ライフサイエンスコーパス: magnetism

1 n spectrum resulting in an intricate nuclear magnetism.

2 ry are at the heart of advances in molecular magnetism.

3 el for the study of geometrically frustrated magnetism.

4 ng application in the field of environmental magnetism.

5 gonal forms of FeS and FeSe display a robust magnetism.

6 ee text] is a consequence of this multiphase magnetism.

7 unconventional superconductivity and quantum magnetism.

8 atterns, is the key to advancing topological magnetism.

9 on is thus inextricably tied to photoinduced magnetism.

10 strong coupling between ferroelectricity and magnetism.

11 ing on the competition between covalency and magnetism.

12 arriers with other quantum phenomena such as magnetism.

13 is work with strong electric field tuning of magnetism.

14 ilms and could open new prospects in surface magnetism.

15 irements for displacive ferroelectricity and magnetism.

16 exhibiting different scenarios of all-carbon magnetism.

17 ory devices in which electric fields control magnetism.

18 e relationship between superconductivity and magnetism.

19 r understanding of nanoscale and interfacial magnetism.

20 eat, but are not classically associated with magnetism.

21 mic closely its unusually rich field-induced magnetism.

22 uing phenomena such as superconductivity and magnetism.

23 o use polarized light to alter or manipulate magnetism.

24 exchange and leading to strongly frustrated magnetism.

25 ism for the origins of both conductivity and magnetism.

26 cles' mass generation, superconductivity and magnetism.

27 y, (semi)conductivity, ferroelectricity, and magnetism.

28 assive stars, their X-ray emission and their magnetism.

29 Ti-on-Al antisite defects lead to interface magnetism.

30 per pairing is indeed mediated by f-electron magnetism.

31 ew window into the mechanisms behind surface magnetism.

32 ation for further exploration of topological magnetism.

33 ge state induced by broken TRS through local magnetism.

34 ted to the unusual behaviour observed in the magnetism.

35 ram and a logarithmic time dependence of the magnetism.

36 ellent system for studies of low-dimensional magnetism.

37 a in solids, including superconductivity and magnetism.

38 ith respect to the potential for anisotropic magnetism.

39 urge of both pure and applied research in 2D magnetism.

40 o complex networks exhibiting strong visible magnetism.

41 uperconductivity, spin-orbit interaction and magnetism.

42 also have applications in studying nanoscale magnetism(2,3) and the quantum geometric phase(11).

43 are also widely used in studying small-scale magnetism(2,3), the Casimir effect(4) and other applicat

44 This includes superconductivity(1,2), magnetism(3), topological edge states(4,5), exciton trap

45 phenomena including superconductivity(1-3), magnetism(4), fractional Chern insulating states(5) and

46 mation of moire excitons(3-8) and interlayer magnetism(9).

47 8) of Hamiltonians for quantum chemistry and magnetism(9).

48 ic material by mitigating Brown's paradox in magnetism, a substantial reduction of coercivity from th

49 The interplay of light and magnetism allowed light to be used as a probe of magneti

50 itz-Thouless phase transition, and classical magnetism, among the many systems that are described by

51 roach by applying it to a problem of quantum magnetism, an antiferromagnetic Heisenberg model in an e

52 tant role in areas as diverse as metallurgy, magnetism and biology as well as in chemical application

53 ssible benefits in potential applications in magnetism and catalysis.

54 This underlines the sensitivity of the magnetism and chemistry of these mixed-valent systems to

55 ting phenomena arising from the interplay of magnetism and chirality.

56 ysis, optical and photocatalysis, as well as magnetism and conclude the review by addressing the pros

57 ocrystals in terms of catalysis, optics, and magnetism and conclude the Review by highlighting applic

58 ave always been one of the central topics of magnetism and condensed matter science.

