ライフサイエンスコーパス: magnet

1 ral cues while in the scanner (a Siemens 3 T magnet).

2 ounds, Dy2Ti2O7 and Ho2Ti2O7, using a vector magnet.

3 st Dy(III) cluster that is a single-molecule magnet.

4 and nano-fibers using a permanent revolving magnet.

5 gallery-mode microcavity actuated by a micro-magnet.

6 nics chips together with a compact permanent magnet.

7 is a candidate for rare-earth free permanent magnet.

8 mass spectrometer (MS) equipped with a 15 T magnet.

9 Ps to remove excess Al(3+) by using external magnet.

10 The {Cr8 Dy8 } wheel is a single-molecule magnet.

11 a magnesium diboride (MgB2) superconducting magnet.

12 ll characteristics of a soft single-molecule magnet.

13 ehensive formulation of this two dimensional magnet.

14 apparatus nearby but separated from the MRI magnet.

15 direct irradiation of the sample inside the magnet.

16 which allows it to be attracted rapidly to a magnet.

17 erroic behavior in a metal-organic framework magnet.

18 e second counter via an external cylindrical magnet.

19 spirit of recent works with single-molecule magnets.

20 ple is the quantum spin liquid in frustrated magnets.

21 c molecular systems, the so-called molecular magnets.

22 neration of high-temperature single-molecule magnets.

23 novel phenomena of geometrically frustrated magnets.

24 r than those of traditional injection molded magnets.

25 cross five sites were obtained using 3-tesla magnets.

26 onents of electronic materials and permanent magnets.

27 onventional current driven switching of nano-magnets.

28 reflect the phase behaviour of triangular XY magnets.

29 ary in single-polar-domain crystals of polar magnets.

30 covering pure REEs from the industrial scrap magnets.

31 enic temperatures or sample transfer between magnets.

32 onents of electronic materials and permanent magnets.

33 ling of the magnetization in single-molecule magnets.

34 ld that is available only by superconducting magnets.

35 metrically magnetized, cylindrical permanent magnets.

36 magnitude far greater than state-of-the-art magnets.

37 idered exclusive to conventional metal-based magnets.

38 oupling to reorient closely spaced nanoscale magnets.

39 known hard ferromagnets and single-molecular magnets.

40 y and is most often used in high performance magnets.

41 facilitating the switching of perpendicular magnets.

42 in the magnetic field generated by permanent magnets.

43 ymium and dysprosium from recycling of NdFeB magnets.

44 ce based on the ME induced switching of nano-magnets.

45 sensing as well as construction of molecular magnets.

46 te matrix, which behave like single-molecule magnets.

47 sotropy in spintronic devices and artificial magnets.

48 ance the high temperature performance of the magnets.

49 may also inform the development of new bulk magnets.

50 es compared to corresponding pure rare-earth magnets.

51 agnetic behaviours in conventional molecular magnets.

52 hydrodynamics (MHD) to take advantage of the magnet (0.56 T) beneath the chip and the uniform flat fl

53 actuation and sliding angle using permanent magnets (1.8-2.1 kG).

54 The MTBE employs a flow-less, magnet-actuated, bead-based ELISA for simultaneous detec

55 Finally, interfacing a device-embedded magnet allows selective capture of 96% of droplet-encaps

56 on between the magnets or the lengths of the magnets (along the axis of measurement) enables the sens

57 nation therapy through the manipulation of a magnet and a NIR laser.

58 The system consists of an implantable soft magnet and an external head-mounted magnetic sensor that

59 mperature information transduction between a magnet and an organic light-emitting diode that does not

60 cells was determined by both location of the magnet and layout of the in-channel magnetic structures.

61 ic generator (TMEG) arrays, composed of soft magnet and piezoelectric polyvinylidene difluoride (PVDF

62 ds to support the formation of a microporous magnet and provide the first example of a structurally c

63 The magnet and separation vessel (collectively dubbed the he

64 law by correlating the distance between the magnet and the measuring paramagnetic bead with unfoldin

65 nd installed within a single superconducting magnet and vacuum system.

