ライフサイエンスコーパス: magnet

1 A expression using miRNA-guided neuron tags (mAGNET).

2 ecreases with increasing the strength of the magnet.

3 with non-uniform magnetization, like helical magnet.

4 ant anomalous Hall response observed in this magnet.

5 ted holder containing an embedded rare-earth magnet.

6 of a magnetic field generated by a permanent magnet.

7 apparatus nearby but separated from the MRI magnet.

8 gallery-mode microcavity actuated by a micro-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 ighest observed for any rare-earth-free hard magnet.

15 hich to develop a new generation of designer magnets.

16 it coupled magnetic resonance in topological magnets.

17 f-principle method for revealing topological magnets.

18 effects in geometrically frustrated quantum magnets.

19 ications of spin wave modes in organic-based magnets.

20 erimental studies on van der Waals monolayer magnets.

21 generated by low-temperature superconducting magnets.

22 rmance without bulky and expensive permanent magnets.

23 optoelectronic devices using two-dimensional magnets.

24 ligand for high-performance single-molecule magnets.

25 lecular systems and high T(C) molecule-based magnets.

26 or potential applications based on permanent magnets.

27 n non-centrosymmetric, e.g. chiral or polar, magnets.

28 e in the ground states of frustrated quantum magnets.

29 g requirements on conductors for fabricating magnets.

30 mily has been missing one crucial member: 2D magnets.

31 spirit of recent works with single-molecule magnets.

32 neration of high-temperature single-molecule magnets.

33 novel phenomena of geometrically frustrated magnets.

34 onventional current driven switching of nano-magnets.

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

36 sensing as well as construction of molecular magnets.

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

38 sotropy in spintronic devices and artificial magnets.

39 ance the high temperature performance of the magnets.

40 ants and as spin-containing units in polymer magnets.

41 may also inform the development of new bulk magnets.

42 urally characterized metal-organic framework magnets.

43 I, cell phone, bonded, swarf, and hybrid car magnets.

44 generation of ultra-high-field (UHF) HTS NMR magnets.

45 t in the development of lanthanide-free hard magnets.

46 r revolutionary rational design of molecular magnets.

47 c relaxation dynamics of the single-molecule magnets 1-Dy through 4-Dy, where stronger J(Gd-rad) for

48 effect is important for the study of quantum magnets(2-7).

49 tocaloric working bodies driven by permanent magnets(3-5) and electrocaloric working bodies driven by

50 erials and macroscopic set-ups with external magnets(4,16), which is not feasible for nanoscale integ

51 two-level systems in a dense and disordered magnet advances the search for qubit platforms emerging

52 conductors above 150 to ensure stability of magnets against quenching.

53 single-cell transcriptome data using the RNA-Magnet algorithm described here.

54 , placed between two like-poles-facing NdFeB magnets, allowed separation of seven relevant compounds

55 A simple magnet allows highly specific isolation of the labeled c

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

57 e exotic states of matter such as frustrated magnets, an extensive field of research from both the th

58 ey can also be assessed using a head-mounted magnet and a magnetometer.

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

60 The catalyst can be recovered by a magnet and recycled without appreciable loss of catalyti

61 e relative to treatment, map quality, imager magnet and sequence, average tumor volume, and reader va

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

63 were actuated by a combination of permanent magnets and electromagnets.

64 These compounds are single-chain magnets and exhibit wide, square magnetic hysteresis bel

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

66 agnetic sponges, luminescent magnets, chiral magnets and photomagnets, SHG-active magnetic materials,

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

68 dimensional crystals, metal-dichalcogenides, magnets and superconductors.

69 nd, and it briefly introduces the classes of magnets and the experimental methods used to characteriz

70 Section 1 outlines the need for new magnets and the potential role of metal-organic framewor

71 viously hidden aspects of magnetism in Sm-Co magnets and, by identifying weak points in the microstru

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

73 r mammalian expression using a CAG promoter, Magnets, and 2A self-cleaving peptide.

