnet.

8 superconductor upon entering the neighboring ferromagnet.

9 ements show that F4BImNN acts as a quasi-1-D ferromagnet.

10 hysteresis loops reminiscent of a classical ferromagnet.

11 ct as a spin analyzer without the need for a ferromagnet.

12 range Coulomb interactions in a quantum Hall ferromagnet.

13 c axis behave as expected for a local moment ferromagnet.

14 herent magnetization switching dynamics in a ferromagnet.

15 antiferromagnet, canted antiferromagnet, and ferromagnet.

16 d in the bistable magnetization state of the ferromagnet.

17 -activated magnetic switching in a nanoscale ferromagnet.

18 the ease of realizing magnetic reading of a ferromagnet.

19 oscillations in ensemble-averaged spins of a ferromagnet.

20 h the reversal of magnetic field in an Ising ferromagnet.

21 ase transition is the transverse field Ising ferromagnet.

22 ty that makes antiferromagnets distinct from ferromagnets.

23 e writing magnetic field angle, analogous to ferromagnets.

24 rt lifetime of these excitations in metallic ferromagnets.

25 class of enigmatic multiband itinerant, weak ferromagnets.

26 s for writing and reading the information in ferromagnets.

27 with properties that cannot be achieved with ferromagnets.

28 DW if grown between non-co-linearly aligned ferromagnets.

29 could assist or accomplish the switching of ferromagnets.

30 ls that are as large as the highest seen for ferromagnets.

31 han the macroscopic scales characteristic of ferromagnets.

32 previously observed only using half-metallic ferromagnets.

33 materials such as electrical conductors and ferromagnets.

34 ectron magnetism similar to that in metallic ferromagnets.

35 ced magnetoresistance in low-carrier-density ferromagnets.

36 litatively similar to the classic d-electron ferromagnets.

37 with noncompensated magnetic materials like ferromagnets.

38 alized in liquid crystals and liquid crystal ferromagnets.

39 ular momentum between photons, electrons and ferromagnets.

40 an electron and a spin flip - in topological ferromagnets.

41 um processing with spin-transport effects in ferromagnets.

42 st common spin ensembles in nature: spins in ferromagnets.

43 fect (AHE) at room temperature comparable to ferromagnets.

44 to manipulate the magnetization in metallic ferromagnets.

45 these antiferromagnetic materials to become ferromagnets.

46 ctronic band crossings in a mirror-symmetric ferromagnet(14-20).

47 erial systems of contemporary interest: a 2D ferromagnet (1T-CrTe(2)) and a topological semimetal (Zr

48 carrier and the associated magnetization in ferromagnets(2).

49 perconductor interface with an inhomogeneous ferromagnet, a gapless odd frequency superconducting sta

50 unctional, yielding a room-temperature Fe-Pt ferromagnet, a superconducting sample of Ag2Pd3S (Tc = 1

51 hase transition from an antiferromagnet to a ferromagnet above room temperature (Tr approximately 370

52 oxides, polycrystalline ferroelectrics, and ferromagnets alike.

53 The easily measured properties of the ferromagnet allow access to the internal magnetic degree

54 In a ferromagnet, an applied electric field E invariably prod

55 an antiferromagnet and those in an adjacent ferromagnet, an effect first discovered in 1956 and refe

56 ferent Prussian blue analogues, where A is a ferromagnet and B is a photoinducible ferrimagnet, have

57 higher than those of any known ferroelectric ferromagnet and rival the best materials that are solely

58 is a nearly ideal two-dimensional Heisenberg ferromagnet and so will be useful for studying fundament

59 ented multiferroic duality (i.e., switchable ferromagnet and switchable magnetic semiconductor) enabl

60 ar coupling between the magnetization in the ferromagnet and the projection of the antiferromagnetic

61 ine the beneficial spintronics properties of ferromagnets and antiferromagnets, garnering significant

62 tic materials that combines features of both ferromagnets and antiferromagnets, have garnered attenti

63 ing the local excitations of systems such as ferromagnets and antiferromagnets, skyrmions, atomically

64 f magnetic structures, from simple collinear ferromagnets and antiferromagnets, to complex magnetic h

65 Recent studies have explored using thin-film ferromagnets and ferrimagnets to host Neel skyrmions for

66 roach to the benchmark SOT materials such as ferromagnets and heavy metals is challenging.

67 s of light-material interactions in metallic ferromagnets and multilayers.

