ライフサイエンスコーパス: ferromagnetism

1 actions drives the stabilization of the weak ferromagnetism.

2 ies on the intrinsic spin-orbit coupling and ferromagnetism.

3 s an element-specific probe of the origin of ferromagnetism.

4 i.e., a coexistence of ferroelectricity and ferromagnetism.

5 extent of hydrogenation, as well as exhibit ferromagnetism.

6 half-metallic, resulting in high-temperature ferromagnetism.

7 anence and routability of voltage-controlled ferromagnetism.

8 ondition for the observed itinerant electron ferromagnetism.

9 e chalcopyrites with excellent prospects for ferromagnetism.

10 ransforms the metastable phase and kills the ferromagnetism.

11 s that have previously been found to support ferromagnetism.

12 l help improve our understanding of metallic ferromagnetism.

13 culation that a "hidden" phase coexists with ferromagnetism.

14 fields toward quantum Hall spin and orbital ferromagnetism.

15 two-dimensional electron gas and interfacial ferromagnetism.

16 room-temperature ferroelectricity and 120 K ferromagnetism.

17 a function of magnetic field, a hallmark of ferromagnetism.

18 systems and processes, such as epidemics or ferromagnetism.

19 o several Tesla, suggesting valley (orbital) ferromagnetism.

20 nce, the occurrence of two-dimensional Ising ferromagnetism.

21 sm at room temperature, confirming intrinsic ferromagnetism.

22 result of charge transfer driven interfacial ferromagnetism.

23 possible mechanism for the origin of excited ferromagnetism.

24 q respectively), and showed room temperature ferromagnetism.

25 s, such as surface asperities for spines, or ferromagnetism.

26 planar Hall effect are deeply entwined with ferromagnetism.

27 the origin of the observed room temperature ferromagnetism.

28 cing the integration of ferroelectricity and ferromagnetism.

29 e) and show reversible voltage-driven ON-OFF ferromagnetism.

30 lation between the defects and the resulting ferromagnetism.

31 ct at zero magnetic field owing to intrinsic ferromagnetism(1-3).

32 te of quantum dots(4) to demonstrate Nagaoka ferromagnetism(5).

33 The recent discovery of ferromagnetism above room temperature in low-temperature

34 Its strong ferromagnetism above the room temperature enables the na

35 Trends in ferromagnetism across the 3d series of TM(2+):ZnO DMSs p

36 of the nematic order and field tuning of the ferromagnetism act as independent control parameters of

37 stabilized by quantum fluctuations, leaving ferromagnetism - along with the Kitaev spin liquid - as

38 We use neutron scattering to show that ferromagnetism and antiferromagnetism coexist in the low

39 th high Curie temperature (Tc), controllable ferromagnetism and easy integration with current Si tech

40 ng charge, spin, orbital, superconductivity, ferromagnetism and ferroelectricity.

41 this is likely caused by the coexistence of ferromagnetism and geometric frustration intrinsic to th

42 Ferromagnetism and its evolution in the orthorhombic per

43 emonstrated, which exhibits room temperature ferromagnetism and magnetoelectric (ME) coupling.

44 the effective electric-field control of both ferromagnetism and magnetoresistance in unique MnxGe1-x

45 agnetic codoping improves the homogeneity of ferromagnetism and modulates the surface band structure.

46 present direct evidence of hydrogen-mediated ferromagnetism and spin polarization in the conduction b

47 eates new opportunities for field control of ferromagnetism and spin-based quantum information proces

48 es determination of the relationship between ferromagnetism and structural distortion.

49 Ferromagnetism and superconductivity are two key ingredi

50 Adversely, ferromagnetism and superconductivity are typically also

51 owards understanding the competition between ferromagnetism and superconductivity in complex-oxide he

52 properties, especially the interplay between ferromagnetism and superconductivity in the ferromagnet/

53 The unusual coexistence of ferromagnetism and superconductivity is accompanied by a

54 A single material platform with concurrent ferromagnetism and superconductivity is actively pursued

55 The interplay between ferromagnetism and topological properties of electronic

56 will stimulate study of interaction between ferromagnetism and unconventional superconductivity.

