ライフサイエンスコーパス: topological

1 ovalent organic frameworks (COFs) results in topological [2 + 2] cycloaddition cross-linking of the p

2 an assess white matter connections revealing topological alterations in multiple sclerosis (MS).

3 Topological analysis and simulation modeling of the netw

4 The retrosynthesis plans that emerge from a topological analysis of the highly bridged frameworks of

5 The interface between topological and normal insulators hosts metallic states

6 an optimal overlap of points sharing similar topological and pharmacophoric neighborhoods.

7 rminus of the CCSSD, a previously unobserved topological arrangement of this domain.

8 ent conclusions: the global absence of local topological-associated domains (TADs) in gametes and the

9 By combining topological band and superconductivity in a single mater

10 e in the edge currents of 2-dimensional (2D) topological band insulators with broken time-reversal sy

11 been performed to question the nature of the topological barriers at play, leading to several predict

12 protein-DNA complexes to efficiently work as topological barriers.

13 such a domino reaction is examined within a topological-based bonding evolution theory perspective.

14 nctionalities, appealing for devising future topological-based nanoelectronics.

15 ising the question of whether there exists a topological bulk-boundary correspondence for Dirac semim

16 We find that the network topological centrality and clustering performance of SCI

17 r model by suggesting that the force-induced topological change of TMDs and subsequent alteration in

18 low threshold T cells were also sensitive to topological changes of the animal surface, caused by con

19 Our analyses suggest that these topological changes repress stemness and invasion progra

20 The discovery of flat electronic bands with topological character in magic-angle twisted bilayer gra

21 riety of unusual features arising from their topological character, including "fractionalization"-ele

22 Finally, the analysis of topological characteristic like bottleneck, degree, GO t

23 We introduce a topological characterization, the hub-set-orientation pr

24 an form spin textures that carry non-trivial topological charge(8) resembling magnetic meron quasipar

25 eptional points (EPs), which carry a nonzero topological charge, can emerge in non-Hermitian systems.

26 r, providing chiral light states of variable topological charges at a single telecommunication wavele

27 ical Fermi arcs that correspond to projected topological charges of +/-1 in the surface Brillouin zon

28 ure: they emerge when a pair of half-integer topological charges(1-3) in the polarization field bounc

29 o-vortex phase transition, and signatures of topological chiral one-way edge currents, completely in

30 model can be parameterized to match the five topological classes encompassing all amyloid fibril stru

31 Attributed to the unique topological complexity and elegant beauty, Borromean sys

32 This review presents the topological concepts related to solids from the viewpoin

33 he surface Fermi arcs in Weyl semimetals are topological consequences of the Weyl points themselves,

34 Overall, we show that NetPAS can take topological constraints of molecular networks into accou

35 We quantitatively analyze the topological constraints on RNA 3D conformational space,

36 d) tertiary contacts can cause much stronger topological constraints on RNA global fold than non-cros

37 This unique aspect of topological control gives rise to highly versatile edge

38 omagnetic spin systems, we identified simple topological counting rules to predict the relative mecha

39 lix size, and loop size, indicating a strong topological coupling between helices and loops in RNA te

40 topological insulator: axion insulator, AFM topological crystalline insulator (TCI), and higher orde

41 Topological crystalline states (TCSs) are short-range en

42 We propose a new method based on Topological Data Analysis (TDA) consisting of Topologica

43 Here we introduce methods based on topological data analysis and interpretable machine lear

44 monolayers in an automatic manner, we apply topological data analysis to experimental data and to re

45 Topological data analysis using human epithelial transcr

46 Topological data analysis was used to visualize the data

47 sus cluster distribution, bootstrapping, and topological data analysis were applied.

48 xperimental binding affinities, we introduce topological data analysis, a variety of network models,

49 Topological defects are a consequence of broken symmetry

50 The impact of topological defects associated with grain boundaries (GB

51 For example, motile, point-like topological defects capture the salient features of two-

52 deliberately create high-density homogeneous topological defects in carbon networks due to the high f

53 activity, enabling temporary aggregations of topological defects in cell packing.

54 Finally, by visualizing the topological defects in these N(r, E) density waves at 2Q

55 and antimerons, into a plethora of composite topological defects such as the fourfold junctions, the

56 ral organization of biological systems, such topological defects were never reported in epithelia.