68 to the coercivity mechanism of Nd-based bulk ferromagnets and provide a new idea to design prospectiv

69 f over 11 T at 2 K outperform all known hard ferromagnets and single-molecular magnets.

70 carriers acquire spin-polarization from the ferromagnet, and dynamically polarize these nuclear spin

71 net-ferromagnet, ferromagnet-paramagnet, and ferromagnet-antiferromagnet metal electrodes.

72 n-pinning at the interface of hetero-bilayer ferromagnet/antiferromagnet structures in conventional e

73 ining effects associated with a conventional ferromagnet/antiferromagnet system.

74 One particularly simple system is a ferromagnet approaching its Curie temperature, T(C), whe

75 ng landscape when the superconductor and the ferromagnet are electron ically coupled or insulated by

76 ct extensions to zigzag antiferromagnets and ferromagnets are also presented.

77 Ferromagnets are commonly magnetized by either external

78 Meanwhile, low-damping metallic ferromagnets are desired for charge-based spintronic dev

79 Ferroelectric ferromagnets are exceedingly rare, fundamentally interes

80 Domain walls in fractional quantum Hall ferromagnets are gapless helical one-dimensional channel

81 to their conductivity, low-damping metallic ferromagnets are preferred to insulating ferromagnets in

82 By contrast, ferromagnets are regarded as an unlikely setting for str

83 La(0.7)Sr(0.3)MnO(3) is a conducting ferromagnet at room temperature.

84 loch point (BP) is a topological defect in a ferromagnet at which the local magnetization vanishes.

85 to induce efficient spin-torque switching of ferromagnets at room temperature.

86 The feasibility of a single-domain ferromagnet based on uniaxial magnetic ions was examined

87 er cooling, the compounds become canted weak ferromagnets below 40 K.

88 for the spin-orbit torques in a heavy metal/ferromagnet bilayer geometry, showing in general both fi

89 that uses current passing through a tantalum-ferromagnet bilayer to switch a nanomagnet, with a magne

90 that spin-orbit interactions in heavy-metal/ferromagnet bilayers can produce strong current-driven t

91 y-metal/ferromagnet or topological-insulator/ferromagnet bilayers, where the heavy metal or topologic

92 ological insulator (TI) is in contact with a ferromagnet, both time-reversal and inversion symmetries

93 progress has been made in investigations of ferromagnets but antiferromagnets are more challenging.

94 nce domain wall motion in ultrathin metallic ferromagnets, but the effects have been relatively modes

95 recently resulted in room-temperature polar ferromagnets, but the electrical polarization has not be

96 c films deposited on electrically insulating ferromagnets, but the films' high resistance limits ther

97 ormed from spin-frustrated semiconductors to ferromagnets by doping with either electrons or holes, p

98 in the magnetization behaviour of thin-film ferromagnets by three distinct mechanisms that can each

99 ar near magnetization inhomogeneities in the ferromagnet, called bifurcations.

100 n current applied to a nanoscale region of a ferromagnet can act as negative magnetic damping and the

101 associated with aligned electron spins in a ferromagnet can be converted to mechanical angular momen

102 The fact that ferromagnets can be studied easily and with high precisi

103 Ferroics, especially ferromagnets, can form complex topological spin structur

104 cyanoethylene) magnetically orders as a weak ferromagnet (canted antiferromagnet) below 21.0 +/- 0.1

105 However, in contrast to the ferromagnet case, few studies have investigated interfac

106 ctly the magnetic anisotropy in the uniaxial ferromagnet CeRu2Ga2B.

107 exponential wavefunction localization at the ferromagnet-chiral molecule interface.

108 ange interactions at the interface between a ferromagnet (Co(0.9)Fe(0.1)) and the antiferromagnet.

109 elds to tune the quasi-one-dimensional Ising ferromagnet CoNb2O6 (cobalt niobate) through its critica

110 In their metallic ferromagnet counterparts, such interfaces also give rise

111 ed by an ultrafast laser pulse within the 2D ferromagnet Cr(2)Ge(2)Te(6).

112 in the recently discovered 2D van der Waals ferromagnet CrI(3).

113 Studies to date on ferromagnet/d-wave superconductor heterostructures focus

114 xamine the dynamics of a uniaxial rare-earth ferromagnet deep within the quantum regime, so that doma

115 the magnetization can be generated within a ferromagnet, despite spin dephasing(8).

116 In common ferromagnets, domain walls are known to be of either Blo

117 nsulators present a promising alternative to ferromagnets due to their ultrafast spin dynamics essent

118 c insulators (e.g. EuO, GdN) or halfmetallic ferromagnets (e.g. CrO2, LCMO).

