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1 any single-molecule magnet or molecule-based magnetic material.
2 ferromagnets may seem to behave like any non-magnetic material.
3 s considered the next-generation quantum and magnetic material.
4 ed through magnetic exchange coupling with a magnetic material.
5 s well as three-dimensional visualization of magnetic material.
6 hm of MTQC to determine the topology of each magnetic material.
7 pen-source code for diagnosing topologies of magnetic materials.
8 een developed by combining ferroelectric and magnetic materials.
9 ey to this new generation of multifunctional magnetic materials.
10 thereby improving our understanding of real magnetic materials.
11 such as water ice, spin ice, and frustrated magnetic materials.
12 associated with external magnetic fields or magnetic materials.
13 the directed synthesis of semiconducting and magnetic materials.
14 organizing nanowires from semiconducting and magnetic materials.
15 transition metal--containing electronic and magnetic materials.
16 delines for improving these high-performance magnetic materials.
17 ich will open new avenues in the field of 2D magnetic materials.
18 dict properties of such two-dimensional (2D) magnetic materials.
19 ology platform to advance the search for new magnetic materials.
20 re predominantly considered zero-dimensional magnetic materials.
21 ound in naturally occurring biomolecules and magnetic materials.
22 rgent field of two-dimensional van der Waals magnetic materials.
23 etry breaking magnetic order parameter of 2D magnetic materials.
24 copic scale in numerous application-relevant magnetic materials.
25 se for proton-based magneto-ionic control of magnetic materials.
26 ble spin structures that naturally emerge in magnetic materials.
27 hicles for the scalable synthesis of complex magnetic materials.
28 s will be important for ultrafast probing of magnetic materials.
29 esses, including the shaping/cutting of soft magnetic materials.
30 including the nature of the ground state in magnetic materials.
31 nveil the crucial roles of chiral phonons in magnetic materials.
32 tions as refractory coatings, catalysts, and magnetic materials.
33 have richer spin Hall properties than do non-magnetic materials.
34 but also in other settings such as laser and magnetic materials.
35 arning models to accelerate the discovery of magnetic materials.
36 tive and memory effects for a broad class of magnetic materials.
37 f new nd-4f single-molecule magnets and bulk magnetic materials.
38 iscover emergent topological solitons in non-magnetic materials.
39 ng interatomic potential for multi-component magnetic materials.
40 resents a step toward functional topological magnetic materials.
41 but also be of interest for realizing new 2D magnetic materials.
42 he design of high-performance molecule-based magnetic materials.
43 radicals is important for the development of magnetic materials.
44 ns, in particular as spin probes and organic magnetic materials.
45 structures, and introducing magnetism in non-magnetic materials.
46 er the system parameters than is possible in magnetic materials.
47 etization state of conducting and insulating magnetic materials.
48 ials, including polymers, semiconductors and magnetic materials.
49 near magnetostructural phase transitions in magnetic materials.
50 g and selective physical vapor deposition of magnetic materials.
51 ake it imperative to explore rare earth free magnetic materials.
52 otential as novel, rare-earth free permanent magnetic materials.
53 etism allowed light to be used as a probe of magnetic materials.
54 ipulation of the magnetization in engineered magnetic materials.
55 is responsible for a variety of phenomena in magnetic materials.
56 a feasible new route in realizing functional magnetic materials.
57 atures and also a basis for novel functional magnetic materials.