57 eptors at the rim of the hemispheric retina, topological defects, called "Y-Junctions", form to maint

58 ven by the (re)combination of the elementary topological defects, merons and antimerons, into a pleth

59 Topological defects, with an asymmetric local electronic

60 ous carbon particles, to create high-density topological defects.

61 , chirality, boundary conditions and induced topological defects.

62 l enable more quantitative insights into the topological determinants of transcriptional control and

63 rovide an enlarged platform for the quest of topological Dirac fermions in a magnetic system.

64 is disordered-crystalline switch between two topological distinct metal-organic frameworks is shown t

65 er local rules governing the identity of the topological domains and their boundaries.

66 lfolobus archaea are organized into CID-like topological domains in addition to previously described

67 ion of clustered pathway genes into distinct topological domains is a common feature in plant genomes

68 by facultative heterochromatin and insulated topological domains that form separately within individu

69 process complexity in both the temporal and topological domains, testing them on functional MRI BOLD

70 es are required to create stable independent topological domains.

71 l knots and an experiment which maps out the topological drumhead region of a Hopf-link.

72 Topological edge modes are excitations that are localize

73 ere, we investigate the properties of the 1D topological edge state of bismuth in the absence of TRS,

74 correspondence between the Chern gap and the topological edge state, as well as the Berry curvature f

75 ly match with theoretical expectations for a topological edge state, having one Kramer's pair of band

76 tum spin Hall effect in one-dimensional (1D) topological edge states, where quasiparticle backscatter

77 9) indicates that the effect arises from the topological edge states, which drive a change in sign of

78 e variety of observable magneto-electric and topological effects.

79 he synthesis of width-modulated GNRs hosting topological electronic quantum phases, with valence elec

80 A giant nontrivial topological energy window and a long topological surface

81 Thus, the topological engineering approach enriches the toolbox fo

82 gh-efficiency catalysts with the strategy of topological engineering of excellent transitional cataly

83 The primary topological excitations are extended, charge-neutral dis

84 dicating the importance of this higher-order topological feature for conscious cognition.

85 The key topological feature in these insulators is instead fract

86 A simple topological feature, the local ID, is thus sufficient to

87 o study the spatial patterns arising on this topological feature, we use a one-dimensional lattice mo

88 al bound states in the continuum (BICs) with topological features and conducted an in-depth character

89 Knots are remarkable topological features in nature.

90 -ray tomography to study the geometrical and topological features of disordered packings of rubber ba

91 ther, our results reveal a unique network of topological features that coalesce around a histone tetr

92 We find that this network exhibits several topological features that favor high functional redundan

93 isting predictors that require structural or topological features which might not be readily availabl

94 copy below the Curie temperature, we observe topological Fermi arcs that correspond to projected topo

95 The preTCR topological fit ensures that CDR3beta reaches the peptid

96 s into leukemia cells, but further uncover a topological framework of a molecular mechanism for oncog

97 We observe a topological Hall effect at the boundary of the phase tra

98 Transport measurements show the topological Hall effect in this heterostructure for temp

99 Topological helical polaritons provide a platform for de

100 olitons, Hopfions, that are characterized by topological Hopf invariant, attract an intense attention

101 opological Data Analysis (TDA) consisting of Topological Image Modification (TIM) and Topological Ima

102 of Topological Image Modification (TIM) and Topological Image Processing (TIP) for object detection.

103 e the usefulness of this proposed method for topological image processing through a case-study of uns

104 ectional guided resonances', are found to be topological in nature: they emerge when a pair of half-i

105 Using the topological information provided by the SOM, RPM provide

106 Our results not only provide novel topological insights for the roles of PML-RARalpha in tr

107 malous Hall (QAH) state is a two-dimensional topological insulating state that has a quantized Hall r

108 ing properties such as near-room-temperature topological insulation in bismuthene, extremely high ele

109 nosecond motion of water at the surface of a topological insulator (TI), Bi[Formula: see text]Te[Form

110 demonstrate a reconfigurable electroacoustic topological insulator exhibiting an analog to the quantu

111 ulation of magnetic and topological order in topological insulator films.