119 Our hybrid device has a ferromagnet electrode as a spin injector and a spin Hall

120 stigated numerically using thin random-field ferromagnets exhibiting the field-driven magnetisation r

121 per pairs, which arise in superconductor (S)-ferromagnet (F) heterostructures with magnetic inhomogen

122 gnetic inhomogeneity at a superconductor (S)-ferromagnet (F) interface converts spin-singlet Cooper p

123 d phases, such as a superconductor (S) and a ferromagnet (F), is driving new fundamental physics and

124 elopment of Ferromagnet(F)/Superconductor(S)/Ferromagnet(F) pseudo spin-valve devices based on amorph

125 results are promising for the development of Ferromagnet(F)/Superconductor(S)/Ferromagnet(F) pseudo s

126 l the flow of electrons by ferromagnets in a ferromagnet (F1)/normal metal (N)/ferromagnet (F2) spin

127 gnets in a ferromagnet (F1)/normal metal (N)/ferromagnet (F2) spin valve, where F1 acts as the polari

128 Although the strong interactions in a ferromagnet favour the excitation of extended collective

129 As the ferromagnet Fe becomes more noble in the FePt compound,

130 etween a quasi-two-dimensional van der Waals ferromagnet Fe(0.29)TaS(2) and a conventional s-wave sup

131 kelvin above room temperature in the kagome ferromagnet Fe(3)Sn with the Curie temperature of 760 ke

132 rperties of the van der Waals weak-itinerant ferromagnet Fe(3-x)GeTe(2) that features gate-tunable ro

133 , in the near-room-temperature van der Waals ferromagnet Fe(5-delta)GeTe(2).

134 stic, and nonvolatile switching of a PMA vdW ferromagnet, Fe(3)GaTe(2), above room temperature (up to

135 alog (GPMA) connected to the combinations of ferromagnet-ferromagnet, ferromagnet-paramagnet, and fer

136 pies, the SOC mediated interaction between a ferromagnet (FM) and a superconductor (SC) enhances the

137 is considered to arise from the bulk of the ferromagnet (FM) and the proximity-induced FM boundary l

138 The magnetic reversal behavior of a ferromagnet (FM) coupled through an FeMn antiferromagnet

139 the magnetisation dynamics of an insulating ferromagnet (FM) deposited on the surface of a three-dim

140 uced spin accumulation in a heavy metal (HM)/ferromagnet (FM) heterostructure can be regulated to a c

141 Recent discoveries from superconductor (S)/ferromagnet (FM) heterostructures include pi-junctions,

142 means of writing information in heavy metal/ferromagnet (FM) multilayer systems.

143 neration (SHG) to study a ferroelectric (FE)/ferromagnet (FM) oxide heterostructure.

144 lm, accompanying an antiferromagnet (AFM) to ferromagnet (FM) phase transition.

145 e it exerts a unidirectional anisotropy to a ferromagnet (FM) when coupled to an antiferromagnet (AFM

146 /-150 mT external magnetic polarization of a ferromagnet (FM).

147 ults presented here show the potential of 2D ferromagnets for low-power memory and logic applications

148 Chromium telluride compounds are promising ferromagnets for proximity coupling to magnetic topologi

149 onary topological solitons in a fluid chiral ferromagnet formed by colloidal dispersions of magnetic

150 5) in some insulating ferromagnets, metallic ferromagnets generally have larger damping due to magnon

151 Depending on the ferromagnet geometry and material parameters, this asymm

152 of a single classical spin (e.g. monodomain ferromagnet) governed by the Landau-Lifshitz-Gilbert-Slo

153 ces that, rather than reorienting spins in a ferromagnet, harness direct control of a materials intri

154 ugh an FeMn antiferromagnet (AF) to a pinned ferromagnet has been investigated by polarized neutron r

155 ts.The study of phase transitions in quantum ferromagnets has shown that the approach to a continuous

156 Therefore, Sr4Ru3O10, a T C = 105 K ferromagnet, has attracted much attention in recent year

157 La(0.7)Sr(0.3)MnO(3), a strong semi-metallic ferromagnet having robust spin polarization and magnetic

158 DMI manifests at metallic ferromagnet/heavy-metal interfaces, owing to inversion s

159 ching in a full vdW topological semimetal/2D ferromagnet heterostructure device.