66 e long-living interface states formed by the magnet and weakly physisorbed molecules.

67 a building block for organic molecule-based magnets and also serves as a model compound for test and

68 The combined action of permanent magnets and an automatically actuated electromagnet enab

69 l attraction of ferritin-expressing cells to magnets and increased contrast for cellular magnetic res

70 successfully recovered from commercial NdFeB magnets and industrial scrap magnets via membrane assist

71 gy levels strongly interact with neighboring magnets and mediate the spatial movement of information

72 iral molecules, magnetic Skyrmions in chiral magnets and nonreciprocal carrier transport in chiral co

73 stability for systems as diverse as solids, magnets and potential exotic quantum materials.

74 study of wind turbines at both the material (magnets) and technology (turbine generators) levels, we

75 The DNA is stretched horizontally by a magnet, and a nanoscale knife made of silicon nitride is

76 OS is a single-domain ferromagnet like a bar magnet, and find the probable cause for the ferromagneti

77 Tag anchoring, sub-micrometer positioning of magnets, and an active correction of the focal drift.

78 ials, spin-orbit Mott insulators, frustrated magnets, and dilute magnetic alloys.

79 ets, skyrmions, atomically assembled quantum magnets, and spin ice.

80 (III) complexes could act as single-molecule magnets, and that the lower oxidation state of Np(II) is

81 o statistical physics models for ordering in magnets, and the correct prediction of scale-free correl

82 lly implanted on the eye, and changes in the magnet angle as the eye rotated were detected by a magne

83 owever, superconducting wires for high-field-magnet applications are still dominated by low-Tc Nb3Sn

84 is one of the best candidates for high-field-magnet applications because of its high upper critical f

85 ture superconductors is important for future magnet applications.

86 2Cu3Ox coated conductors for very high field magnet applications.

87 In this work, by using small commercial magnets ( approximately 0.5-1.2 T) the orientation of th

88 cient cooling system and the superconducting magnet are essential components of magnetic resonance im

89 Single-molecule magnets are a type of coordination compound that can ret

90 Rare-earth-free magnets are highly demanded by clean and renewable energ

91 Away from the dislocation, the magnets are locally unfrustrated, but frustration of the

92 nly found at 1.5-3 tesla (T), these powerful magnets are massive and have very strict infrastructure

93 Ultrafine-grained die-upset Nd-Fe-B magnets are of importance because they provide a wide re

94 Above-room-temperature polar magnets are of interest due to their practical applicati

95 a in striking similarity to single-molecular magnets are particularly pronounced for x<<1 and indicat

96 On the other hand, perpendicularly polarized magnets are preferred over in-plane magnets for high-den

97 Double corundum-related polar magnets are promising materials for multiferroic and mag

98 Chiral magnets are promising materials for the realisation of h

99 lex low-temperature-ordered states in chiral magnets are typically governed by a competition between

100 ple arrives at a room-temperature, permanent magnet array, where rapid dissolution with 40 degrees C

101 ng board using graphene suspension and a bar magnet as a pen.

102 netic gradients parallel to the faces of the magnets as a means of increasing the sensitivity of MagL

103 anic framework featuring Dy2 single-molecule magnets as nodes.

104 are defined, by analogy with single-molecule magnets, as bistable molecules with a toroidal magnetic

105 We specifically show that molecular magnets, as the most promising technology, can implement

106 ing hyperpolarized signals using a permanent magnet at 1 Tesla (1T) is a simple and cost-effective me

107 ecyclable in viscous solutions simply with a magnet bar in an experimental demonstration.

108 Single-molecule magnets based on lanthanides have accounted for many imp

109 The reduced cluster displays single molecule magnet behavior manifest in both variable-temperature ze

110 a trigonal prism geometry showing single ion magnet behavior with very high Orbach relaxation barrier

111 ferromagnets, mediating both exchange-spring magnet behaviour and exchange bias.

112 behaves as a U(V) -localized single molecule magnet below 4 K.