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

75 lications, such as radical magnetoelectrics, magnets, and optoelectronics.

76 high-performance permanent magnets, flexible magnets, and printable magnetic inks for energy and sens

77 for ultra-high-field (> 1 GHz or 23.5 T) NMR magnets, and thus unaffected from the windings' diamagne

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

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

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

81 rmance Sm(x) Co(y) nanomagnets for permanent magnet applications.

82 2Cu3Ox coated conductors for very high field magnet applications.

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

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

85 Skyrmions in chiral magnets are a particle-like texture that has been attrac

86 nce (LF-(1)H NMR) devices based on permanent magnets are a promising analytical tool to be extensivel

87 ctor coils(1), and such high-power resistive magnets are available in only a few facilities worldwide

88 Among these, Sm(2) Co(17) -based magnets are excellent candidates owing to their high-tem

89 Low dimensional quantum magnets are interesting because of the emerging collecti

90 However, current vdW magnets are limited by their extreme sensitivity to air,

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

92 Kagome magnets are predicted to support intrinsic Chern quantum

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

94 Chiral magnets are promising materials for the realisation of h

95 f the layered structure, van der Waals (vdW) magnets are sensitive to the lattice deformation control

96 Some of the best-performing high-temperature magnets are Sm-Co-based alloys with a microstructure tha

97 Among them, Magnets are small modules engineered from the Neurospora

98 Lanthanide permanent magnets are widely used in applications ranging from nan

99 By contrast, superconducting magnets are widespread owing to their low power requirem

100 Dynamically adjustable permanent magnet arrays have been proposed to generate switchable

101 on radiation from free electrons, emitted in magnet arrays such as undulators, forms the basis of muc

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

103 material with properties far beyond an Ising magnet as initially assumed.

104 rromagnetic NiPS(3) introduces van der Waals magnets as a platform to study coherent many-body excito

105 mplified by the scale invariance of an Ising magnet at the critical point.

106 lysis using magnetic rotation of an external magnet, at high (5000) rpm, to induce the rotation of a

107 nature of the constructed nano-adsorbent, a magnet bar was used to separate the nano-adsorbent from

108 ne the literature of metal-organic framework magnets based on diamagnetic and radical organic linkers

109 We tested the ESA and deflector, magnet-based mass spectrometer, and anode in the laborat

110 AM8-22), and scratching was assessed using a magnet-based recording technology.

111 r (ESA) and a deflector, backed by a static, magnet-based, mass spectrometer.

112 des find extensive applications in displays, magnets, batteries, contrast reagents, and biological pr

113 Further, by combining magnet beads, we established a rapid and wash-free homog

114 is is particularly true for rare-earth-based magnets because of the large effective spin anisotropy i

115 nts revealed the existence of a single-chain magnet behavior hidden below the canted antiferromagneti

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

117 or ingestions by children of small neodymium magnets between 2009 and 2019, before, during, and after

118 ntial for enhancing the performance of Sm-Co magnets, but experiments and theory have not yet converg

119 e magnetization switching of a perpendicular magnet by utilizing an Iridium (Ir) layer.

120 ) for high-field copper oxide superconductor magnets by achieving a field twice as high as those gene

121 he giant magnetoelectric effect in permanent magnets by engineering grain boundaries with hydrogen at

122 ent synthesis of lightweight, molecule-based magnets by postsynthetic reduction of preassembled coord

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

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

125 ding molecular magnetic sponges, luminescent magnets, chiral magnets and photomagnets, SHG-active mag

126 The van der Waals magnet chromium triiodide (CrI(3)) has been shown to be

127 ucidate the topology of the room temperature magnet Co(2)MnGa.

128 explore magnetic correlations in the kagome magnet Co(3)Sn(2)S(2).

129 engineered quantum impurity in a topological magnet Co(3)Sn(2)S(2).

130 h and effect of electronic correlations in a magnet Co(3)Sn(2)S(2).

131 recent discovery of meron lattice in chiral magnet Co(8)Zn(9)Mn(3) raises the immediate challenging

132 ness of the nanoparticle aggregate, near the magnet compares well with the theoretical prediction.