57 magnet, and find the probable cause for the ferromagnetism and weak magnetization hysteresis in Fe-d

58 ombination with inversion symmetry breaking, ferromagnetism, and strong spin-orbit coupling contribut

59 elements (REEs), known for their brightness, ferromagnetism, and superconductivity, are essential in

60 ated the co-occurrence of superconductivity, ferromagnetism, and topological band structure in the ma

61 The ferromagnetism appears in isolated patches whose density

62 d material parameters for the control of the ferromagnetism are investigated, and the mechanism relat

63 Superconductivity and ferromagnetism are two antagonistic phenomena that combi

64 Its weak ferromagnetism arises from the canting of the antiferrom

65 he nickel d-states, which generally leads to ferromagnetism as is the case in metallic Ni.

66 DMSQDs are shown to exhibit room-temperature ferromagnetism, as expected from theoretical arguments.

67 (1.85)Sr(0.15)CuO(4) thin films develop weak ferromagnetism associated to the charge transfer of spin

68 Charge-transfer ferromagnetism assumes no essential role of dopant as a

69 ed Mn oxide by pulsed laser deposition shows ferromagnetism at low Zn concentration for an optimum ox

70 To this end, tunable ferromagnetism at room temperature and a thermally induc

71 wever, the ability to turn on and off robust ferromagnetism at room temperature and above has remaine

72 e extrinsic defects are eliminated, metallic ferromagnetism at room temperature can be stabilized in

73 Here we combine ferroelectricity and ferromagnetism at room temperature in a bulk perovskite

74 Polar corundum GaFeO3 exhibits weak ferromagnetism at room temperature that arises from its

75 thod for reversible, light-induced tuning of ferromagnetism at room temperature using a halide perovs

76 Our discovery opens another path to 2D ferromagnetism at room temperature with the advantage of

77 e presence of the copper at Zn sites induces ferromagnetism at room temperature, confirming intrinsic

78 ized even at ambient conditions, manifesting ferromagnetism at room temperature.

79 ultiferroic, exhibiting ferroelectricity and ferromagnetism at room temperature.

80 milar to that found in the 2D Ising model of ferromagnetism at the critical temperature.

81 the technological realm, with chirality- and ferromagnetism-based spin-tunable devices.

82 ctric and magnetic fields, we observe Stoner ferromagnetism below moire lattice filling one and Chern

83 ucidate the origins of the TM(n+):TiO(2) DMS ferromagnetism but also represent an advance toward the

84 simultaneously display ferroelectricity and ferromagnetism, but also enable magnetic moments to be i

85 rrelations persisted despite the presence of ferromagnetism, but the Kondo peak in the differential c

86 Monolayer Cr(2)Te(3) retains robust ferromagnetism, but with a suppressed Curie temperature,

87 Here, we discovered emergent ferromagnetism by interfacing non-magnetic WS(2) layers

88 We confirmed the high-temperature ferromagnetism by multiple characterizations.

89 It presents a rare example of a system where ferromagnetism can be induced by controlling the vacanci

90 Ferromagnetism can occur in wide-band gap semiconductors

91 ching the percolation limit, charge-transfer ferromagnetism can switch to a double exchange mechanism

92 d TMDs toward half-metallic room-temperature ferromagnetism character.

93 The presence of intrinsic ferromagnetism combined with strong spin-orbit coupling

94 reversal-symmetry-breaking characteristic of ferromagnetism, combined with the antiferromagnetic-like

95 enabled the discovery of superconductivity, ferromagnetism, correlated insulators, and a series of n

96 ates for the next generation of spintronics, ferromagnetism decays severely when the thickness is sca

97 al thin films also exhibits room temperature ferromagnetism deriving from the Fe doping Ga2O3.

98 , the core-shell particles exhibit increased ferromagnetism, despite the bulk diamagnetic properties

99 These defects are passivated and the ferromagnetism destroyed by further aerobic annealing.

100 Notably, the light-induced high-temperature ferromagnetism discovered in our work is metastable over

101 The discoveries of ferromagnetism down to the atomically thin limit in van

102 tice has been extensively studied to realize ferromagnetism due to its exotic flat band.