113 magnetic field drives the three-dimensional magnet beta-Li2IrO3 from its incommensurate ground state

114 ll be especially valuable for high-field NMR magnets beyond the present 1 GHz proton resonance limit

115 ssible to switch a perpendicularly polarized magnet by SOT without needing an external magnetic field

116 substitution of Nd in NdFeB-based permanent magnets by Ce, the most abundant and lowest cost rare ea

117 cture of a novel lanthanide-based single-ion magnet, {C(NH2)3}5[Er(CO3)4].11H2O, was comprehensively

118 droplets to provide a "handle" by which the magnet can exert a force on the droplet.

119 that the field levels generated by permanent magnets can be sufficient to completely transform the al

120 ail melanoma models, Fe(Salen) delivery with magnet caused a robust decrease in tumor size, and the a

121 he magnetic field induces force on the micro-magnet causing deformation in the polymer around the mic

122 perties, ranging from catalytic to molecular magnet characteristics.

123 the magnets; (ii) by moving a small external magnet close to the levitating objects while keeping the

124 The starting polymer magnet composite pellets consist of 65 vol% isotropic Nd

125 Magnetic field gradients from permanent magnets confine the particle in two dimensions, while co

126 A new type of carbon charge-transfer magnet, consisting of a fullerene acceptor and single-wa

127 a levitating object above the surface of the magnet corresponds to its density; the strength of the g

128 e case of a copper-nitroxide based molecular magnet Cu(hfac)2L(i-Pr) that does not exhibit quantitati

129 problem and makes it possible to switch the magnet deterministically.

130 ction of high-field-strength superconducting magnets, digital RF systems, and phased-array coils.

131 The sensor consists of a thin magnet disc, aligned at the back of the electrode, in or

132 istically switch a perpendicularly polarized magnet due to symmetry reasons.

133 Here we show that the layered Ising magnet Dy3Mg2Sb3O14 hosts an emergent order predicted th

134 urrent density which can be used to switch a magnet efficiently and there is increasing interest in i

135 All magnets elongate and contract anisotropically when place

136 bination of continuous flow and a stationary magnet enables a degree of autonomy in the system, while

137 ifies manufacturing of near-net-shape bonded magnets, enables efficient use of rare earth elements th

138 Single-molecule magnets exhibit magnetic hysteresis of molecular origin-

139 surements reveal that most densely populated magnets exhibit similar memory behavior characterized by

140 ined at one of the electrodes by a permanent magnet external to the cell.

141 Uncalibrated strong field magnet extraction techniques have been typically used to

142 photocatalyst can be recycled and reused by magnet extraction.

143 rameworks, can rotate microscopic rotors and magnets fast enough to generate an electric power of 0.1

144 Here we report giant ME effects in a polar magnet Fe2Mo3O8 at temperatures as high as 60 K.

145 NMR instrument equipped with a 1.5 T Halbach magnet for direct detection of ammonium N, total P, and

146 n In pregnant miniature pigs, the use of 3-T magnets for diagnostic MR imaging with normal SAR regime

147 e critical Heavy Rare Earth (HRE) content of magnets for green technologies, HRE-free Nd-Fe-B has bec

148 onclude that within the application of NdFeB magnets for HDDs, the potential for loop-closing is sign

149 olarized magnets are preferred over in-plane magnets for high-density data storage applications due t

150 ropose to use an array of large-spin quantum magnets for realizing a device which has two modes of op

151 c magnetic properties and for designing bulk magnets for technological applications.

152 agents and washing solutions via an external magnet, for the rapid detection of the inflammatory biom

153 ted for single lanthanide atoms in molecular magnets, for lanthanides diluted in bulk crystals, and r

154 g spin stripes, never observed in the chiral magnets, forms.

155 closest realization of the transverse Ising magnet found to date.

156 ooks, and today's high-performance permanent magnets--found in hybrid cars, wind turbines, and disk d

157 chip have made imperative the exploration of magnet free alternatives.

158 our advantage to realize a new generation of magnet-free non-reciprocal components.

