ライフサイエンスコーパス: magnetism

1 el for the study of geometrically frustrated magnetism.

2 ory devices in which electric fields control magnetism.

3 e relationship between superconductivity and magnetism.

4 r understanding of nanoscale and interfacial magnetism.

5 eat, but are not classically associated with magnetism.

6 mic closely its unusually rich field-induced magnetism.

7 ng application in the field of environmental magnetism.

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

9 uing phenomena such as superconductivity and magnetism.

10 o use polarized light to alter or manipulate magnetism.

11 exchange and leading to strongly frustrated magnetism.

12 ism for the origins of both conductivity and magnetism.

13 cles' mass generation, superconductivity and magnetism.

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

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

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

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

18 correlation between octahedral rotation and magnetism.

19 ovided direct information on the host of the magnetism.

20 and Sr2-yLayRuO4, implying orbital dependent magnetism.

21 electric materials that display some form of magnetism.

22 ze lattice spin models for exploring quantum magnetism.

23 C are more typically drivers of commensurate magnetism.

24 face do not need to be itinerant to generate magnetism.

25 ory animals are among organisms that exploit magnetism.

26 mistry to provide model objects in molecular magnetism.

27 coating with cationic polymers did not alter magnetism.

28 putationally intractable problems in quantum magnetism.

29 ry, but not sufficient, for the formation of magnetism.

30 opportunities for electric-field control of magnetism.

31 l and neural networks to protein folding and magnetism.

32 the edge Cu atoms do not exhibit significant magnetism.

33 triguing coexistence of ferroelectricity and magnetism.

34 unconventional superconductivity and quantum magnetism.

35 on is thus inextricably tied to photoinduced magnetism.

36 strong coupling between ferroelectricity and magnetism.

37 ing on the competition between covalency and magnetism.

38 arriers with other quantum phenomena such as magnetism.

39 ilms and could open new prospects in surface magnetism.

40 irements for displacive ferroelectricity and magnetism.

41 In the context of quantum magnetism, a number of experiments have demonstrated the

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

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

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

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

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

47 ssible benefits in potential applications in magnetism and catalysis.

48 structural trimerization, ferroelectricity, magnetism and charge conduction are intricately coupled.

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

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

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

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

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

54 produces clearly discernible effects on the magnetism and conductivity.

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

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

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

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

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

60 rconductivity and giant magnetoresistance to magnetism and ferroelectricity.

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

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

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

64 ortant step towards the quest for artificial magnetism and negative refractive index metamaterials at

65 al applications including mapping of crustal magnetism and ocean circulation measurements, yet availa

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

67 way toward a new probe of frustrated quantum magnetism and perhaps the design of new quantum material

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

69 l behaviour of these materials proposes that magnetism and superconductivity develop out of quasi-loc

70 3.2) as well as the phase separation between magnetism and superconductivity point to a conventional

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

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

73 tely equal contributions; one from itinerant magnetism and the other from dangling bonds.

74 provide clues about the relationship between magnetism and unconventional superconductivity.

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

76 lead to some unusual phenomena in molecular magnetism, and are important to the functionality of imp

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

78 sport in semiconductors and superconductors, magnetism, and devices such as terahertz oscillators.

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

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

81 tials, X-ray structures, elemental analysis, magnetism, and requirement of an oxidant (O(2)) indicate

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

83 large or negative refractive index; optical magnetism; and controlled anisotropy.

84 interference device microscopy we find that magnetism appears only above a critical LaAlO(3) thickne

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

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

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

88 gas, low temperature superconductivity, and magnetism, are not present in the bulk materials, genera

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

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

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

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

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

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

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

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

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

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

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

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

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

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

103 This newfound control over emergent magnetism at the interface between two non-magnetic oxid

104 tween the two phases indicates the nature of magnetism at the LaAlO3/SrTiO3 interface as both having

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

106 The discovery of conductivity and magnetism at the polar-nonpolar interfaces of insulating

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

108 Within molecular magnetism, at least two very different definitions of fr

109 oposed recently to induce artificial optical magnetism based on the principle that magnetic effects a

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

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

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

113 3-) anion support both superconductivity and magnetism but can consist of fundamentally distinct thre

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

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

116 Control of magnetism by applied voltage is desirable for spintronic

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

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

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

120 Here we simulate the emergence of magnetism by implementing a fully connected non-uniform

121 Controlling magnetism by means of electric fields is a key issue for

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

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

124 le functionalities, such as fluorescence and magnetism, can exhibit enhanced efficiency and versatili

125 c materials that equilibrium descriptions of magnetism cannot explain.

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

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

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

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

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

131 In one dimension, the study of magnetism dates back to the dawn of quantum mechanics wh

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

133 As the magnetism disappears and T-->0, the magnetotransport sca

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 eveals an initial quantum coherent regime of magnetism, distinguished from the picosecond (10(-12) se

138 study to demonstrate that these two types of magnetism do not only coexist but complement each other

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

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

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

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

143 t phenomena, including superconductivity and magnetism, found in the two-dimensional electron liquid

144 the ordering temperature of the photoinduced magnetism from 18 to 75 K.