59 We report the magnetism and conductivity for a redox pair of iron-quin

60 We report on a strong correlation between magnetism and conductivity in the iodine-bonded molecula

61 The interplay between magnetism and crystal structures in three CaFe2As2 sampl

62 ingly, we observe strong optically activated magnetism and diluted magnetic semiconductor behaviour,

63 ults hinges on the possibility to manipulate magnetism and electronic band topology by external pertu

64 r parameters coexist, enable manipulation of magnetism and electronic properties by external electric

65 de new insights into fundamental problems of magnetism and exciting potentials for novel magnetic tec

66 rconductivity and giant magnetoresistance to magnetism and ferroelectricity.

67 ng from electrical and ionic conductivity to magnetism and ferroelectricity.

68 tes with interesting properties that include magnetism and high electrical conductivity.

69 line materials upon suitable balance between magnetism and hydrodynamics.

70 IONPs such as colloidal stability, toxicity, magnetism and labelling efficiency.

71 puzzle, a result of strong coupling between magnetism and lattice vibrations.

72 s (IO)-graphene oxide (GO) with tunable core magnetism and magnetic resonance transverse relaxivity (

73 recise understanding of the coupling between magnetism and microstructure is essential for enhancing

74 r findings suggest that the SOPs can enhance magnetism and more robust time-reversal-symmetry-breakin

75 of charge-transfer complex system where the magnetism and optoelectronics interact.

76 enue for the nonvolatile tuning of SOC based magnetism and spintronic effects, but also helps to clar

77 3.2) as well as the phase separation between magnetism and superconductivity point to a conventional

78 Strong electronic correlations, such as magnetism and superconductivity, can be produced as the

79 In the present work the suppression of magnetism and the occurrence of superconductivity in CrA

80 ibes advances in the area of single-molecule magnetism, and 5) summarizes the coordination and activa

81 f an iron oxide core that provides color and magnetism, and a Janus coating that provides biospecific

82 d single-site starting point for considering magnetism, and can lead to a qualitatively new behavior.

83 mena, such as superconductivity, pseudo-gap, magnetism, and density waves.

84 related phenomena such as superconductivity, magnetism, and ferroelectricity have yet to be developed

85 ied physical properties, including band gap, magnetism, and porosity, with hierarchical micro/mesopor

86 ick model(25,26), an iconic model in quantum magnetism, and report the observation of distinct dynami

87 c characterizations on electrical transport, magnetism, and scanning tunneling spectroscopy.

88 cluding orbitals, fluctuating local moments, magnetism, and the crystal structure, have resisted pred

89 in-plane length scale over which charge and magnetism are correlated in (La0.4Pr0.6)1-xCaxMnO3 films

90 n these materials, both ferroelectricity and magnetism are coupled to an additional, non-ferroelectri

91 static optics', in which the electricity and magnetism are decoupled, while the fields are temporally

92 ich can harbour both strong correlations and magnetism, are considered ideal candidates for realizing

93 antum wells-such as 2D superconductivity and magnetism-are intimately connected to specific orbital s

94 We show that this strong magnetism arises from a van Hove singularity associated

95 of mutant Ft proteins indicate that improved magnetism arises in part from increased iron oxide nucle

96 The nature of magnetism arises mainly from the B-site Fe exhibiting a

97 Using magnetism as a fingerprint of the transformation process

98 on-limited imaging of both stress fields and magnetism as a function of pressure and temperature.

99 togalvanic effect (MPGE) that introduces the magnetism as a key ingredient and induces a giant BPVE.

100 enge that must be overcome to establish soil magnetism as a trusted paleoenvironmental tool.

101 slabs, along with the quantum nature of the magnetism associated with V(4+) , means that these mater

102 m, enabling direct electric-field control of magnetism at 200 kelvin.

103 al-free magnetic material that would exhibit magnetism at a higher temperature with an excellent spin

104 ducing and controlling both conductivity and magnetism at general polar-nonpolar interfaces.

105 c semiconductors possessing intrinsic static magnetism at high temperatures represent a promising cla

106 nterrelation between octahedral rotation and magnetism at interface is scarce.

107 rt by the discovery of superconductivity and magnetism at interfaces between SrTiO3 and other non-mag

108 posed and implemented to generate artificial magnetism at optical frequencies using plasmonic metamat

109 esearch for energy-efficient manipulation of magnetism at smaller and smaller length scales.

