ライフサイエンスコーパス: ferromagnetic

1 lets as the nanoreactors, which are strongly ferromagnetic.

2 even though the bulk ground state of LSMO is ferromagnetic, a large lattice constant together with an

3 ffect, a magnetic interaction that couples a ferromagnetic and an antiferromagnetic material, resulti

4 ts both the combination of pairwise Mn(III)2 ferromagnetic and antiferromagnetic exchange interaction

5 attributed to the relative stability of the ferromagnetic and antiferromagnetic ground states, arisi

6 2) Rh(0.48) thin films designed so that both ferromagnetic and antiferromagnetic phases are bistable

7 Materials that are simultaneously ferromagnetic and ferroelectric - multiferroics - promis

8 surate magnetic domains, can be described by ferromagnetic and ferroelectric domains only.

9 ction (IDMI) occurs at the interface between ferromagnetic and heavy metal layers with strong spin-or

10 extracting the crossover region between the ferromagnetic and paramagnetic phases.

11 ntrol of the transition temperature (between ferromagnetic and paramagnetic states) using very small

12 MENs and control ferromagnetic and polymer nanoparticles conjugated with

13 s study presents an opportunity to integrate ferromagnetic and semiconducting properties through the

14 The SmCo(5) particles are strongly ferromagnetic and the aligned particles in epoxy resin e

15 m of correlated insulating, superconducting, ferromagnetic and topological phases(1-6).

16 magnetic phases, such as ferromagnetic, anti-ferromagnetic, and frustrated spin configurations on a l

17 We realize various magnetic phases, such as ferromagnetic, anti-ferromagnetic, and frustrated spin c

18 or skyrmion formation in a bilayer system of ferromagnetic/antiferromagnetic (FM/AFM) films, in which

19 ions, we find that the Kitaev interaction is ferromagnetic, as in 5d(5) iridium honeycomb oxides, and

20 VI(3) becomes ferromagnetic at 49 K, below which magneto-optical Kerr

21 tic at 5 unit cells (ucs) of LMO or below to ferromagnetic at 6 ucs or above, yet such a study is mis

22 ordering changing from antiferromagnetic to ferromagnetic at a critical magnetic field.

23 T thin films are multiferroic (ferroelectric-ferromagnetic) at room temperature.

24 In 3D-MTC, ferromagnetic beads are bound to the cell surface via su

25 ange 5-300 K, the Te-doped nanowires exhibit ferromagnetic behavior with the easy axis of magnetism p

26 the surface, while the plates show distinct ferromagnetic behaviour due to the strong competition be

27 old evolution from the superferromagnetic to ferromagnetic behaviour within the FeNi layer leads to t

28 etic order in an interlayer exchange-coupled ferromagnetic bilayer.

29 urrently accessible in ultrathin heavy metal/ferromagnetic bilayers and multilayers with a strong Dzy

30 electrical and programmable manipulations of ferromagnetic bits are highly pursued for the aim of hig

31 The spin on a ferromagnetic Co surface can interact with the asymmetri

32 Perpendicular magnetic anisotropy (PMA) ferromagnetic CoFeB with dual MgO interfaces is an attra

33 but a canted antiferromagnetic order with a ferromagnetic component for T < 304 K.

34 trate the predicted emergence of spontaneous ferromagnetic correlations through pairwise measurements

35 amics is expected to be much faster than its ferromagnetic counterpart.

36 Magnetic susceptibility reveals strong ferromagnetic coupling between iron centers, with a coup

37 [((R)DDB)Fe(NO)2((*)NO)](+) results from the ferromagnetic coupling between two strictly orthogonal o

38 , an orthorhombic-like structure, and strong ferromagnetic coupling.

39 ultiferroics by stacking up atomic layers of ferromagnetic Cr(2)Ge(2)Te(6) and ferroelectric In(2)Se(

40 ement with respect to previously studied all-ferromagnetic crosses, as they also reduce the pinning p

41 e visualized the electronic structure of the ferromagnetic crystal Co(3)Sn(2)S(2) and discovered its

42 limited by superparamagnetism in very small ferromagnetic crystals.