103 raphite oxide, however, pi electrons develop ferromagnetism due to the unique structure of the materi

104 Similar to HP-EuCo2As2, the itinerant 3d ferromagnetism emerges from electronic doping into the C

105 ce-level transport signatures of interfacial ferromagnetism emerging with superconducting states for

106 tomic scale and not so large as to eliminate ferromagnetism entirely.

107 Ferromagnetism exhibiting spontaneous spin alignment is

108 d is predicted to give rise to a Stoner-type ferromagnetism, experimental visualization of the magnet

109 The ferromagnetism extends ~2 nm into the Bi2Se3 from the in

110 An alternative to induce long-range ferromagnetism (FM) in TMDs is by introducing magnetic d

111 uctures have been discovered to show sizable ferromagnetism (FM) with the potential applications in s

112 Quenched ferromagnetism for N<4 superlattices is correlated to a

113 ractive interactions, and Stoner's itinerant ferromagnetism for repulsive interactions.

114 allows us to study the kinetics of emergent ferromagnetism from the femtosecond up to the nanosecond

115 Instead, we conclude that transfer of ferromagnetism from the ferromagnet to the Au or Pt take

116 FMIs are innately rare to find in nature as ferromagnetism generally accompanies metallicity.

117 This intrinsic ferromagnetism has also been identified by the splitting

118 y between antagonistic superconductivity and ferromagnetism has been a interesting playground to expl

119 or these applications, but the origin of its ferromagnetism has been controversial for several decade

120 Room temperature ferromagnetism has been observed in the Cu doped ZnO fil

121 tic oxide, 6H-BaTiO3-delta, room-temperature ferromagnetism has been previously reported.

122 The field of two-dimensional (2D) ferromagnetism has been proliferating over the past few

123 Electric-field manipulation of ferromagnetism has the potential for developing a new ge

124 lectricity, the electrostatic counterpart to ferromagnetism, has long been thought to be incompatible

125 This demonstration of Nagaoka ferromagnetism highlights that quantum simulators can be

126 ext], preceding the onset of the spontaneous ferromagnetism, implying that besides interaction, the r

127 Because ferromagnetism in (Ga,Mn)As is hole-mediated, the nature

128 ling reveals a primary contribution from the ferromagnetism in (Ga,Mn)As.

129 a new method for the robust manipulation of ferromagnetism in (Ga,Mn)As.

130 are closely linked to the strongly modified ferromagnetism in (LaMnO3+delta)N/(SrTiO3)N superlattice

131 e the dual nature of localized and itinerant ferromagnetism in 2D magnets.

132 r gadolinium atoms across IAEs, inducing the ferromagnetism in [Gd(2)C](2+).2e(-) electride.

133 Carrier-induced nature of ferromagnetism in a ferromagnetic semiconductor, (Ga,Mn)

134 ferromagnetism with gate voltage, and detect ferromagnetism in a non-conducting p-type sample.

135 vation of superconductivity on the border of ferromagnetism in a pure system, UGe2, which is known to

136 rently, the merge of altermagnetism and weak ferromagnetism in a single material excites significant

137 strate a giant intrinsic SHE coexisting with ferromagnetism in AB-stacked MoTe(2)/WSe(2) moire bilaye

138 Here we predict and rationalize robust ferromagnetism in an insulating oxide perovskite structu

139 Femtosecond laser excitation can induce ferromagnetism in antiferromagnetic FeRh, but the mechan

140 Additionally, the weak ferromagnetism in BiFeO3 films is largely changed in R-T

141 iS(2) parallels findings at the threshold of ferromagnetism in clean metallic systems, in which criti

142 etic oxides, we demonstrate room-temperature ferromagnetism in Co-doped graphene-like Zinc Oxide, a c

143 ental support for the existence of intrinsic ferromagnetism in cobalt-doped TiO(2), these results dem

144 Here, we report a thickness-dependent ferromagnetism in epitaxially grown Cr(2)Te(3) thin film

145 that features gate-tunable room-temperature ferromagnetism in few-layer device.