112 nomalous Hall effect in a magnetically-doped topological insulator grown on the antiferromagnetic ins

113 he lowest possible dimension for achieving a topological insulator in this class.

114 rs or the thickness of the interior magnetic topological insulator layer.

115 agnetic doping concentration in the magnetic topological insulator layers or the thickness of the int

116 s are able to reduce this higher-dimensional topological insulator phenomena to lower dimensionality

117 ulator was recently demonstrated in magnetic topological insulator sandwich samples.

118 and no mixed valency), YbB(6) (mixed valent topological insulator), and rather ordinary LaB(6) .

119 and [Formula: see text] [Formula: see text] (topological insulator).

120 reciprocal charge transport(3) in a magnetic topological insulator, Cr-doped (Bi,Sb)(2)Te(3).

121 ile topological states at a surface, i.e., a topological insulator-air/vacuum interface, have been st

122 result of nonlinearity-in a photonic Floquet topological insulator.

123 rystalline insulator (TCI), and higher order topological insulator.

124 el state containing three different types of topological insulator: axion insulator, AFM topological

125 Recently introduced quantized multipole topological insulators (QMTIs) reveal new types of gappe

126 Magnetic topological insulators (TI) provide an important materia

127 Emergent topological insulators (TIs) and their design are in hig

128 Here, the strong SOC from topological insulators (TIs) is utilized to provide a la

129 Here we show that chalcogenide topological insulators are particularly apt candidates f

130 The boundary modes of topological insulators are protected by the symmetries o

131 Recently, mechanical topological insulators have sought to overcome this chal

132 ogical materials, such as the quintessential topological insulators in the Bi(2)X(3) family (X = O, S

133 and magnetization measurements of the doped topological insulators Nb(x)Bi(2)Se(3) and Cu(x)Bi(2)Se(

134 rotected boundary states that are themselves topological insulators of lower dimensions, have recentl

135 manifest themselves in momentum space, as in topological insulators or in strong Rashba materials.

136 This is demonstrated for 3D topological insulators, 3D Dirac materials, and 1D quant

137 ial insulators, semimetals, and metals or as topological insulators, Dirac and Weyl nodal-line semime

138 several topical materials systems, including topological insulators, transition metal dichalcogenides

139 mented by the EAs, the EX possesses a hybrid topological invariant (HTI), which consists of distinct

140 erials' edges and yet are characterized by a topological invariant defined in the bulk.

141 d nodal band degeneracies characterized by a topological invariant known as the Chern number (C).

142 uction of the Seifert surface and hence knot topological invariants like the Alexander polynomial.

143 s structural polyprotein forms two competing topological isomers during its biosynthesis at the ribos

144 ing tunnelling microscopy, we identify a new topological kagome magnet, TbMn(6)Sn(6), that is close t

145 Unlike topological lasers that rely on large-scale features to

146 rimentally implement a four-dimensional (4D) topological lattice.

147 Transcending different topological levels, proteins that controlled a large num

148 n (DMI) is responsible for exotic chiral and topological magnetic states such as spin spirals and sky

149 e skyrmion patterns, is the key to advancing topological magnetism.

150 r, which can be experimentally observed as a topological magneto-electric effect of inversion-broken

151 Here we integrated topological maps for colon tumors and normal colons with

152 es at a pai-phase shift DW in a proximitized topological material.

153 perty measurement techniques to characterize topological materials beyond their structure and provide

154 Topological materials offer a new avenue for energy harv

155 uantum devices by marrying the advantages of topological materials to versatile semiconductors.

156 aces, via symmetry and topology, classifying topological materials within a single-particle picture i

157 rstanding of and the search for paramagnetic topological materials(5,6).

158 The discoveries of intrinsically magnetic topological materials, including semimetals with a large

159 Topological materials, such as the quintessential topolo

160 stics can be a powerful tool to characterize topological matter.

161 We utilise a topological measure called the trophic incoherence param

162 s, Dirac and Weyl nodal-line semimetals, and topological metals.

163 under realistic conditions, the interfacial topological modes are delocalised over many lattice spac

164 Here we emphasize their topological nature and show that these self-patterned po

165 The topological nature of the quantum anomalous Hall effect

166 It is essential to understand how the topological nature of these materials changes with growt

167 By probing these states, we investigate the topological nature of tilt and shed light on novel trans

168 Because of their proposed topological nature, the surface states are of sufficient

169 applications derived from the chirality and topological nature.