43 ductivity, our observations suggest that the ferromagnetic Dirac fermions in Fe(3)Sn(2) are subject t

44 ing of a square array of micrometer-sized Py ferromagnetic disks covered by a superconducting Nb thin

45 tures based on controllable ferroelectric or ferromagnetic domain configurations offer the opportunit

46 rromagnetic pyrochlores with strongly-pinned ferromagnetic domain walls, which both exhibit antisymme

47 magnetic field as well as antiferromagnetic/ferromagnetic domains at finite magnetic fields.

48 to-optical Kerr effect imaging clearly shows ferromagnetic domains, which can be manipulated by the a

49 ion today is encoded in the magnetization of ferromagnetic domains.

50 Incorporating ferromagnetic dopants into three-dimensional topological

51 ional quantum materials that remain strongly ferromagnetic down to monolayer thickness are highly des

52 of antiferromagnetic domain walls (DWs) than ferromagnetic DWs.

53 Thus far, NV sensing of ferromagnetic dynamics has been constrained to the case

54 ecific interactions of the molecule with the ferromagnetic electrode but from the polarized spin that

55 flipping the magnetization direction of the ferromagnetic electrode.

56 lations, the strength of interaction between ferromagnetic electrodes and graphene monolayers is show

57 has long been encumbered by its reliance on ferromagnetic electrodes for polarized spin injection.

58 hylammonium lead bromide films from metallic ferromagnetic electrodes in two spintronic-based devices

59 esults confirm that quasi-atomic IAEs act as ferromagnetic elements and trigger ferromagnetic spin al

60 tured [Gd(2)C](2+).2e(-) electride behave as ferromagnetic elements in two-dimensional interlayer spa

61 zation completely in out-of-plane magnetized ferromagnetic elements, but the switching is determinist

62 e interfacial magnetic exchange field from a ferromagnetic EuS substrate, and band-to-band tunnel fie

63 rfacial magnetic exchange field (MEF) from a ferromagnetic EuS substrate.

64 ghbor antiferromagnetic and nearest-neighbor ferromagnetic exchange interactions can induce rich magn

65 form, tphz(*-), promotes a remarkably large ferromagnetic exchange of +214(5) K with Ni(II) spins.

66 The correlated Chern insulator is ferromagnetic, exhibiting substantial magnetic hysteresi

67 ic ordering is dominated by the formation of ferromagnetic Fe(3+)-Fe(2+)-Fe(3+) trimers which are evi

68 ange as paramagnetic Al addition dilutes the ferromagnetic Fe/Co/Ni additions.

69 a and magnetic FeNi nanoisland layers, where ferromagnetic FeNi nanoislands have giant magnetic momen

70 out the need for solution processing, yields ferromagnetic FePt nanomotors that are noncytotoxic, bio

71 Here we study the multiferroic domains in ferromagnetic ferroelectric Mn2GeO4 using neutron diffra

72 ministic magnetization switching in a hybrid ferromagnetic/ferroelectric structure with Pt/Co/Ni/Co/P

73 Among such ferromagnetic ferroelectrics are conical spin spiral mag

74 spontaneous magnetic reversal of the entire ferromagnetic film, and an inverted magnetic hysteresis,

75 strain manipulates the magnetization of the ferromagnetic film.

76 Thin ferromagnetic films are growing in importance technologi

77 Upon doping, ferromagnetic fluctuations are argued to lead to spin-tr

78 h results in four stable magnetic states: +/-ferromagnetic (FM) and +/-antiferromagnetic (A-FM).

79 The sign reversal is attributed to competing ferromagnetic (FM) and antiferromagnetic (AFM) exchange

80 We report the observation of ferromagnetic (FM) and antiferromagnetic (AFM) interlaye

81 Spin-orbit torques (SOTs) in multilayers of ferromagnetic (FM) and non-magnetic (NM) metals can mani

82 the realization of MeRAM relies primarily on ferromagnetic (FM) based heterostructures which exhibit

83 The change of magnetization in ferromagnetic (FM) layer induces an elastic stress in th

84 a: see text]1.5 GPa, and the other is from a ferromagnetic (FM) metal to an antiferromagnetic (AFM) i

85 spontaneous helical light emission(3,4) from ferromagnetic (FM) monolayers and electric-field induced

86 ctrical control of magnetic properties using ferromagnetic (FM) nanostructures, an opportunity of man

87 ansition from an antiferromagnetic (AF) to a ferromagnetic (FM) phase between 75-105 degrees C.