159 ent of recycling technologies for rare earth magnets from postconsumer products, we present herein an

160 Dismantling and separate processing of NdFeB magnets from their end-use products can be a more prefer

161 ated from the in-flow matrix using permanent magnet, Further, removal of the cell debris, proteins, a

162 pin-liquid state in the canonical frustrated magnet gadolinium gallium garnet (Gd3Ga5O12).

163 t this approach is increasingly effective as magnets get smaller.

164 Magnet-guided localization of FeO nanoparticles within p

165 The transverse Ising magnet Hamiltonian describing the Ising chain in a trans

166 Thermal transport of quantum magnets has elucidated the nature of low energy elementa

167 Quantum magnets have occupied the fertile ground between many-bo

168 biocomposite is captured at SPCE by a super magnet (Hb/MHAM@Mag-NPs/SPCE).

169 matter, the frustrated rare-earth pyrochlore magnets Ho2Ti2O7 and Dy2Ti2O7, so-called spin ices, exhi

170 ments were more favorable in Magnet than non-Magnet hospitals.

171 years since the discovery of single-molecule magnets, hysteresis temperatures have increased from 4 k

172 ded in the paramagnetic solution between the magnets; (ii) by moving a small external magnet close to

173 ation and be easily separated by an external magnet in 60 second.

174 etailed mapping of stocks and flows of NdFeB magnets in Denmark.

175 magnetic states predicted for this family of magnets-including collective spin-vortices of relevance

176 nt magnetization of the Dy-Cu press injected magnets increased substantially in comparison with those

177 applications of gallium are NdFeB permanent magnets, integrated circuits and GaAs/GaP-based light-em

178 conductivity at superconductor/inhomogeneous magnet interfaces.

179 it shows that the surface of common Nd2Fe14B magnet is chemically and structurally very different fro

180 uent diffusion process, a higher performance magnet is expected to be obtained.

181 An intrinsic switching time of 100 ps per magnet is observed.

182 printed electrode (SPE) by using a permanent magnet is presented.

183 etization, the so-called 'A-phase' in chiral magnets is an example of a thermodynamically stable phas

184 udies for the improvement of single-molecule magnets is underlined.

185 on of low-energy quantized spin waves in the magnet, known as magnons, into a flow of spins from the

186 ein L as a molecular template, we generate a magnet law by correlating the distance between the magne

187 We demonstrate that, using this magnet law, we can accurately measure the dynamics of pr

188 reased by increasing the number of permanent magnet layers to determine PM removal characteristics.

189 In frustrated quantum magnets, long-range magnetic order fails to develop desp

190 of insulin transgene expression with RF or a magnet lowers blood glucose.

191 Different from the bulk magnet, magnetic NPs exhibit unique magnetism, which ena

192 o study a rare-earth element based permanent magnet material, Nd2Fe14B.

193 ration, where lithographically patterned bar magnets mimic the frustrated interactions in real materi

194 Complementing the magnet miniaturization, here we integrate the NMR spectr

195 he operating temperatures of single-molecule magnets-molecules that can retain magnetic polarization

196 The magnetic transition of permanent magnet nanoparticles from ferromagnetism to paramagnetis

197 through the magnetic transition of permanent magnet nanoparticles.

198 Frustrated quantum magnets not only provide exotic ground states and unusua

199 igned a 2-part, titanium-encased, rare-earth magnet oculomotor prosthesis, powered to damp nystagmus

200 PdCrO2, a frustrated metallic magnet, offers the opportunity to examine the relationsh

201 classical and quantum dynamics of molecular magnets on graphene.

202 impaired by attachment of a strong neodymium magnet or were controls.

203 igh-energy synchrotron X-rays from a bending magnet or wiggler source.

204 t and excluded volume, and (ii) using weaker magnets or reducing the magnetic susceptibility of the m

205 high magnetic fields generated by permanent magnets or superconducting coils has found applications

206 ating the distance of separation between the magnets or the lengths of the magnets (along the axis of

207 ving a "ghost" demonstration (ball moved via magnet) or without demonstration.