170 The topological nodal-line semimetal (TNS) is a unique class

171 calculations, we report the observation of a topological nodal-loop (TNL) in SrAs(3), whereas CaAs(3)

172 It has been demonstrated that topological nontrivial surface states can favor heteroge

173 Vortices are topological objects representing the circular motion of

174 Despite the lack of significant topological or sequence similarity to their natural gran

175 (2), interacting quantum systems can exhibit topological order and are instead characterized by intri

176 ve been made to enhance our understanding of topological order by forming Laughlin states in syntheti

177 didates for the manipulation of magnetic and topological order in topological insulator films.

178 most integrative tools completely ignore the topological order of gene regulatory networks that hold

179 can be boosted significantly by introducing topological order.

180 to be an anchored membrane protein, but its topological organization is unknown, raising questions a

181 omposition, interactions, stoichiometry, and topological organization of proteins within IACs are not

182 BacA then serves as a stalk-specific topological organizer for PG synthesis activity, includi

183 Network topological parameters also reveal novel potential cellu

184 which can be complicated by the presence of topological permutations within a polypeptide chain and/

185 lectrons represent an SSH chain close to the topological phase boundary, i.e., when the intra- and in

186 f orbitals allows us to analytically compute topological phase diagrams, which determine quantized ob

187 Furthermore, we reveal topological phase transitions from higher- to lower-orde

188 tains to cosmological structure creation and topological phase transitions in quantum matter(10-12),

189 rimental observation of quantized quadrupole topological phase.

190 plification can be elegantly obtained from a topological 'phase diagram', which provides a guiding pr

191 which themselves represent lower-dimensional topological phases and host symmetry protected zero-dime

192 The instances in which topological phases emerge only as a result of strong int

193 ates the key role of dimensionality and dual topological phases in selecting desired spin properties,

194 ies crucially underlie the classification of topological phases of matter.

195 In particular, novel topological phases that can only exist in non-Hermitian

196 sulating, superconducting, ferromagnetic and topological phases(1-6).

197 pportunity to search for strongly correlated topological phases(2-9).

198 ed insulators(1-3), superconductors(2-4) and topological phases(3,5,6).

199 Quadrupole topological phases, exhibiting protected boundary states

200 f these materials display previously unknown topological phases, including symmetry-indicated magneti

201 sets an upper limit to the magnitude of many topological phenomena in these materials.

202 Topological photonics in strongly coupled light-matter s

203 th towards exploration of higher-dimensional topological physics with time as a synthetic dimension.

204 molecular weights <400 Da, log D(7.4) < 2.5, topological polar surface area < 75, ligand efficiency >

205 Topological polaritons, i.e., hybrid exciton-photon quas

206 The helical nature of the topological polaritons, where polaritons with opposite h

207 venumber in triangulated origami, preventing topological polarization but permitting a family of zero

208 it comes to the poly(monothiocarbonate)s, no topological polymers have been reported.

209 ers provides efficient and concise access to topological polymers.

210 involved ED_co-occurrences are in important topological positions in the network, suggesting relatio

211 resents a characteristic example of applying topological principles(4,5) to control optical fields an

212 bjects, and construct new objects with known topological properties in irrelevant regions of an image

213 Here we report the striking topological properties in the non-centrosymmetric spin-o

214 We investigate how the memory and topological properties influence the control effort by c

215 Under strong magnetic fields, the topological properties of Dirac/Weyl materials can direc

216 such as the size and morphology of domains, topological properties of domain walls or their thermal

217 We further develop a protocol in which the topological properties of framed knots are used in conju

218 The electronic and topological properties of materials are derived from the

219 Topological properties of materials are typically presen

220 exploratory graph theory analysis to compare topological properties of structural covariance networks

221 5HT2A-R density, but related closely to the topological properties of the brain's anatomical connect

222 The analysis of topological properties of the human histone interactome

223 th limited information about the chemical or topological properties of the ligand itself.

224 y the effects of long-term memory and of the topological properties on the minimum number of driven n

225 We show that the coupling of this material's topological properties to its magnetic texture leads to

226 ximant, and investigate their electronic and topological properties.