88 nusual first-order antiferromagnetic (AF) to ferromagnetic (FM) phase transition.

89 synergic influence of superconductor (SC) - ferromagnetic (FM) stray fields, in both the superconduc

90 y in pairs or groups in two-dimensional (2D) ferromagnetic (FM) systems.

91 report the observation of exchange bias in a ferromagnetic Ga(0.94)Mn(0.06)As(0.77)P(0.23)/ Ga(0.94)M

92 uss the use of planar Hall effect (PHE) in a ferromagnetic GaMnAs film with two in-plane easy axes as

93 e in creating magnetic field noise below the ferromagnetic gap frequency which causes NV spin relaxat

94 Ferromagnetic Gd(5)Si(4) particles were formulated in te

95 quasi-atomic IAEs through a transition from ferromagnetic [Gd(2)C](2+).2e(-) to antiferromagnetic Gd

96 Hybrid normal metal/ferromagnetic, gold/permalloy (Au/Py), nanojunctions are

97 Here, we report the first example of ferromagnetic graphene achieved by controlled doping wit

98 s ratio grows greater than 1, resulting in a ferromagnetic ground state at filling factor nu = 2.

99 We find that the ferromagnetic ground state is remarkably robust to engin

100 at while the sample exhibits an out-of-plane ferromagnetic ground state, an in-plane antiferromagneti

101 ingle-particle ab initio calculations in the ferromagnetic ground state, which indicates intermediate

102 red, non-magnetic, ground state to a splayed ferromagnetic ground state.

103 itrogen contributed much less to the overall ferromagnetic ground state.

104 magnetism is metastable within the otherwise ferromagnetic ground state.

105 ructure calculations confirm the presence of ferromagnetic ground states that arise from direct excha

106 ting in a unidirectional displacement of the ferromagnetic hysteresis loop by an amount called the 'e

107 at [Formula: see text], we observe emergent ferromagnetic hysteresis, with a giant anomalous Hall (A

108 the pristine bandgap and displays pronounced ferromagnetic hysteresis.

109 uple [Bi(2)Te(3)] layers, we show that it is ferromagnetic in plane but antiferromagnetic along the c

110 When restoring stoichiometry, an enhanced ferromagnetic insulating state in LMO films with a thick

111 esponses in the prototypical two-dimensional ferromagnetic insulator, CrI(3).

112 es of the three phases-HSrCoO2.5 is a weakly ferromagnetic insulator, SrCoO3-delta is a ferromagnetic

113 . Nb, Al) and either strongly spin-polarized ferromagnetic insulators (e.g. EuO, GdN) or halfmetallic

114 Ferromagnetic insulators (FMIs) are one of the most impo

115 At half-filling, ferromagnetic insulators are stabilized with valley Cher

116 sm and giant Kerr signals in atomically thin ferromagnetic insulators.

117 ward a new generation of antiferromagnetic - ferromagnetic interactions for spintronics.

118 he of Cr(3+) moments and suggest short-range ferromagnetic interactions.

119 s and/or octahedral rotations, ferroelectric-ferromagnetic interfaces are affected by symmetry mismat

120 e state of a bilayer, which is terminated by ferromagnetic iron clusters that break TRS.

121 system upon laser-induced demagnetization of ferromagnetic iron is transferred to the lattice on sub-

122 r magnetic energy transduction that utilizes ferromagnetic islands (FIs) on the surface of a 3D time-

123 hese complexes, which is not manifest in the ferromagnetic J(SQ-B-NN) values.

124 antum de Haas-van Alphen oscillations of the ferromagnetic kagome lattice metal Fe(3)Sn(2).

125 ectively defect-free, purely manganese-based ferromagnetic kagome lattice with atomic resolution.