208 l for the development of new single-molecule magnets: organometallic chemistry presents possibilities

209 MRCP was performed in a 1.5-Tesla magnet (Philips) with SSH MRCP 3DHR and SSHMRCP rad prot

210 results directly demonstrate that a powerful magnet placed on the scalp modulates normal brain activi

211 Operational parameters such as magnet position, hybridization buffer composition, hybri

212 separated from the digests with a hand-held magnet prior to analysis.

213 clinical MRI scanners employ superconducting magnets producing very high magnetic fields.

214 The density of the final BAAM magnet product reached 4.8 g/cm(3), and the room tempera

215 can deterministically switch a perpendicular magnet, provided an in-plane magnetic field is applied.

216 exploring the spin dynamics in 5d pyrochlore magnets.Pyrochlore 5d transition metal oxides are expect

217 r quantum spin liquids in frustrated quantum magnets recently has enjoyed a surge of interest, with v

218 ated, trimetallic dysprosium single-molecule magnet relaxes via the second-excited Kramers' doublet,

219 azards regressions revealed abnormal cranial magnet resonance imaging (cMRI; hazard ratio [HR] = 5.94

220 e@C-Fc-2, in the presence and absence of the magnet, respectively.

221 07mugdL(-1) in the absence and presence of a magnet, respectively.

222 netic beads will be attracted by an external magnet revealing the golden color of the sensor surface

223 electrical current, based on control via the magnet's remanent field of the exciton recombination pro

224 +) dinuclear cations produced a single-chain magnet (SCM) involving stacking interactions of TCNQF (-

225 ion vessel (collectively dubbed the hexapole magnet separator or HMS) was tested on four human and fo

226 A promising permanent magnet should possess high remanent magnetic flux densit

227 m coherence is detected in the 4f single-ion magnet (SIM) Yb(trensal), by isotope selective pulsed EP

228 Dy(III) single-ion magnets (SIMs) with strong axial donors and weak equator

229 ld, they are often referred to as single-ion magnets (SIMs).

230 compounds exhibit switchable single-molecule magnet (SMM) and exchange-bias behavior depending on the

231 the Mn49 cluster displaying single-molecule magnet (SMM) behavior and being the second largest repor

232 coupling and results in hard single-molecule magnet (SMM) behavior, with an effective barrier to magn

233 The prototypical single-molecule magnet (SMM) molecule [Mn12O12(O2CCH3)16(OH2)4] was inco

234 The single-molecule magnet (SMM) properties of the isocarbonyl-ligated dyspr

235 t of the dimer is a separate single-molecule magnet (SMM) with an S = 6 ground state and that the two

236 termining factors in whether single-molecule magnets (SMMs) may be used as the smallest component of

237 Single-molecule magnets (SMMs) with one transition-metal ion often rely

238 recent advent of mononuclear single-molecule magnets (SMMs), a rational approach based on lanthanides

239 schemes for high-temperature single-molecule magnets (SMMs).

240 zation measurements on the dimerized quantum magnet SrCu2(BO3)2 at cryogenic temperatures and through

241 magnetic transitions from ferromagnet to non-magnet state at room temperature.

242 xplain magnetic excitations of the molecular magnet states.

243 e) and hospitals (size, teaching status, and Magnet status) were included as control variables.

244 age, mean physical disability score, imager magnet strength, lesion load, and number of diffusion di

245 her factors to the BOLD signal for different magnet strengths and pulse sequences.

246 1.25 mmol/L of gadolinium in iohexol at both magnet strengths.

247 mplished by engineering an anisotropy in the magnets such that the magnetic easy axis slightly tilts

248 discovery that strongly spin-orbital-coupled magnets, such as alpha-RuCl3, may display a broad excita

249 agnetic field (120-200 mT at 2-3 cm from the magnet surface) over the human occiput produces a focal

250 up the door to moving from a pure permanent-magnet system to a stronger nanocomposite system at lowe

251 s here demonstrated with the single-molecule magnet TbPc2 evidencing also an exceptional long-range t

252 practice environments were more favorable in Magnet than non-Magnet hospitals.