133 Both Magnets components, which are well-tolerated as protein

134 rrors in the MIT 1.3-GHz high-resolution NMR magnet composed of an 835-MHz HTS insert, while another

135 n the presence of an external Fe(14) Nd(2) B magnet, concomitant with the introduction of a concentra

136 edictable locations, the quenches of Bi-2212 magnets consistently occurred in the high field regions

137 alization of paramagnetic particles near the magnet decreases with increasing the strength of the mag

138 Magnets derived from inorganic materials (e.g., oxides,

139 ls (OR 0.62, 95% CI 0.39-0.99, P = 0.045) or Magnet designated hospitals (OR 0.45, 95% CI 0.29-0.71,

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

141 sal that is still conceptual in conventional magnets due to the limited strain-tuning range of the co

142 anisotropic dysprosium-based single-molecule magnet [Dy(Tp(py))F(pyridine)(2)]PF(6).

143 Applications include magnets, electron nematics, and quantum gases.

144 We validated these 'enhanced' Magnets (eMags) by using them to rapidly and reversibly

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

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

147 cused on their application as molecule-based magnets exhibiting long-range magnetic ordering resultin

148 ade in the theoretical understanding of such magnets, experimental realizations of this low-dimension

149 photocatalyst can be recycled and reused by magnet extraction.

150 strain is applied to thin flakes of the vdW magnet Fe(3) GeTe(2) (FGT), and a dramatic increase of t

151 form (REOs) from a wide range of end-of-life magnet feedstocks including hard disk drives (HDDs), MRI

152 cessing larger quantities of different scrap magnet feedstocks with a membrane area of more than 1 m(

153 or fabrication of high-performance permanent magnets, flexible magnets, and printable magnetic inks f

154 for future design innovations in high-field magnets for accelerators and compact fusion reactors, an

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

156 new opportunities to explore these ultrathin magnets for such applications.

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

158 lso different from Nb-Ti, Nb(3)Sn, and REBCO magnets for which localized thermal runaways occur at un

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

160 ian for the quasi-one-dimensional (1D) Ising magnet [Formula: see text] that captures detailed and hi

161 in the low T state of the pyrochlore quantum magnet [Formula: see text] While magnetic Bragg peaks ev

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

163 g to the advantages of integration and being magnet-free and light-weight, the switched-capacitor-con

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

165 structing quench-predictable superconducting magnets from Bi-2212.

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

167 skyrmions in the centrosymmetric tetragonal magnet GdRu(2)Si(2) without a geometrically frustrated l

168 The 122-kg low-field (80 mT) magnet has a Halbach cylinder design that results in a m

169 Extensive work on single molecule magnets has identified a fundamental mode of relaxation

170 Along these lines, several kagome magnets have appeared as the most promising platforms.

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

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

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

174 phenomena, represents a unique van der Waals magnet in the family of metallic 2D transition-metal dic

175 possibilities for the use of two-dimensional magnets in nonlinear and nonreciprocal optical devices.

176 rature realization of a singlet ground state magnet, in which magnetism occurs through a process that

177 stom 6-well cultureware with toroidal shaped magnets incorporated in the base of each well for confor

178 e use of a 31-megawatt, 33.6-tesla resistive magnet inside 11.4-tesla low-temperature superconductor

179 ce based on the Nernst geometry, an external magnet is required as an integral part.

180 current density is possible only because the magnet is wound without insulation(4), which allows rapi

181 bench-scale breakthrough curve with a NdFeB magnet leachate revealed a two-bed volume increase in br

182 For the Ising magnet LiHo(0.045)Y(0.955)F(4), the quality factor Q for

183 ample is spin liquid formation in frustrated magnets like Dy(2)Ti(2)O(7).