126 eld Nernst effect in a newly discovered hard-ferromagnetic kagome-lattice Weyl-semimetal Co(3) Sn(2)

127 Here we provide evidence that the pure ferromagnetic Kondo lattice(9,10) CeRh(6)Ge(4) becomes a

128 ffect with a pulsed tunneling current from a ferromagnetic La(0.67)Sr(0.33)MnO(3) electrode.

129 a strain-released film of epitaxially grown ferromagnetic La(0.7)Sr(0.3)MnO(3) and an electroactive

130 cate a multiferroic tunnel junction based on ferromagnetic La0.7Sr0.3MnO3 electrodes separated by an

131 the interactions between the geometry of the ferromagnetic layer and components of the spin-orbit tor

132 By varying the ferromagnetic layer composition, we can tailor the magne

133 t flowing through the heavy metal instead of ferromagnetic layer realizes the "end to end" circulatio

134 t with transverse spin polarization into the ferromagnetic layer via the spin Hall effect.

135 sembled molecular monolayer on a gold-coated ferromagnetic layer with perpendicular magnetic anisotro

136 esulting in a lateral Pt gradient within the ferromagnetic layer, as confirmed by microstructure and

137 spin-orbit interactions and transition-metal ferromagnetic layers provide a large and tunable DMI.

138 ferromagnetism is the spatial arrangement of ferromagnetic layers with antiferromagnetic interlayer c

139 Nothing similar to the ferromagnetic-like hysteresis loop can be observed in Bi

140 he field dependence of magnetization reveals ferromagnetic-like hysteresis loop with a remanent magne

141 agnetic susceptibility measurements revealed ferromagnetic-like phase transitions at temperatures of

142 These ferromagnetic liquid droplets exhibit a finite coercivit

143 und that quark nuggets could well exist as a ferromagnetic liquid with a 10(12)-T magnetic field.

144 at quark nuggets may exist in magnetars as a ferromagnetic liquid with a magnetic field B(S) = 10(12+

145 Since the magnetic field needed to flip the ferromagnetic magnetization within femtosecond timescale

146 Recently, ferromagnetic material is demonstrated in AOS under mult

147 pond and be aligned to magnetic field like a ferromagnetic material.

148 Two-dimensional (2D) van der Waals ferromagnetic materials are emerging as promising candid

149 Solid ferromagnetic materials are rigid in shape and cannot be

150 owave fields on specimens, such as observing ferromagnetic materials at resonance.

151 l model may provide a guide to find suitable ferromagnetic materials for AOS.

152 Here we study two classes of ferromagnetic materials, rare-earth magnets with high in

153 In soft ferromagnetic materials, the smoothly varying magnetizat

154 omain walls have been intensively studied in ferromagnetic materials, where they nucleate at the boun

155 d devices are typically related to inorganic ferromagnetic materials.

156 that in a nonmagnetic metal (NM) or at a NM/ferromagnetic metal (FM) bilayer interface, the symmetry

157 (AFM-I) and the perovskite SrCoO3 that is a ferromagnetic metal (FM-M), owing to their multiple vale

158 Uniaxial and biaxial strain suppresses the ferromagnetic metal at distinctly different strain value

159 a sample excites resonant magnons in a thin ferromagnetic metal layer.

160 Using the ferromagnetic metal SrRuO(3) as a model system, we demon

161 y ferromagnetic insulator, SrCoO3-delta is a ferromagnetic metal, and SrCoO2.5 is an antiferromagneti

162 er" phenomena has remained elusive in nearly ferromagnetic metals and in dielectrics on the border of

163 ore, a possible experimental scheme by using ferromagnetic metals as electrodes is proposed to detect

164 rvations of switching of magnetic domains in ferromagnetic metals by circularly polarized light, so-c

165 r injection into organic semiconductors from ferromagnetic metals by using various interface engineer

166 ar effects are also observed in other common ferromagnetic metals, including Co, Ni and Fe.

167 s that include only interband transitions in ferromagnetic metals.

168 equency of the LC circuit composed of a soft ferromagnetic microwire coil that contains the ferromagn

169 scribe results in three models: the 2D Ising ferromagnetic model, the 3D Vicsek flocking model and a

170 tematically modulated by the rotation of the ferromagnetic moment.