146 l valence-level energy range, indicates that ferromagnetism in Ga(1-x)Mn(x)As must be considered to a

147 ent current-induced switching of the surface ferromagnetism in hetero-bilayers consisting of the topo

148 l evidence of a new form of room-temperature ferromagnetism in high surface area nanocrystalline mang

149 thodology is reported for maintaining strong ferromagnetism in insulating LaCoO(3) (LCO) layers down

150 s been long predicted to bolster the surface ferromagnetism in magnetic topological insulators (MTIs)

151 f which are standard signatures of itinerant ferromagnetism in metals.

152 The occurrence of ferromagnetism in Mn(2+):ZnO and its dependence on synth

153 Room-temperature ferromagnetism in Mn-doped chalcopyrites is a desire asp

154 The discovery of ferromagnetism in Mn-doped GaAs has ignited interest in

155 Antisite-stabilized spin-flipping induces ferromagnetism in MnPt films, although it is robustly an

156 e demonstration of electric-field control of ferromagnetism in MOS ferromagnetic capacitors up to 100

157 otations as routes to enhancing induced weak ferromagnetism in multiferroic oxides.

158 of the coexistence of superconductivity and ferromagnetism in one two-dimensional nanomaterial.

159 Enhancing ferromagnetism in semiconductors requires us to understa

160 ined by either of the two dominant models of ferromagnetism in semiconductors.

161 ent discovery of the strong room temperature ferromagnetism in single layers of VSe(2) grown on graph

162 lps unveil the mechanism of carrier-mediated ferromagnetism in spintronic materials.

163 nation of relativistic fermion behaviour and ferromagnetism in Sr1-yMn1-zSb2 offers a rare opportunit

164 e unexpected evolution from high-temperature ferromagnetism in SrRuO3 to low-temperature superconduct

165 nfluence on ferroelectricity in bulk STO and ferromagnetism in STO-based heterostructures.

166 understanding of the microscopic origins of ferromagnetism in such materials.

167 le of internal strain in establishing defect ferromagnetism in systems with competing structural phas

168 An enhanced ferromagnetism in the h-CBN emerges due to the spin pola

169 nd magnetization studies have shown signs of ferromagnetism in the LaAlO3/SrTiO3 heterostructure, an

170 perconductivity adjoining itinerant-electron ferromagnetism in the phase diagram has for many years c

171 This result reveals not only that the ferromagnetism in the ruthenates is extremely sensitive

172 g, probably associated with the formation of ferromagnetism in the surface layer.

173 Enhancing ferromagnetism in these semiconductors not only represen

174 The plausible origin of ferromagnetism in these Te-doped GaAsSb nanowires is dis

175 To explain the origin of ferromagnetism in these ZrO2 nanostructures, we hypothes

176 strates the existence of intrinsic high-T(C) ferromagnetism in this class of DMSs.

177 ependent spin-momentum locking coexists with ferromagnetism in this material, a cohabitation that pro

178 d thin-film studies, we demonstrate that the ferromagnetism in this system originates in a metastable

179 amous double exchange, the main mechanism of ferromagnetism in transition metal compounds.

180 ve phenomena such as charge transfer gap and ferromagnetism in two dimensions; however, the experimen

181 se of surface molecular adsorption to induce ferromagnetism in two-dimensional superconducting NbSe2,

182 The recent discovery of ferromagnetism in two-dimensional van der Waals crystals

183 upon octahedral tilting, resulting in robust ferromagnetism in ultrathin cobaltites.

184 The discovery of intrinsic ferromagnetism in ultrathin two-dimensional van der Waal

185 Discoveries of room-temperature ferromagnetism in wide-bandgap DMSs hold great promise,

186 The ferromagnetism in WTe(2) manifests in the anomalous Nern

187 oximity effect between superconductivity and ferromagnetism in YBCO/LCMO heterostructures.

188 ed to enhance and stabilize high-temperature ferromagnetism in YTiO(3), a material that shows only pa

189 the layered polymorph of GdAlSi demonstrates ferromagnetism, in contrast to the nonlayered, tetragona

190 The observed ferromagnetism increases with decreasing constituent nan

191 f different oxidation states is the basis of ferromagnetism induced by Stoner splitting of the local

192 d our data validate the most basic model for ferromagnetism introduced by Stoner.