110 ts from first-principles calculations on the magnetism at the BiFeO3/YBa2Cu3O7 interfaces.

111 However, selective measurement of induced magnetism at the buried interface has remained a challen

112 y is crucial for the creation and control of magnetism at the interface between non-magnetic ABO(3)-p

113 The search for novel tools to control magnetism at the nanoscale is crucial for the developmen

114 Our findings not only allow characterizing magnetism at the TI-FMI interface but also lay the groun

115 Here, we report a new type of magnetism-based nanoscale distance-dependent phenomenon

116 ge ground state spin values, single-molecule magnetism behaviour or impressively large magnetocaloric

117 measurements revealed a large difference in magnetism between oxygenated and deoxygenated forms of t

118 or understanding physical properties such as magnetism, but technically challenging due to the small

119 orm to magnetic Ti(3+) with quenched orbital magnetism, but the concentration is anomalously low.

120 demonstrate topologically enhanced interface magnetism by coupling a ferromagnetic insulator (EuS) to

121 Manipulating magnetism by electric current is of great interest for b

122 oelectric materials were employed to control magnetism by electric fields in multiferroic heterostruc

123 This work creates opportunities for studying magnetism by harnessing the unusual features of atomical

124 magnetism, which enables the tuning of their magnetism by systematic nanoscale engineering.

125 on top for which novel phenomena related to magnetism can be anticipated.

126 allization and localized Co(2+) -3d low-spin magnetism can coexist prior to the full 3d-electron delo

127 t for practical applications in spintronics, magnetism, catalysis and medicine.

128 a variety of distinct ground states, such as magnetism, charge order or superconductivity.

129 Thus, the weak short-range magnetism combined with the nearly ideal honeycomb struc

130 exposure, along with abiotic properties like magnetism, conductivity, and multifluorescence.

131 In magnetism, correlated states such as spin ice and the sp

132 The magnetism correlates intimately with the Fe(2+)/Fe(3+) r

133 oxide with well-controlled phase and tunable magnetism demonstrated in this work provides a promising

134 gy spin-polarized muons, we find that static magnetism disappears close to where superconductivity be

135 As the ratio increases, the weak magnetism displayed by unordered magnetic moments intens

136 Solar magnetism displays a host of variational timescales of w

137 romising architecture with induced unnatural magnetism, especially at visible frequencies.

138 l properties such as band-gap, conductivity, magnetism, etc.

139 dynamical behaviors.Exploring unconventional magnetism facilities both fundamental understanding of m

140 onstrates that juvenile eels use the Earth's magnetism for their dispersal, with possible implication

141 ns, the role of strain in voltage-controlled magnetism for these BiFeO3-based heterostructures.

142 with various forms of inhomogeneous barrier magnetism, Fraunhofer patterns are increasingly complex.

143 secondary variability is driven by surges of magnetism from the activity bands.

144 This review charts progress in molecular magnetism from the perspective of ligands in which the d

145 -magnetized iron garnets, rare-earth orbital magnetism gives rise to an intrinsic spin-orbit coupling

146 rstanding of how the interplay of motion and magnetism gives rise to new states of matter.

147 This form of itinerant magnetism has been rigorously studied theoretically(6-9)

148 rstanding of the relationship between Hb and magnetism has enabled the quantitative measurement of th

149 liquid behavior isolated from the border of magnetism has long been speculated, no experimental conf

150 Electric-field control of magnetism has remained a major challenge which would gre

151 croscopy, quantum-chemical calculations, and magnetism has shed light on the intrinsic features of th

152 r, no two-dimensional crystal with intrinsic magnetism has yet been discovered; such a crystal would

153 ligand types, small-molecule activation, and magnetism have been reported.

154 emergent conductivity, superconductivity and magnetism have helped to fuel intense interest in the ri

155 c and surface chemistry as well as molecular magnetism illustrate the points made.