171 ayered antiferromagnetism, in which adjacent ferromagnetic monolayers are antiferromagnetically coupl

172 ting film, patterned with antidots, and with ferromagnetic nano-rods grown inside them.

173 ternating temperature excites magnons in the ferromagnetic nanolayer which are detected by measuring

174 lectivity effect is used along with 30-50 nm ferromagnetic nanoplatelets in order to realize a simple

175 Domain walls in ferromagnetic nanowires are potential building-blocks of

176 induced stochastic switching effects in soft ferromagnetic nanowires is a critical challenge for real

177 ms of stochastic domain wall pinning in soft ferromagnetic nanowires.

178 on spin resonance measurement elucidates the ferromagnetic nature of ZnCoO by the formation of Co-H-C

179 N-PT) unclamped piezoelectric membranes with ferromagnetic Ni overlayers.

180 ion when investigating spin-orbit torques in ferromagnetic/non-magnetic bilayers.

181 Spintronic ferromagnetic/non-magnetic heterostructures are novel so

182 c) ) of 49.2 kOe, the largest H(c) among all ferromagnetic NPs ever reported, and saturated magnetic

183 The method was extended to synthesize other ferromagnetic NPs of Sm(2) Co(17) , and, for the first t

184 tion is one and a half times larger than the ferromagnetic one, a magnetic phase composed of canting

185 ends on the stacking order and can be either ferromagnetic or antiferromagnetic.

186 space to tune the hybridization between the ferromagnetic order and meron-like defects.

187 We report the emergence of itinerant ferromagnetic order below 4 kelvin for doping beyond the

188 This material exhibits a ferromagnetic order for 304 K < T < 565 K, but a canted

189 Neel order in an antiferromagnetic CrSb and ferromagnetic order in Cr-doped (Bi,Sb)2Te3, we realize

190 Here we report intrinsic long-range ferromagnetic order in pristine Cr2Ge2Te6 atomic layers,

191 The realization of long-range ferromagnetic order in two-dimensional van der Waals cry

192 The existence of this ferromagnetic order is evidenced by negative, anisotropi

193 transition from layered antiferromagnetic to ferromagnetic order tunes the spectral intensity of the

194 native explanation - competition of HTS with ferromagnetic order, fluctuating in superconducting samp

195 netic Bragg peaks evidence long-range static ferromagnetic order, inelastic scattering shows that sho

196 S with overdoping is not caused by competing ferromagnetic order.

197 e with in-plane magnetic field, suggesting a ferromagnetic order.

198 The ordered magnetic arrangement (ferromagnetic ordering in the ab plane and antiferromagn

199 ase in bandgap is additionally attributed to ferromagnetic ordering in the monoclinic phase to facili

200 observed at room temperature, and it retains ferromagnetic ordering in the temperature range 5-395 K.

201 olid [(+)-NDI-Delta(3(-*))(CoCp2(+))3] shows ferromagnetic ordering with a Curie temperature TC = 20

202 a metallic phase with high conductivity and ferromagnetic ordering with high saturation moment.

203 l direction, with both antiferromagnetic and ferromagnetic orders.

204 coupling of its antiferromagnetic order to a ferromagnetic overlayer.

205 A room temperature amorphous ferromagnetic oxide semiconductor can substantially redu

206 emonstrate a strategy for creating ultrathin ferromagnetic oxides by exploiting atomic heterointerfac

207 urify trypsin based on affinity binding with ferromagnetic particles of azocasein composite (mAzo).

208 e devices are based on a pair of interacting ferromagnetic particles of different size and different

209 Yb(2)Ti(2)O(7) is a quantum spin liquid or a ferromagnetic phase induced by a Higgs transition appear

210 e ability to write arbitrary patterns of the ferromagnetic phase is demonstrated by local heating wit

211 Metamagnetism occuring inside a ferromagnetic phase is peculiar.

212 The sp(2) carbon framework induces ferromagnetic phase transition to develop spin-spin cohe

213 Here we show that a canted ferromagnetic phase which is preceded by local point sym

214 nnealing in oxygen exhibit a transition to a ferromagnetic phase, and this is the true magnetic groun

215 The metastable ferromagnetic phases of LaTcO(3) and LaPtO(3) with prese

216 gnetoelectric (ME) antennas with a suspended ferromagnetic/piezoelectric thin-film heterostructure.