184 Most HTS magnets made so far have been made out of REBCO coated c

185 This study suggests that HT of LHC magnets, made of reduced-Sn wires having a Nb/Sn ratio o

186 The HTS shim coil is placed inside the HTS magnet, mainly for ultra-high-field (> 1 GHz or 23.5 T)

187 The internal magnetization of magnets means that the electrical Hall effect can occur

188 c fields in superconducting energy-efficient magnets means we must understand and control the high se

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

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

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

192 through the magnetic transition of permanent magnet nanoparticles.

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

194 at became possible with the appearance of 2D magnets, offering new perspectives in this rapidly expan

195 All superconductors in high field magnets operating above 12 T are brittle and subjected t

196 spin state without freezing into an ordered magnet or a spin glass at low temperatures.

197 magnetic particles either aggregate near the magnet or diffusive away from the magnet, respectively.

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

199 roscopy but also for the design of molecular magnets or quantum computing devices.

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

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

202 hese limitations by engineering an optimized Magnets pair requiring neither concatemerization nor low

203 he conceptualized strategy utilizes a simple magnet placed beneath the three-dimensional printed LF d

204 erties in the non-centrosymmetric spin-orbit magnet PrAlGe by combining spectroscopy and transport me

205 Quantum magnets provide the simplest example of strongly interac

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

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

208 romising design strategy for next-generation magnets relies on the versatile coordination chemistry o

209 However, Magnets require concatemerization for efficient response

210 milestones and key advances in metal-organic magnet research that laid the foundation for structurall

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

212 07mugdL(-1) in the absence and presence of a magnet, respectively.

213 e near the magnet or diffusive away from the magnet, respectively.

214 reveal that the magnetization state in Sm-Co magnets results from curling instabilities and domain-wa

215 specific rungs, the structural integrity of magnet rungs would not be compromised.

216 In the present work, enhanced single-chain magnet (SCM) behavior is observed for a Mo(III) -Mn(II)

217 of Nb-Ti and Nb(3)Sn magnets, these Bi-2212 magnets showed no training quenches and entered the flux

218 three-dimensional (3D) conductive single-ion magnet (SIM), (TTF)(2) [Co(pdms)(2) ] (TTF=tetrathiafulv

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

220 vibrational properties of a single-molecule magnet (SMM) incorporating Dy(III) , namely [Dy(Cy(3) PO

221 llenge in the advancement of single-molecule magnet (SMM) research.

222 operties of a Dy(III) -based single-molecule magnet (SMM).

223 t examples of single-molecule and single-ion magnets (SMMs and SIMs) as well as molecular spin qubits

224 Single-molecule magnets (SMMs) are metal complexes with two degenerate m

225 Single-molecule magnets (SMMs) have potential applications in high-densi

226 bipyramidal dysprosium(III) single-molecule magnets (SMMs) with high anisotropy barriers of U(eff) =

227 underpins the development of single-molecule magnets (SMMs), a family of magnetic materials that can

228 previously reported Mn(2) Mo single-molecule magnets (SMMs).

229 some extent on the composition of the scrap magnet source.

230 ates, interaction-driven insulators, orbital magnets, states with non-zero Chern numbers and supercon

231 uperconductors (HTS) could enable high-field magnets stronger than is possible with Nb-Ti and Nb(3)Sn

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

233 broad range of applications, these inorganic magnets suffer several drawbacks, including energeticall

234 etization-switching paradigm of pinning-type magnets, suggesting a critical reconsideration of engine

235 rsity of Munich using a Gas-Filled Analyzing Magnet System (GAMS) and a 14 MV Tandem accelerator is g

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

237 The compactness of the BiSb-magnet system with high ZT enables the utilization of ma

238 oscopy, we identify a new topological kagome magnet, TbMn(6)Sn(6), that is close to satisfying these

239 organic solids that have dominated permanent magnet technology for decades, metal-organic frameworks

240 ntly developed series-connected hybrid (SCH) magnet technology.

241 nstrate an exception in a disordered quantum magnet that divides itself into nearly isolated subsyste

242 and describes recently discovered molecular magnets that can be regarded, currently, as defining the

243 ns have so far been observed in a variety of magnets that exhibit nearly parallel alignment for neigh

244 k crystals and present an overview of the 2D magnets that have been explored recently.