160 rse magnetostriction effect in piezoelectric/ferromagnet heterostructures holds promise for ultra-low

161 tional superconductors coupled with metallic ferromagnets; however it is still less known for oxide m

162 re, the magnetization of a semiconducting 2D ferromagnet, i.e., Cr(2) Ge(2) Te(6) , is studied using

163 Each nanocylinder consists of a ferromagnet in a single-domain magnetic state and a high

164 of exchange bias with unusual features of a ferromagnet in contact with a spin glass, demonstrating

165 fields from both, the superconductor and the ferromagnet in hybrid magnetic nano-devices based on hig

166 nifested in heterostructures consisting of a ferromagnet in intimate contact with the multiferroic Bi

167 , exhibited loss of magnetic contrast on one ferromagnet in MFM imaging.

168 ntronics to control the flow of electrons by ferromagnets in a ferromagnet (F1)/normal metal (N)/ferr

169 lic ferromagnets are preferred to insulating ferromagnets in charge-based spintronic devices, but are

170 The ferromagnets in question are disordered, low-carrier-den

171 erial is well described as a two-dimensional ferromagnet, in sharp contrast to the high-T(C) cuprates

172 ng of ferromagnetic/nonmagnetic systems, the ferromagnet-induced magnetic moment in the adjacent nonm

173 ons, we explain why the Co chalcogenides are ferromagnets instead of superconductors as in their iron

174 In particular, by switching the graphene/ferromagnet interaction, spin transport reveals magneto-

175 magnetic exchange field at a superconductor/ferromagnet interface converts spin-singlet Cooper pairs

176 imity effect at the hybridized 2D material / ferromagnet interface for 2D-MTJs.

177 we report a study of spin pumping at the TI-ferromagnet interface, investigating spin transfer dynam

178 pin-Hall-effect-driven antidamping torque in ferromagnets interfaced with paramagnets with strong int

179 ephson junctions in which the superconductor/ferromagnet interfaces (S/F) are magnetically inhomogene

180 effect at complex-oxide-based superconductor/ferromagnet interfaces is not so clear.

181 and few-layer Cr(2)Ge(2)Te(6), an insulating ferromagnet, into close proximity in an heterostructure,

182 as the hysteresis-loop shift observed when a ferromagnet is in contact with an antiferromagnet.

183 of the TI spin onto the magnetization of the ferromagnet is measured as a voltage.

184 nowledge of how magnetization looks inside a ferromagnet is often hindered by the limitations of the

185 igh-resolution spectroscopic study of the 2D ferromagnet is still lacking due to the small size and a

186 The physics of weak itinerant ferromagnets is challenging due to their small magnetic

187 perties in recently discovered van der Waals ferromagnets is essential for their integration in futur

188 al control of the magnetization switching in ferromagnets is highly desired for future spintronic app

189 m that drives the magnetisation switching in ferromagnets is unclear.

190 magnetization of a model disordered uniaxial ferromagnet, is an isothermal regulator of domain pinnin

191 ffect, discovered more than 150 years ago in ferromagnets, is also present in AFMs.

192 d that when an ultrafast laser impinges on a ferromagnet, its spin moment undergoes a dramatic change

193 2Cu3O7 (YBCO) and colossal magnetoresistance ferromagnet La0.67Ca0.33MnO3 (LCMO).

194 Here we show that the ferromagnet La2-2xSr1+2xMn2O7 (x = 0.38) possesses minor

195 on by interfacial coupling to the insulating ferromagnet LaMnO3, and used to generate interlayer magn

196 e target spin separation is smaller than the ferromagnet lateral dimensions; typically about a tenth

197 and so drive the spin precession of another ferromagnet layer coherently?

198 ultrafast demagnetization of a perpendicular ferromagnet leads to spin accumulation in a normal metal

199 intense photoexcitation in several metallic ferromagnets leads to a drop in magnetization on a times

200 dict that Fe-doped CaZnOS is a single-domain ferromagnet like a bar magnet, and find the probable cau

201 in a bulk semiconductor without the need for ferromagnets, lithographic patterning techniques, or qua

202 hous paramagnetic layer through proximity to ferromagnets, mediating both exchange-spring magnet beha

203 an reach 10(-4) to 10(-5) in some insulating ferromagnets, metallic ferromagnets generally have large

204 neutron scattering experiments that the bulk ferromagnet Mn(5)Ge(3) hosts gapped topological Dirac ma

205 tronic structure and lattice dynamics in the ferromagnet MnBi using first-principles calculations and

206 lt of Weyl bands in inversion-symmetric Weyl ferromagnet MnSb(2)Te(4).