156 restrictions for achieving a full control of magnetism in an extensive operational dynamic range, lim

157 On the other hand, manipulation of magnetism in antiferromagnetic (AFM) based nanojunctions

158 route towards the ultrafast manipulation of magnetism in antiferromagnetic spintronics.

159 The resulting zero net magnetic moment makes magnetism in antiferromagnets externally invisible.

160 The recent discovery of magnetism in atomically thin layers of van der Waals cry

161 d by a series of prominent reports regarding magnetism in biological systems.

162 The discovery of magnetism in carbon structures containing zigzag edges h

163 However, chiral magnetism in centrosymmetric oxides has not yet been obs

164 studies of previously inaccessible nanoscale magnetism in condensed-matter systems.

165 uB/Fe), this provides a picture of itinerant magnetism in CuFe2Ge2.

166 The rings are hence ideal for understanding magnetism in elegant exchange-coupled systems.

167 ffects of hydrostatic pressure on the static magnetism in Eu(Fe0.925Co0.075)2As2 are investigated by

168 Voltage control of magnetism in ferromagnetic semiconductor has emerged as

169 er spectroscopy, we show that nematicity and magnetism in FeSe under applied pressure are indeed stro

170 rge transport, metal-insulator crossover and magnetism in field-effect devices based on ionically gat

171 ular to heterostructures) voltage controlled magnetism in heterostructures consisting of CoFe nanodot

172 and provides novel insights into anisotropic magnetism in iridates.

173 state characterized by the absence of static magnetism in its ground state.

174 critical insights into the origins of chiral magnetism in low-damping magnetic oxides and identify pa

175 Voltage-modulated magnetism in magnetic/BiFeO3 heterostructures can be dri

176 at this same pressure, we show here that the magnetism in metallic GdSi remains completely robust eve

177 The origin of magnetism in metals has been traditionally discussed in

178 ions, electronic structures, and introducing magnetism in non-magnetic materials.

179 e in the field of electrical manipulation of magnetism in numerous material systems.

180 Magnetism in plutonium has been debated intensely, but t

181 The lack of magnetism in PuCoGa5 has made it difficult to reconcile

182 se to unusual forms of superconductivity and magnetism in quantum many-body systems.

183 findings reveal previously hidden aspects of magnetism in Sm-Co magnets and, by identifying weak poin

184 ntally and theoretically, the development of magnetism in Tb clusters from the atomic limit, adding o

185 Mutual control of the electricity and magnetism in terms of magnetic (H) and electric (E) fiel

186 Here we investigate magnetism in the Na filled Fe-based skutterudites using

187 e, we observed stacking-dependent interlayer magnetism in the two-dimensional (2D) magnetic semicondu

188 ce microscopy to search for room-temperature magnetism in the well-studied LaAlO3/SrTiO3 system.

189 ns to uncover the origin of high-temperature magnetism in these superlattices and the charge-ordering

190 Magnetism in transition metal compounds is usually consi

191 ion measurements and demonstrate contrasting magnetism in two of the phases, Am = GUA and FA, that ar

192 s, and we determine the defect structure and magnetism in Y2Ti2O7-delta using diffuse neutron scatter

193 (e.g., density, electrical conductivity, and magnetism) in bismuth could be due to the formation of t

194 -1200 degrees C, and low values of remanent magnetism indicate the meltglass was not created by ligh

195 The magnetism induced at the interface resulting from the la

196 The MPGE emerges from the magnetism-induced asymmetry of the carrier velocity in t

197 Molecular quantum magnetism involving an isolated spin state is of particu

198 here is a rich interplay between phonons and magnetism involving both magnetoelastic and magnetostric

199 The interplay of superconductivity and magnetism is a subject of ongoing interest, stimulated m

200 n group chemistry at the interface molecular magnetism is an area with huge potential to deliver new

201 with theoretical results, the strain-tunable magnetism is attributed to the sensitive change of magne

202 Uranium(IV) 5f(2) magnetism is dominated by a transition from a triplet to

203 cularly suitable in the regime where quantum magnetism is expected.