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

246 On a 1.5 Tesla magnet, the imaging protocol consisted of three sequence

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

248 In two-dimensional magnets these effects manifest themselves in the large m

249 le training performance of Nb-Ti and Nb(3)Sn magnets, these Bi-2212 magnets showed no training quench

250 wly discovered rare-earth triangular-lattice magnet TmMgGaO(4).

251 sla inside a 31.1-tesla resistive background magnet to obtain a d.c.

252 sla inside a 31.1-tesla resistive background magnet to obtain a d.c. magnetic field of 45.5 tesla-the

253 a novel concept of applying reverse bending magnets to adjust the energy-dependent path length diffe

254 ue opportunities provided by two-dimensional magnets to control the combined time-reversal and invers

255 levitation setup consisting of two opposing magnets to create a gradient of a magnetic field, a glas

256 class of materials, ranging from insulating magnets to superconductors.

257 form for increasing the applicability of vdW magnets to the field of spin-based electronics.

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

259 The magnet uses a conductor tape coated with REBCO (REBa(2)C

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

261 structures of two-dimensional Van der Waals magnets using continuum field theory.

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

263 The organic-based magnet [V(TCNE)(x) ; TCNE = tetracyanoethylene; x ~ 2] h

264 The 45.5-tesla test magnet validates predictions(11) for high-field copper o

265 We designed mAGNET viral vectors containing a CaMKIIalpha promoter a

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

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

268 medical syringe (5 mL) prefabricated with a magnet was used for in situ separation of the enzyme-cap

269 Neodymium magnet was used for separation of analyte ions.

270 e earth elements (REEs) from scrap permanent magnets was demonstrated by processing larger quantities

271 On the surface of the magnet, we observe electronic wave functions that take t

272 d the solution is transferred to a secondary magnet where strongly enhanced magnetic resonance signal

273 avior is expected for the majority of 2D vdW magnets where higher-order exchange interactions are app

274 into a receiving structure in the secondary magnet, where the bullet is retained and the polarized s

275 nductors, they are unexplored in topological magnets which can feature spin-orbit tunability.

276 ties and metal-ligand covalency in molecular magnets, which has implications in areas such as magneti

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

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

279 ring temperatures of metal-organic framework magnets while maintaining structural integrity and addit

280 other version for an MIT 1-GHz microcoil NMR magnet whose small-scale model we are currently building

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

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

283 compact and lightweight permanent rare-earth magnet with a built-in readout field gradient.

284 2) @C(79) N is found to be a single-molecule magnet with a high 100-s blocking temperature of magneti

285 imensional magnetization in a two-phase bulk magnet with a lateral spatial resolution of 50 nm.

286 Here, Rh(2) CoSb is introduced as a new hard magnet with potential for thin-film magnetic recording.

287 The Fe(18)Dy(6) CCC is a Single Molecule Magnet with the highest nuclearity among Ln containing c

288 ly that this compound is a highly frustrated magnet with unusual magnetic phase behaviours.

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

290 shinskii-Moriya interaction, centrosymmetric magnets with a triangular lattice can also give rise to

291 The seamless integration of 2D magnets with dissimilar electronic and photonic material

292 Pinning-type magnets with high coercivity at high temperatures are at

293 asses of ferromagnetic materials, rare-earth magnets with high intrinsic coercivity and antiferromagn

294 attributes, the realization of metal-organic magnets with high ordering temperatures represents a for

295 is crucial to the design of single-molecule magnets with improved properties, yet such studies on mu

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

297 potential to deliver new types of molecular magnets with previously unseen properties and applicatio

298 Our study predicts that two-dimensional magnets with weak spin-orbit coupling can be a promising

299 her reveals monolayer VSe(2) as a frustrated magnet, with its spins exhibiting subtle correlations, a

300 y experiments with a liquid jet at a bending magnet X-ray beamline demonstrate the feasibility of the