207 utron scattering to study the itinerant near-ferromagnet MnSi, we find that the system's fundamental

208 fluctuations in the canonical weak itinerant ferromagnet MnSi.

209 le AHE is rather well-understood in metallic ferromagnets, much less is known about the relevance of

210 Nb/EuS structures where EuS is an insulating ferromagnet, Nb is a superconductor and Au is a heavy me

211 NaFe4Sb12 is a known ferromagnet near a quantum critical point.

212 this is possible in composites of conducting ferromagnets (Ni or MnBi) containing metallic nanopartic

213 Semiconducting ferromagnet-nonmagnet interfaces in van der Waals hetero

214 Although now a ubiquitous observation in ferromagnets, obvious flux-closure patterns have been so

215 register between perpendicularly magnetized ferromagnets of subnanometre thickness, similar to the l

216 omagnets has much shorter timescales than in ferromagnets, offering attractive properties for potenti

217 This record low damping for metallic ferromagnets offers new opportunities for charge-based a

218 f anisotropy of a thin layer of a conductive ferromagnet on a dielectric substrate under the influenc

219 py magnetic devices comprised of heavy-metal/ferromagnet or topological-insulator/ferromagnet bilayer

220 agnetic devices results from the torque on a ferromagnet owing to its interaction with a spin-polariz

221 easurements of magnetic noise emanating from ferromagnets owing to domain motion were first carried o

222 The ferromagnet/oxide interface is key to developing emergin

223 the combinations of ferromagnet-ferromagnet, ferromagnet-paramagnet, and ferromagnet-antiferromagnet

224 in torques induced by a lateral current at a ferromagnet/paramagnet interface are a candidate spintro

225 e presence of two-channel Kondo physics in a ferromagnet, pointing to considerable robustness of the

226 The bistability of ordered spin states in ferromagnets provides the basis for magnetic memory func

227 d state switches between antiferromagnet and ferromagnet, providing an additional tuning parameter in

228 The superconductor-ferromagnet proximity effect describes the fast decay of

229 urrents can be manipulated in superconductor/ferromagnet proximity systems via nonequilibrium spin in

230 tion of charge pumping in which a precessing ferromagnet pumps a charge current, demonstrating direct

231 nuclear polarization (DNP) in a quantum Hall ferromagnet (QHF) is a highly sensitive method for the d

232 gy are central to understanding quantum Hall ferromagnets (QHFMs), two-dimensional electronic phases

233 an arise by a different mechanism in certain ferromagnets--quantum interference effects rather than s

234 Spin selectivity in a ferromagnet results from a difference in the density of

235 perconducting diodes based on superconductor/ferromagnet (S/F) bilayers were demonstrated more than a

236 tion of the magnetic field in superconductor/ferromagnet (S/F) hybrids.

237 ow well established that at a superconductor/ferromagnet (S/F) interface an unconventional supercondu

238 polarized nuclear spins that align along the ferromagnet's magnetization.

239 stinguishing feature of spin accumulation in ferromagnet-semiconductor devices is its precession in a

240 ues in a prepared epitaxial transition-metal ferromagnet/semiconductor-paramagnet single-crystal stru

241 e generated with magnetic inhomogeneity at a ferromagnet/spin-singlet-superconductor interface.

242 However, spin-polarized supercurrents in ferromagnet/spin-triplet-superconductor junctions can be

243 induction of spin-triplet correlation into a ferromagnet SrRuO(3) epitaxially deposited on a spin-tri

244 c magnon modes in a spin-source/multiferroic/ferromagnet structure.

245 e spin-orbit torque switching in heavy metal/ferromagnet structures have been proposed with magnetic

246 While the energy scales of the rare earth ferromagnet studied here restrict the effects to cryogen

247 e required for switching nonlayered metallic ferromagnets such as CoFeB.

248 structure phase diagram as seen in itinerant ferromagnets such as ZrZn2 and UGe2.