193 a magnetic material, local on/off control of ferromagnetism is achieved using a global voltage bias a

194 The transition from antiferromagentism to ferromagnetism is attributed to atomic-scale disorder in

195 The origin of the ferromagnetism is attributed to the trivalent Sm dopant,

196 re of the layered manganite, and the loss of ferromagnetism is attributed to weakened double exchange

197 Ferromagnetism is broadly accepted as an intrinsic prope

198 Our conclusion of interfacial ferromagnetism is confirmed by the presence of a hystere

199 The most important factor for activating ferromagnetism is found to be the creation of grain boun

200 Homogeneity in ferromagnetism is found to be the key to high-temperatur

201 The ferromagnetism is further supported by electron transpor

202 BiFeO3, we are able to show that a metallic ferromagnetism is induced near the interface.

203 n is substantially deficient at x = 0.26 and ferromagnetism is maintained with a T(c) of approximatel

204 Ferromagnetism is most common in transition metal compou

205 In contrast, unexpected ferromagnetism is observed in tensile-strained LaCoO(3)

206 Surprisingly, strong ferromagnetism is observed with T(c) = 223 K.

207 mic scale understanding of LMO/STO ambipolar ferromagnetism is offered by quantifying the interface c

208 s achieved at low temperatures and transient ferromagnetism is realized up to T(neq) > 80 K, nearly t

209 Here the discovery of ferromagnetism is reported in a layered van der Waals se

210 y, a rigorous theoretical basis for metallic ferromagnetism is still largely missing.

211 Thus, the ferromagnetism is traced down to its microscopic electro

212 Ferromagnetism is usually deemed incompatible with super

213 ly, the coexistence of superconductivity and ferromagnetism is usually observed only in elegantly des

214 tor Cr(0.32)Ga(0.68)Te(2.33), with intrinsic ferromagnetism, is a possible candidate for bulk ferrova

215 exhibit robust high-Curie-temperature (T(C)) ferromagnetism (M(s)(300 K) = 0.8 mu(B)/Ni(2+), T(C) >>

216 So far, electric-field control of ferromagnetism, magnetization and magnetic anisotropy ha

217 ile, however, unveils the characteristics of ferromagnetism, marked by a substantial magnetic retenti

218 This propensity for ferromagnetism may account for much of the unexplained b

219 tinct from the well-known half-metallic Weyl ferromagnetism observed in the bulk counterpart.

220 ect, whereas in trilayer CrI3 the interlayer ferromagnetism observed in the bulk crystal is restored.

221 interaction, also at the origin of the weak ferromagnetism of bulk cuprates, propagates the magnetis

222 Our observations imply that itinerant ferromagnetism of delocalized fermions is possible witho

223 The strong ferromagnetism of Eu coexists with the pressure-induced

224 electric fields to a MOS gate structure, the ferromagnetism of the channel layer can be effectively m

225 ic structures and polarity-dependent high-TC ferromagnetism of TM(2+):ZnO DMSs, where TM(2+) denotes

226 ependence of magnetic interaction leading to ferromagnetism on the carrier density is shown.

227 ing in the Fraunhofer patterns pinpoints the ferromagnetism on the junction interface.

228 g that it may be possible to switch the weak ferromagnetism "on" and "off" under the application of s

229 of 2D FM CrTe(2) films with room-temperature ferromagnetism opens a new avenue for developing large-s

230 l time-reversal symmetry breaking (e.g., via ferromagnetism) or with a combination of spin-orbit inte

231 es, structural domains, ferroelectricity, or ferromagnetism-or a much more common property of insulat

232 ent a broad opportunity to tailor intriguing ferromagnetism originating from quasi-atomic interstitia

233 Sr(1-y)Ba(y)RuO3 makes it possible to study ferromagnetism over a broader phase diagram, which inclu

234 The ferromagnetism persists up to approximately 980 K, and f

235 This interfacial ferromagnetism persists up to room temperature, even tho

236 erature superconductivity, ferroelectricity, ferromagnetism, piezoelectricity and semiconductivity.

237 The itinerant ferromagnetism proceeds through a double-exchange mechan

238 wo-dimensional (2D) materials with intrinsic ferromagnetism provide unique opportunity to engineer ne

239 xhibiting emergent properties including anti-ferromagnetism, purely magnetic-based Fano resonances, a

240 de-bandgap DMSs hold great promise, but this ferromagnetism remains poorly understood.