204 The magnetism is found to be more suppressed for the La0.67C

205 We show that magnetism is globally absent in the new phase, as low-sp

206 With the processed samples, d(0) magnetism is realized and negative magnetoresistance is

207 hown to involve solely Os-O interactions and magnetism is revealed as the driving microscopic mechani

208 lizing non-volatile, E-field manipulation of magnetism lies in finding an energy efficient means to s

209 nes or responsive elements (e.g. ultrasound, magnetism, light) to deliver its cargo within a local re

210 effects in superconductivity, superfluidity, magnetism, liquid crystals, and plasticity of solids.

211 our previous theoretical prediction of block magnetism (magnetic order of the form [Formula: see text

212 le of a material where superconductivity and magnetism may be intertwined.

213 eir potential existence on Mercury and their magnetism may contribute to its present magnetic field.

214 Magnetism may increase or decrease with pressure, depend

215 s chemistry include, but are not limited to, magnetism, melting point, hydrophobicity, fluorescence q

216 on Mars where striking evidence for remnant magnetism might suggest an early phase of crustal spread

217 applications in diverse fields such organic magnetism, MRI contrast agents, and spintronics.

218 n of a singlet ground state magnet, in which magnetism occurs through a process that resembles excito

219 Elucidating the nature of the magnetism of a high-temperature superconductor is crucia

220 Inspired by the natural magnetism of aromatic molecules, the cyclic ring cluster

221 We report on the magnetism of charge-stripe ordered La(2)NiO(4.11+/-0.01)

222 as In(2)Se(3) reverses its polarization, the magnetism of Cr(2)Ge(2)Te(6) is switched, and correspond

223 are essential to quantitatively describe the magnetism of CrI(3) but quantum rescaling corrections ar

224 w how this 5f-6d hybridization regulates the magnetism of each sublattice in UCu2Si2 and UMn2Si2 comp

225 istic field perturbation due to the inherent magnetism of electrochemical materials.

226 The magnetism of Fe2MnAl and Mn2FeAl compounds are studied b

227 e demonstrate the reading and writing of the magnetism of individual Ho atoms on MgO, and show that t

228 In this work, an investigation of the magnetism of micromechanically cleaved CrCl(3) flakes wi

229 vative core-shell nanocarrier, combining the magnetism of surface active maghemite nanoparticles (SAM

230 As the magnetism of the Fe d-orbitals is intertwined with the s

231 esults demonstrate that the intricate static magnetism of the hexagonal phase is not intrinsic, but r

232 The high surface area and magnetism of the particles makes them ideal building blo

233 rization that exceeds that stemming from the magnetism of these chains.

234 The reactivity and magnetism of these compounds are discussed in the contex

235 of 3d transition metals in the Earth's core, magnetism of these materials in their dense phases has b

236 The control of the magnetism of ultra-thin ferromagnetic layers using an el

237 e of proximity-induced superconductivity and magnetism on the helical hinge states of bismuth(111) fi

238 er in the FeAs layers, without either static magnetism or broken C 4 symmetry, while suppressing the

239 avor new and subtle forms of matter, such as magnetism or superconductivity, they can even cause the

240 Magnetism, originating from the moving charges and spin

241 ) spin chain is the Drosophila of frustrated magnetism, our understanding of a pair of coupled zigzag

242 ferromagnetic behavior with the easy axis of magnetism perpendicular to the longitudinal axis of the

243 (2) , featuring both charge density wave and magnetism phenomena, represents a unique van der Waals m

244 esirability of continued interchange between magnetism physics and neurobiology.

245 understood and the role of proximity induced magnetism (PIM) in the heavy metal is unknown.

246 Electrical manipulation of magnetism presents a promising way towards using the spi

247 , i.e., frustrated, interactions can display magnetism prolific in intricate structures, discrete jum

248 ir intriguing structural characteristics and magnetism properties that attract the interest of synthe

249 Electric field control of magnetism provides a promising route towards ultralow po

250 e ions display unique characteristics (i.e., magnetism, radioactivity, and luminescence), often with

251 Here we report the molecular quantum magnetism realized in an inorganic solid Ba3Yb2Zn5O11 wi

252 nues to realise it, however, their interface magnetism remains an open question up to this day.