145 semiconducting structure (density-based MC), magnetism from magnetic structure (mobility-based MC), a

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

147 Superconductivity and magnetism generally do not coexist.

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

149 Magnetism has been observed in LaAlO(3)/SrTiO(3), but it

150 The field of molecular magnetism has grown tremendously since the discovery of

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

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

153 Electrical control of magnetism has the potential to bring about revolutionary

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

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

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

157 It has been a long-standing goal to create magnetism in a non-magnetic material by manipulating its

158 ests that disorder or local strain generates magnetism in a population of the interface carriers.

159 c bio-magnetism, we explored the creation of magnetism in a simple model organism.

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

161 By demonstrating a route to quantum magnetism in an optical lattice, this work should facili

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

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

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

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

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

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

168 detailed understanding of the origin of the magnetism in dilute magnetic semiconductors is crucial t

169 etal-doped quantum dots (QDs), the origin of magnetism in diluted magnetic semiconductors (DMSs) is y

170 t density functional calculations predicting magnetism in doped semiconducting beta-FeSi(2) and CrSi(

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

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

173 Voltage control of magnetism in ferromagnetic semiconductor has emerged as

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

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

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

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

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

179 These results merge two fields, femtosecond magnetism in metals and band insulators, and non-equilib

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

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

182 ons have a significant role in mediating the magnetism in oxides, and recently attracts a lot of inte

183 Magnetism in plutonium has been debated intensely, but t

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

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

186 Understanding exotic forms of magnetism in quantum mechanical systems is a central goa

187 ustrate a new aspect to the phenomenology of magnetism in SrTiO3 by reporting the observation of an o

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

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

190 The absence of known signatures of static magnetism in the Sr-rich side of the (Ca, Sr) substituti

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

192 Magnetism in transition metal compounds is usually consi

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

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

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

196 The magnetism induced at the interface resulting from the la

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 Magnetism is a consequence of broken time-reversal symme

200 For instance, frustrated magnetism is a hallmark of poorly understood systems suc

201 Novel or unusual magnetism is a subject of considerable interest, particu

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

203 roposed an exotic pairing mechanism in which magnetism is accommodated by the formation of pairs with

204 Metallic magnetism is both ancient and modern, occurring in such

205 makes use of electromagnetism, and that same magnetism is essential in generating the power these new

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

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

208 The much-discussed vacancy magnetism is found to have a dual origin, with two appro

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

210 rs into itinerant carriers in a metal, where magnetism is preserved in the form of strong correlation

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

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

213 city, viscosity, electrical conductivity and magnetism, is well known.

214 ts indicate that the lattice distortions and magnetism jointly play a critical role in inducing super

215 cies, revealing a detailed interplay between magnetism, lattice defects, and light in an archetypal c

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

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

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

219 various physical properties such as colour, magnetism, luminescence, chirality, porosity, etc.

220 various physical properties such as colour, magnetism, luminescence, chirality, porosity, etc. due t

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

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

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

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

225 , demonstrating the close connection between magnetism, nematicity and unconventional superconductivi

226 A comprehensive comparative analysis of the magnetism of [K(18-crown-6)][Ln(COT)2] (Ln = Sm, Tb, Dy,

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

228 Here we show that the magnetism of adatoms in graphene is itinerant and can be

229 Our results suggest a common origin for the magnetism of all the Fe-based superconductors, despite h

230 gnetic 2D Ising system, and support that the magnetism of BaFe2(PO4)2 is uniaxial (g perpendicular =

231 The magnetism of DySc(2)N@C(80) endofullerene was studied wi

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

233 The magnetism of Fe2MnAl and Mn2FeAl compounds are studied b

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

235 state, raises the issue of the existence and magnetism of other [M(4)S(4)L(4)](z) clusters, none of w

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

237 The conclusions about the magnetism of the 0 and +1 charge states were also reprod

238 The magnetism of the cells is due to a mum-sized intracellul

239 d that geometric considerations dominate the magnetism of the Cp* complexes, while topology and alkyn

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

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

242 The magnetism of the interface, however, was observed to be

243 electronics combine more subtly to drive the magnetism of the new complexes reported here.

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

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

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

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

248 Control of magnetism on the atomic scale is becoming essential as d

249 In the absence of natural magnetism, optical Fano resonances have so far been base

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

266 w-pressure spin-singlet regime, the onset of magnetism results in an expansion of the lattice with de

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

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

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

270 nisms, a pure surface charge modification of magnetism shows a strong correlation to polarization of

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

272 target new materials exhibiting interesting magnetism such as spin frustration.

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

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

275 In magnetism, systems incorporating geometrical frustration

276 in technology recently, arguably more so in magnetism than in any other branch of science and techno

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

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

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

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

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

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

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

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

285 ion chemistry with the concepts of molecular magnetism to design magnetic Metal-Organic Frameworks (M

286 In such materials the interplay of magnetism, transport and other Fermi liquid properties c

287 e report spectroscopic investigations of the magnetism using element-specific techniques, including X

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 problem of how ET affects the Au25 magnetism was addressed by comparing the continuous-wave

291 The term "frustration" in the context of magnetism was originally used by P. W. Anderson and quic

292 Chiral magnetism was seen in several film structures on appropr

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

294 duction and the application of synthetic bio-magnetism, we explored the creation of magnetism in a si

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

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

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

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

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

300 Goodenough-Kanamori rules suggested that the magnetism within the ladder and ladder-single chain syst