217 We find that the ferromagnetic polarization of the unpaired-spin states i

218 ubic perovskite (i.e. Fm - 3m), (2) the weak ferromagnetic properties and excess magnetic moment of P

219 st importantly, strange-metal behaviour at a ferromagnetic QCP suggests that quantum entanglement-not

220 esults open up a direction for research into ferromagnetic quantum criticality and establish an alter

221 netic systems under pressure have shown that ferromagnetic quantum criticality is avoided either by a

222 ral chemical approach to synthesize strongly ferromagnetic rare-earth metal (REM) based SmCo and SmFe

223 on of antiferromagnetic coupling between the ferromagnetic region and the pinned layer.

224 with a pathway to "hide" or "reveal" a given ferromagnetic region at zero magnetic field.

225 sis of the critical properties in the forced ferromagnetic region yields 3D Heisenberg exponents beta

226 ferromagnetically reduced layer and the bulk ferromagnetic region.

227 nature of magneto-electric (ME) coupling by ferromagnetic resonance (FMR) under an electric field in

228 oherent GHz ac spin current pumped by the Py ferromagnetic resonance can transmit coherently across a

229 in Pt by reproducing published experimental ferromagnetic resonance data in the bilayer geometry.

230 refore, by applying the model to analyze the ferromagnetic resonance data, the distribution of orient

231 By employing ferromagnetic resonance driven spin pumping and the inve

232 Quasi-static magnetometry and dynamic ferromagnetic resonance measurements identify a uniaxial

233 effect are evident from the deeply modulated ferromagnetic resonance of Py due to the perpendicular-s

234 Here, we use ferromagnetic resonance spectroscopy to measure the magn

235 Using x-ray scattering and ferromagnetic resonance techniques, we provide unambiguo

236 al can be controlled by driving the system's ferromagnetic resonance.

237 ng sample magnetometry and a frequency-swept ferromagnetic resonant flip-chip technique, respectively

238 The magnetic properties and ferromagnetic resonant frequencies were experimentally c

239 tal murine colonic window with a stabilizing ferromagnetic scaffold for chronic imaging, minimizing m

240 We report a new diluted ferromagnetic semiconductor Li(1+y)(Cd,Mn)P, wherein car

241 ounterparts, diamondene is predicted to be a ferromagnetic semiconductor with spin polarized bands.

242 inertial displacement of a domain wall in a ferromagnetic semiconductor.

243 of Eu-cyclooctatetraene (EuCot), a predicted ferromagnetic semiconductor.

244 Ferromagnetic semiconductors (FMSs) featuring a high Cur

245 g three distinct surface terminations of the ferromagnetic semimetal Co(3)Sn(2)S(2), we verify spectr

246 llow more flexible control than conventional ferromagnetic skyrmions(5-10).

247 art-Derrick theorem, like in two-dimensional ferromagnetic solitons, dubbed 'baby skyrmions'.

248 quantum electrodynamics system with a small ferromagnetic sphere in a microwave cavity and engineer

249 engenders up to a 90% increase in potential ferromagnetic spin alignments in the central layer and t

250 Es act as ferromagnetic elements and trigger ferromagnetic spin alignments within the antiferromagnet

251 Given that pairing is usually mediated by ferromagnetic spin fluctuations, uranium-based heavy-fer

252 Exploiting an analogy with long-range ferromagnetic spin systems, we identified simple topolog

253 he decay of a non-singular spin texture in a ferromagnetic spin-1 Bose-Einstein condensate.

254 , N-doped graphene exhibited transition to a ferromagnetic state at approximately 69 K and displayed

255 ansition from an antiferromagnetic to a weak ferromagnetic state at filling factors near 0.6.