253 The magnetism remains bulk up to p approximately 3.5 kbar wh

254 fort, a full understanding of all-in-all-out magnetism remains elusive as the associated magnetic exc

255 The field of single molecule magnetism remains predicated on super- and double exchan

256 Taking advantage of the magnetism, remotely triggered drug release was facilitat

257 Pushing the frontiers of condensed-matter magnetism requires the development of tools that provide

258 ne of the most challenging topics in today's magnetism research.

259 that lead to significantly enhanced cellular magnetism, resulting in increased physical attraction of

260 ogical considerations for ESR as pertains to magnetism, sample preparation and proper incubation time

261 ion since the first detailed observations of magnetism several hundred years ago.

262 h dominant direct exchange and non-collinear magnetism show surprisingly large IXS cross-section for

263 e of the neutral cluster, itinerant electron magnetism similar to that in metallic ferromagnets.

264 of the most extensively studied phenomena in magnetism, since it exerts a unidirectional anisotropy t

265 bit rich emergent properties such as unusual magnetism, superconductivity and heavy fermion behaviour

266 important for developments in fields such as magnetism, superconductivity, photonics and electronics.

267 f the applied non-magnetic potentials and/or magnetism switching.

268 In magnetism, systems incorporating geometrical frustration

269 Here we discover chiral magnetism that allows for pure spin-current-driven domai

270 Owing to the interfacial nature of the magnetism, the ability to move oxygen vacancies within t

271 provide ideal platforms for understanding 2D magnetism, the control of which has been fueling opportu

272 uple perovskite BiMn(7)O(12) In analogy with magnetism, the electric dipole helicoidal texture is sta

273 In magnetism, the topology of spin order manifests itself i

274 When coupled to magnetism, they become so-called multiferroic systems, a

275 ayer across the heterointerface and modulate magnetism through magnetoelastic coupling.

276 n addressed theoretically, and triggering of magnetism through N-doping has not yet been proved exper

277 Controlling magnetism through non-magnetic means is highly desirable

278 Magnetism thus deploys an authentic myogenic directive t

279 rbon nanocones are conducting and can induce magnetism, thus opening new avenues on the exploitation

280 e an important class of materials that allow magnetism to be manipulated through the application of e

281 This allows magnetism to couple to phonons on an unprecedented scale

282 lous Hall (QAH) effect combines topology and magnetism to produce precisely quantized Hall resistance

283 in zero field as p(c) is approached, we find magnetism to strengthen under strong magnetic fields due

284 gy conversion/storage, nano-composites, nano-magnetism, to nano-optics.

285 uantum spin liquid with no detectable static magnetism together with the presence of diffuse continua

286 Magnetism typically arises from the joint effect of Ferm

287 Electric field control of magnetism ultimately opens up the possibility of reducin

288 her provide crucial insight into controlling magnetism via magneto-ionic motion, both at interfaces a

289 probed the non-equilibrium two-orbital SU(N) magnetism via Ramsey spectroscopy of atoms confined in a

290 the recent observation of plutonium dynamic magnetism, we construct a theory for plutonium that agre

291 portunities to study novel phenomena such as magnetism which broadens the range of their applications

292 st intriguing properties is the emergence of magnetism which is sensitive to chemical defects.

293 the bulk magnet, magnetic NPs exhibit unique magnetism, which enables the tuning of their magnetism b

294 nt problem in many-body physics is itinerant magnetism, which originates purely from long-range inter

295 tors, FeSe exhibits nematic ordering without magnetism whose relationship with its superconductivity

296 l of multiferroics is the ability to control magnetism with electric field.

297 As a result, controlling spin magnetism with electric fields-a longstanding technologi

298 ent a platform for the simulation of quantum magnetism with full control of interactions between pair

299 bservations pave the way for manipulating 2D magnetism with layer twist angle control.

300 The recent discovery of magnetism within the family of exfoliatable van der Waal