59 yer exchange interactions in two-dimensional magnetic materials(15-18), we demonstrate a coexisting f
60 agnetic materials while tin entered into non-magnetic materials; (2) The tin-enriched non-magnetic ma
62 se results mark a crucial step in making vdW magnetic materials a viable choice for the development o
63 is using mixed-valence iron hydroxide as the magnetic material, a deep eutectic solvent as the coporo
64 rostructures formed by stacking together two magnetic materials, a ferromagnetic topological insulato
65 ted a high-throughput search for topological magnetic materials across 522 new, experimentally report
68 These devices are now smaller, with less magnetic material and improved electromagnetic interfere
69 ich is a record for a rare earth- or Pt-free magnetic material and retain values as high as 17.1 MGOe
70 coercivity are key properties of functional magnetic materials and are generally associated with rar
71 stals composed of metals, semiconductors, or magnetic materials and capped with various MCC ligands c
74 This is essential for the design of new bulk magnetic materials and for diminishing processes such as
76 This approach overcomes the limitations of magnetic materials and it does not require an external m
77 -reversal symmetry, typically achieved using magnetic materials and more recently using the quantum H
78 as originally studied as Barkhausen noise in magnetic materials and now is used in diverse fields fro
79 ailoring molecular spinterface between novel magnetic materials and organic semiconductors offers pro
81 magnetic inverse SHE) that are absent in non-magnetic materials and that can be dominant in some magn
84 ce planarity but also the homogeneity of the magnetic materials, and our method is likely to find imm
85 nt magnetocaloric effects in a wide range of magnetic materials, and the parallel development of nano
99 alization of topological semimetal states in magnetic materials at room temperature, but also suggest
100 le very efficient electrical manipulation of magnetic materials at room temperature, for memory and l
102 to cobalt introduces potential new routes to magnetic materials based on strongly coupled, triangular
103 gation of disordered or distorted as well as magnetic materials, because it is not based on symmetry
104 to create an effective magnetic field in the magnetic material being probed, which makes it possible
106 etic anisotropy has been explored in various magnetic materials, but the efficient electric-field con
107 lver chalcogenides, Ag2Se and Ag2Te, are non-magnetic materials, but their electrical resistance can
108 s been the method of choice to magnetize non-magnetic materials, but they are difficult to focus.
109 g-standing goal to create magnetism in a non-magnetic material by manipulating its structure at the n
110 ddition improves the performance of the hard-magnetic material by mitigating Brown's paradox in magne
113 ular, geometrical frustration among spins in magnetic materials can lead to exotic low-temperature st
115 ructures that combine natural and artificial magnetic materials, can play a key role in terahertz dev
116 torage and separation, optical, electric and magnetic materials, chemical sensing, catalysis, and bio
120 plied this methodology to more than 4835 non-magnetic materials consisting of heavy atoms and low ban
121 the physical and magnetic properties of the magnetic material constituents and fabrication processes
122 to create a comprehensive, experiment-based, magnetic materials database named the Northeast Material
125 nets (SMMs), which are an important class of magnetic materials due to their nanometre size, remain u
129 agnetism can remove this obstacle, as chiral magnetic materials exhibit magneto-chiral dichroism, a d
131 e as building blocks for obtaining molecular magnetic materials exhibiting an additional and useful p
133 esis of colloidal nanostructures combining a magnetic material (FePt) with a narrow-gap semiconductor
134 prepared in the L1(0) phase, as a promising magnetic material for biomedical applications with super
135 which in turn expands the base of available magnetic materials for devices with properties that cann
136 ticles (including metals, semiconductors and magnetic materials) form stable colloids in various molt
139 cond-order magnetic phase transition in soft magnetic material, gadolinium, was employed to obtain me
140 ects of magnetic disorder and frustration in magnetic materials generally, but also highlight as desi
141 current technology, a search for a low-cost magnetic material has been more important than ever.