256 ical insulators such as Bi2Te3, a long-range ferromagnetic state can be established by chemical dopin

257 d giant negative magnetoresistance (~80%) in ferromagnetic state that will benefit potential spintron

258 rge densities, a spontaneous transition to a ferromagnetic state when [Formula: see text] surpasses 3

259 f a magnetar star may be a quark nugget in a ferromagnetic state with core magnetic field B(surface)

260 e low temperature high magnetic-field driven ferromagnetic state, a series of additional minima appea

261 ] film and decrease the magnetization of the ferromagnetic state, allowing rapid rewriting of the mag

262 disappearance of the volume fraction of the ferromagnetic state.

263 ns drive the twisted bilayer graphene into a ferromagnetic state.

264 ic structure in the ground state, via a pure ferromagnetic structure under the intermediate pressure,

265 and erasure of arbitrary shapes of thin-film ferromagnetic structures is reported.

266 llected that originated from both underlying ferromagnetic substrates and the organic films, with kin

267 Spin selectivity in photo-emission from ferromagnetic substrates functionalized with chiral orga

268 place UTe(2) at the paramagnetic end of this ferromagnetic superconductor series.

269 stability suggests that UTe(2) is related to ferromagnetic superconductors such as UGe(2), URhGe, and

270 c performance of a prototype (3.6 mm) of the ferromagnetic swimmer in fluids of different viscosity a

271 al verification of a new class of autonomous ferromagnetic swimming devices, actuated and controlled

272 and theoretical investigations on itinerant ferromagnetic systems under pressure have shown that fer

273 current can switch the magnetization of the ferromagnetic TBG near 3/4 filling as observed in the ex

274 s a promising multiferroic material but it's ferromagnetic TC is well below room temperature and the

275 Although the individual monolayer CrBr(3) is ferromagnetic, the interlayer coupling in bilayer depend

276 ing the three-dimensional magnetization in a ferromagnetic thin film heterostructure.

277 stimulate magnetization oscillations of the ferromagnetic thin film, which results in the radiation

278 n Seebeck effect (SSE) measured for metallic ferromagnetic thin films in commonly used longitudinal c

279 reversal symmetry) and chemical potential in ferromagnetic thin films of Cr-(Bi,Sb)2Te3 grown on SrTi

280 re we demonstrate magnetization switching of ferromagnetic thin layers that is induced solely by adso

281 netoelectric (ME) phenomena in piezoelectric/ferromagnetic thin-film bilayers are a promising paradig

282 Fe-containing frameworks, a transition from ferromagnetic to antiferromagnetic coupling between the

283 reased carrier density, leading to an exotic ferromagnetic to paramagnetic phase transition.

284 , where the gate voltage reversibly drives a ferromagnetic-to-paramagnetic phase transition.

285 y of the crystal structure of the thin-film, ferromagnetic topological insulator (Bi, Sb)2-x V x Te3.

286 Here, we show a reversible paramagnetic-to-ferromagnetic transformation of ferrofluid droplets by t

287 e report here a gate-controlled quantum Hall ferromagnetic transition between two real spin states in

288 istivity under pressure demonstrate that the ferromagnetic transition is continuously suppressed to z

289 wn that the approach to a continuous quantum ferromagnetic transition is typically interrupted by eit

290 onstruction leads to an antiferromagnetic to ferromagnetic transition, making them viable for spin fi

291 kinetic (Fermi) energy, leading to a (Bloch) ferromagnetic transition.

292 Quantum Hall ferromagnetic transitions are typically achieved by incr

293 that the observation of both structural and ferromagnetic transitions in the end members of the seri

294 Ferromagnetic van der Waals (vdW) insulators are of grea

295 ature is a hallmark of soft, two-dimensional ferromagnetic van der Waals crystals.

296 rromagnetic microwire coil that contains the ferromagnetic VSe(2) film subject to applied DC magnetic

297 modification via a weak magnetic field in a ferromagnetic Weyl semimetal candidate, Co(2)MnAl, at ro

298 [Formula: see text]S[Formula: see text] is a ferromagnetic Weyl semimetal that has been the subject o

299 Co(2)TiGe is one of the predicted ferromagnetic Weyl semimetals.

300 ich is comparable to conventional insulating ferromagnetic YIG films.