253 ards the fabrication of thin films of chiral magnets that host certain spin whirls, so-called skyrmio

254 In triangular-lattice magnets, the coexistence of third-neighbor antiferromagn

255 ic properties of two metal-organic polymeric magnets, the quasi-one-dimensional (1D) Cu(pyz)(NO3)2 an

256 In contrast to the magnons in conventional magnets, their spin excitations are poorly understood.

257 ns, into a flow of spins from the precessing magnet to adjacent leads.

258 ctor volume, if the sample trajectory in the magnet toward NMR detector is long enough to polarize th

259 cted (uncleaved) QD-CPs by using a permanent magnet, ultrasensitive fluorescent detection of DV is re

260 A 0.37 T magnet under the chip generated a magnetic field perpend

261 netic relaxation typical for single molecule magnets under an applied direct current magnetic field.

262 ween the organic molecules and the inorganic magnets used as electrodes.

263 information may be obtained with a permanent magnet using enzyme solutions and in whole cells.

264 ercivity (H ci) of a hard/soft nanocomposite magnet using the mass fraction.

265 nduced low energy and fast switching of nano-magnets using the magneto-electric (ME) effect.

266 cterization of a new thin-film organic-based magnet V[MeTCEC]x (V = vanadium; MeTCEC = methyl tricayn

267 ion using a "sunlight simulator" outside the magnet versus direct irradiation of the sample inside th

268 ommercial NdFeB magnets and industrial scrap magnets via membrane assisted solvent extraction (MSX).

269 Upon hybridization, a magnet was applied to concentrate the hybridization sand

270 An external magnet was fixed on the back of the sensor to accelerate

271 A small magnet was surgically implanted on the eye, and changes

272 -surface regions of the Dy-Cu press injected magnets was also investigated.

273 MALDI-FTICR-MS platform equipped with a 15 T magnet, we reported on the mass analysis of intact human

274 DDs) containing neodymium-iron-boron (NdFeB) magnets were selected as the case product for this exper

275 So far, skyrmions were amply investigated in magnets, where due to the presence of chiral interaction

276 ffective technique for fabricating permanent magnets which frequently involve critical rare earth ele

277 ution in high-temperature annealed die-upset magnets, which had significant impact on the improvement

278 n additional spin-orbit torque on the CoNiCo magnets, which is confirmed by macrospin calculations an

279 parison with those of the annealed reference magnets, which is distinct from the reported experimenta

280 A prominent example occurs in conventional magnets, which support bosonic magnons-quantized harmoni

281 ly most researches are focused on frustrated magnets, which usually have complicated magnetic structu

282 s, may provide another option for high-field-magnet wires.

283 irst time, the corresponding pure rare-earth magnet with 58% enhancement in energy product.

284 this complex to behave as a single-molecule magnet with a relaxation barrier of U(eff) = 14(1) cm(-1

285 We combined a pulsed magnet with an x-ray free-electron laser to characterize

286 Simulations of a quantum magnet with antiferromagnetic and dimerized ground state

287 here is no report on the formation of Fe16N2 magnet with high Br and large Hc in bulk format before.

288 change in the relative position of the soft magnet WITH respect to the external sensor as the result

289 in a model of a disordered, one-dimensional magnet with spin one-half edge excitations.

290 presented a route to obtain a new die-upset magnet with substantially improved magnetic properties.

291 netic ferroelectrics are conical spin spiral magnets with a simultaneous reversal of magnetization an

292 ing, are viable with low-field, single-sided magnets with an inhomogeneous magnetic field.

293 We predict that several (frustrated) magnets with dominant direct exchange and non-collinear

294 tic chemist in the design of single-molecule magnets with enhanced relaxation barriers.

295 or future bonded, consolidated and thin film magnets with high energy density and high thermal stabil

296 pectrometer miniaturization, small permanent magnets with high field homogeneity have been developed.

297 loring next-generation ultrastrong permanent magnets with less expensive rare-earth elements.

298 ricate isotropic near-net-shape NdFeB bonded magnets with magnetic and mechanical properties comparab

299 the magnetic properties of rare-earth based magnets with nano-sized building blocks.

300 Here we report dysprosium single-molecule magnets with neutral and anionic phosphorus donor ligand