142 gh unconventional methods without the use of magnetic material has recently become a subject of great
144 er, the limited availability of intrinsic 2D magnetic materials has driven efforts to induce and mani
146 nderstood as voltage-driven ion transport in magnetic materials, has largely relied on controlled mig
152 agnetic insulators are a ubiquitous class of magnetic materials, holding the promise of low-dissipati
154 ow that by embedding nanoparticles of a soft magnetic material in a thermoelectric matrix we achieve
155 ice is mimicked by Dy2Ti2O7, a site-ordered magnetic material in which the spins reside on a lattice
156 coupling self-assembly to the generation of magnetic materials in a simple, straight-forward manner
157 Nonreciprocal optical elements often require magnetic materials in order to break time-reversal symme
158 pproach to carry out an efficient search for magnetic materials in the Bilbao Crystallographic Server
162 transition materials, photomagnets, solvato-magnetic materials, including molecular magnetic sponges
163 ration and is readily implementable to other magnetic materials independent of their size and shape a
164 nical exchange coupling between Fe and Ni in magnetic materials influences magnetic switching dynamic
165 One currently active area of research in magnetic materials involves compounds in which long-rang
166 Our finding shows that optical control of magnetic materials is a much more general phenomenon tha
167 or spin-electric coupling) in molecule-based magnetic materials is a relatively nascent but promising
169 bility to rapidly manipulate domain walls in magnetic materials is key to developing novel high-speed
173 fect, extraordinarily strong among other non-magnetic materials, is traced back to the specific Dirac
175 ontaneously broken time-reversal symmetry in magnetic materials leads to a Hall response, with a nonz
177 metal-to-insulator resistive switching in a magnetic material, local on/off control of ferromagnetis
179 e interplay between symmetry and topology in magnetic materials makes it possible to engineer exotic
181 spin-dependent thermoelectric properties of magnetic materials, novel means of generating spin curre
183 temperature for any metal boride and for any magnetic material of the vast 122 family of layered stru
185 angement of spins at interfaces in a layered magnetic material often has an important effect on the p
188 superconductors with strongly spin-polarized magnetic materials opens the possibility to discover new
191 esigning new rare-earth-free (REF) permanent magnetic materials (PMM) to replace the high performing
193 Similarly, the interaction of X-rays with magnetic materials provides unique element-specific cont
194 chiral magnets and photomagnets, SHG-active magnetic materials, pyro- and ferroelectrics, ionic cond
195 lizable optical readout method for molecular magnetic materials, reinforcing its potential for future
196 to targeted stimuli, they displace attached magnetic material relative to the phone's magnetometer.
199 previous research has focused mainly on non-magnetic materials, so the magnetic contribution to the
202 roperties in a broad range of high-frequency magnetic materials such as two-dimensional magnets, spin
204 hniques to characterize other nanostructured magnetic materials, such as nanoparticles, is also revis
205 quest for a novel low-dimensional metal-free magnetic material that would exhibit magnetism at a high
206 re familiar realm of polymers, colloids, and magnetic materials that all exhibit thermal fluctuations
207 single-molecule magnets (SMMs), a family of magnetic materials that can retain magnetization in the
210 have revealed extraordinary spin dynamics in magnetic materials that equilibrium descriptions of magn
211 lassification of collinear, spin compensated magnetic materials that host net-zero magnetization yet
212 niobium magnet and, after discarding the non-magnetic material, the copper(II) ions were eluted with
218 nual disassembly allows in principle for all magnetic material to be recovered, shredding leads to ve
219 rporating newly discovered ferroelectric and magnetic materials to engineer symmetries and add a new
221 idase mimic for analyte detection), and as a magnetic material (to simplify the (bio)-sensing steps).
222 overy of emergent magnetism in van der Waals magnetic materials (vdWMM) has broadened the material sp
224 ef that grain boundaries are "weak links" in magnetic materials, we demonstrate grain boundaries unde
225 magnetic materials; (2) The tin-enriched non-magnetic materials were briquetted with CaCl(2) and anth
226 ve devices requires high-quality low-damping magnetic materials where magnon spin currents can effici
228 nsition metal centers are a diverse class of magnetic materials where the spin density and ordering b
229 ens a new realm of possibility for molecular magnetic materials, where their unprecedented localized
230 ver, most soft machines are limited to solid magnetic materials, whereas further progress also relies
231 fficient spin detection without the need for magnetic materials, which could lead to useful spintroni
232 n process, and 90.8 wt% iron was enriched in magnetic materials while tin entered into non-magnetic m
233 nt with arbitrary polarization using typical magnetic materials will benefit the development of magne
234 nding and control of the dynamic response of magnetic materials with a three-dimensional magnetizatio
235 ffect was considered excluded in compensated magnetic materials with collinear ordering, in the recen
236 other hand, disordered freezing of spins in magnetic materials with decreasing temperature, the so-c
238 The FePt/ferritin assemblies are integrated magnetic materials with ferritin providing added magneti
239 study indicates ingredients for engineering magnetic materials with high angular sensitivity by latt
241 ent important case studies in the pursuit of magnetic materials with inherently larger magnetic momen
242 y accomplished through the use of inherently magnetic materials with large magnetic permeability, suc
247 ociation reported here of the assembled soft magnetic materials with tuneable sizes could be interest
248 by integrating monolithic ferroelectric and magnetic materials, with interfacial coupling between el
249 l Hall effect has rarely been studied in non-magnetic materials without external magnetic fields, owi