241 ch phases of matter, such as spin liquid and ferromagnetism, resulting from strong electron correlati

242 The suppression/recovery of interfacial ferromagnetism results from the asymmetric effect that i

243 that, within the phase space showing robust ferromagnetism, rho is near unity for Fermi liquid state

244 in a limited pressure range on the border of ferromagnetism, seems to arise from the same electrons t

245 The emergence of interfacial ferromagnetism should have implications to electronic an

246 Furthermore, the samples (x = 0.1-0.7) with ferromagnetism show magnetoelectric coupling effects at

247 nanowires is discussed on the basis of d(0) ferromagnetism, spin ordering of the Te dopants and the

248 d, EuTiO(3), was predicted to exhibit strong ferromagnetism (spontaneous magnetization, approximately

249 to homogeneous strain is too small to induce ferromagnetism, suggesting a dominant role for strain gr

250 emergent organized behavior (crystallinity, ferromagnetism, superconductivity, etc.) at long wavelen

251 sics, underpinning such diverse phenomena as ferromagnetism, superconductivity, superfluidity and the

252 nanoscale quantum imaging of low-dimensional ferromagnetism sustained in Fe(3)GeTe(2)/hBN van der Waa

253 harge density waves, superconductivity, hard ferromagnetism) that may be tuned by composition, pressu

254 antiferromagnetism could be converted to 2D ferromagnetism, the range of 2D magnets and their potent

255 patial control over electronic bandwidth and ferromagnetism through the creation of octahedral supers

256 etic properties: we show that the trend from ferromagnetism to incommensurate ordering as atomic numb

257 ition of permanent magnet nanoparticles from ferromagnetism to paramagnetism provides an effective ap

258 c transition of BaFe12O19 nanoparticles from ferromagnetism to paramagnetism.

259 Here we employ the phenomenon of itinerant ferromagnetism to realize magnetic ordering at T(C) = 22

260 The observed ferromagnetism upon doping arises from a Dirac (valence)

261 the controlled manipulation of high-T(C) DMS ferromagnetism using external chemical perturbations.

262 te to revealing the origin of defect-induced ferromagnetism using SiC as a prototypical example.

263 c fingerprint of bulk metallic character and ferromagnetism versus depth.

264 No evidence of macroscopic ferromagnetism was found in SQUID magnetometry.

265 o, while bulk SmMnO(3) is antiferromagnetic, ferromagnetism was induced in the composite films.

266 Robust ferromagnetism was observed in spin-coated thin films of

267 antum anomalous Hall effect with spontaneous ferromagnetism was observed in twisted bilayer graphenes

268 ontrary to previous reports, no evidence for ferromagnetism was observed.

269 tail behaviour, whereas for c/a < 0.99 clear ferromagnetism was observed.

270 In this work, reversible control of ferromagnetism was realized by the guided motion of Li-i

271 at orbital ordering may be the origin of the ferromagnetism we observe in this material.

272 etic as colloids but showed room-temperature ferromagnetism when spin-coated aerobically into films.

273 dicate the presence of novel two-dimensional ferromagnetism with a complicated magnetic domain dynami

274 Intrinsic ferromagnetism with a Curie temperature (T(C)) up to 300

275 These nanosheets exhibit robust ferromagnetism with a Curie temperature of ~100 K and re

276 port an approach to control and switch local ferromagnetism with an electric field using multiferroic

277 ts reveal the possibility to locally control ferromagnetism with an electric field.

278 We observe no change in ferromagnetism with gate voltage, and detect ferromagnet

279 nhancement and suppression, respectively, of ferromagnetism with modulation of the Curie temperature

280 Ferromagnetism with T(C) > 350 K is observed in aggregat

281 strate room temperature ferroelectricity and ferromagnetism with T(C,FM) ~ 90 K, matching exactly wit

282 nce of high n-type electrical conduction and ferromagnetism with Tc approximately 450 K.

283 d structure, the compound exhibits itinerant ferromagnetism, with the ordering temperature of 307 K.

284 sites represent the first instance of strong ferromagnetism within a Kagome layered framework.