249 Owing to strong magnetic coupling with the ferromagnet, such independent switching of an adsorbed m

250 In magnetically coupled, planar ferromagnet-superconductor (F/S) hybrid structures, magn

251 nd induced spin-triplet superconductivity at ferromagnet/superconductor interface arising from Rashba

252 ensitivity is practically unchanged when the ferromagnet surface to the target spin separation is sma

253 ploited, it does not extend to semiconductor/ferromagnet systems, because the effect is too weak for

254 For heavy-metal/ferromagnet systems, harmonic characterization is a powe

255 nerated by the magnetization dynamics of the ferromagnet that also forms at the same interface, which

256 Despite recent advances in exfoliated vdW ferromagnets, the widespread application of 2D magnetism

257 ty for the phase diagram of metallic quantum ferromagnets.The study of phase transitions in quantum f

258 c exchange interaction with the surface of a ferromagnet; the device shows an unexpected interfacial

259 rison with those of useful ferroelectrics or ferromagnets: their spontaneous polarizations or magneti

260 zewski-like torque inversely scales with the ferromagnet thickness, and the field-like torque has a t

261 trical current can apply a large torque to a ferromagnet, through direct transfer of spin angular mom

262 involving the change of the magnetic state (ferromagnet to antiferromagnet) has been proposed.

263 rent, which can be injected into an adjacent ferromagnet to exert a torque.

264 duces a two serial magnetic transitions from ferromagnet to non-magnet state at room temperature.

265 ere that by forcing the magnetization in the ferromagnet to precess at resonance instead of relying o

266 ept may eventually reduce the sensitivity of ferromagnets to magnetic field perturbations to being a

267 intronics depends on the spin sensitivity of ferromagnets to the spin of the equal spin-triplet Coope

268 viding evidence of a spin selectivity of the ferromagnets to the spin of the triplet Cooper pairs.

269 At a critical temperature, where the ferromagnet transitions to a paramagnetic state, we obse

270 tum locking has been detected recently using ferromagnet/tunnel barrier contacts, where the projectio

271 he pioneering S/FI (where FI is a insulating ferromagnet) tunneling experiments of Meservey and Tedro

272 Herein we show that, unlike in ferromagnets, ultrafast damping plays a crucial role in

273 omalous Hall conductivity in a Kondo lattice ferromagnet USbTe which is dominated by intrinsic Berry

274 detail required for the characterization of ferromagnets used in fields ranging from spintronics to

275 a of spin Hall material into a small area of ferromagnet using a normal metal with large spin diffusi

276 omagnetic are transformed into ferroelectric ferromagnets using a single control parameter, strain.

277 e quantization, in super-conductor/insulator/ferromagnet (V/MgO/Fe) junctions, we discover a giant in

278 ently, however, a new route to ferroelectric ferromagnets was proposed by which magnetically ordered

279 etically soft, two-dimensional van der Waals ferromagnet, we achieve unprecedented control of the tra

280 ture of cousin material Fe(3)Sn(2) that is a ferromagnet, we find that electronic density-of-states o

281 0 < or = x < or = 2) phases are not ordinary ferromagnets where all the magnetic spins are parallel a

282 ntiferromagnet film is exchange coupled to a ferromagnet, which allows us to reorient the antiferroma

283 ween an antiferromagnet or ferrimagnet and a ferromagnet, which has been widely employed to manipulat

284 c quantum phenomenon is spin tunnelling in a ferromagnet, which may be formulated in terms of domain

285 In this regime, insulating 2D ferromagnets, which remain rare, are of special importan

286 However, the presence of dipolar fields in ferromagnets, which restricts the formation of ultrasmal

287 hod is to investigate macroscopic disordered ferromagnets, whose dynamics are dominated by domain wal

288 re energetically stable entities formed in a ferromagnet with a diameter of typically below 100 nm an

289 system comes from the fact that it is a hard ferromagnet with a large coercive field (Hc > 1.0 T) and

290 olayer chromium triiodide (CrI3) is an Ising ferromagnet with out-of-plane spin orientation.

291 preserving the magnetic properties of solid ferromagnets with classic north-south dipole interaction

292 CoSe and CoS are found to be weak itinerant ferromagnets with Curie temperatures close to 10 K.

293 Ferromagnets with high spin polarization are known to be

294 romagnets can improve the functionalities of ferromagnets with higher response times, and having the

295 om temperature in ultrathin transition metal ferromagnets with magnetic transmission soft X-ray micro

296 le to existing classes of highly anisotropic ferromagnets with ordering at room temperature or above.

297 The switching of ferromagnets with perpendicular magnetization is of part

298 work demonstrates that in spin-orbit-coupled ferromagnets with weak extrinsic domain wall pinning, th

299 r spin-orbit torque in spintronic devices of ferromagnets without inversion symmetry.

300 iscovered several decades ago, the itinerant ferromagnets ZrZn2 and Sc3In, the understanding of their