227 ain network, and subsequently quantifies its topological property using graph theory.

228 ates may open routes to the practical use of topological protection in electrically driven laser sour

229 Topological protection is a universal phenomenon that ap

230 that rely on large-scale features to impart topological protection, our compact design makes use of

231 ions have high physical stability because of topological protection.

232 Here we demonstrate a temporal topological pump that produces on-demand, robust transpo

233 Topological pumps are able to reduce this higher-dimensi

234 ariton hybridization and are controlled by a topological quantity.

235 Topological quantum chemistry(4) has enabled the underst

236 emerged as a promising Majorana platform for topological quantum computation.

237 For topological reasons, this led to the generation of four

238 However, the complex topological relationship of DOPA and Lys as well as the

239 by previous studies that used it to display topological relationships between different components o

240 Further topological remodeling of light and dark zone follicular

241 spite of the fact that the same physical and topological rules are involved in the structural organiz

242 Notably, these materials are topological semimetal candidates with symmetry-protected

243 tronic properties of the prototypical chiral topological semimetal PdGa.

244 , under modest magnetic fields or strain, to topological semimetallic behaviors.

245 Topological semimetals feature protected nodal band dege

246 optical and transport experiments in chiral topological semimetals.

247 scover magnetic and statistically disordered topological semimetals.

248 c platform: equivalent mapping occurs for 3D topological singularities such as Dirac-Weyl synthetic m

249 networks but also for data stream mining in topological space.

250 However, material realizations of topological spin states are still limited.

251 The emergence of magnetic skyrmions, topological spin textures, has aroused tremendous intere

252 ay be small, but drive the transition to the topological state for appropriate nodal structure of the

253 field revealed the quantum Hall effect(1), a topological state of matter featuring a finite Chern num

254 is crucial for understanding this correlated topological state.

255 experiment and theory to study such embedded topological states (ETSs) in heterostructures of GeTe (n

256 cuum interface, have been studied intensely, topological states at a solid-solid interface have been

257 While topological states at a surface, i.e., a topological ins

258 gases remain the only systems in which such topological states have been definitively observed(6,12-

259 ork offers a pathway to explore higher-order topological states in 3D classical platforms.

260 identify paths toward engineering chiral and topological states in centrosymmetric oxides through rar

261 in other classical systems, further study of topological states in graded materials, and the developm

262 oward a complete classification of amorphous topological states in real space using quasilocal proper

263 Building blocks are lower-dimensional topological states protected by onsite symmetries alone,

264 lications, it is crucial to manipulate these topological states under external stimuli.

265 This work may spark future investigations of topological states with complex wavenumbers in other cla

266 (RS) and the preferential resolution of DNA topological stress ahead of the fork.

267 ation, confirming that cohesin-dependent DNA topological stress impacts on normal replication progres

268 Topoisomerase II (TOP2) relieves topological stress in DNA by introducing double-strand b

269 ps in a new light as powerful and reversible topological stress relievers, an insight that significan

270 Tof1 in DRC signalling and resolution of DNA topological stress require distinct N and C terminal reg

271 can disrupt genome stability by trapping DNA topological stress.

272 ked to both the generation and repair of DNA topological-stress-linked damage in these regions.

273 The topological structure (3 D fiber hydrogel, 3 D GelMA hyd

274 erarchy discovery should be sensitive to the topological structure, reward distribution, and distribu

275 ed polycarbonates by modifying the polymer's topological structure.

276 es is explored, including the observation of topological structures and control of their structures a

277 rogress over the last decade in the study of topological structures in ferroic thin films and heteros

278 coherent single-electron transport through a topological superconducting island via a mechanism refer

279 ssibilities for realizing and characterizing topological superconductivity.

280 (2) is a strong candidate for chiral-triplet topological superconductivity.

281 , suggesting a promise route for engineering topological superlattices for high-performance TI-spintr

282 trivial topological energy window and a long topological surface FA are expected at the surface when

283 go a distinct maturation step during which a topological switch of the large envelope protein confers

284 mple quality and is readily adapted to other topological systems with antiperovskite structures.

285 r future studies of quantum fluid physics in topological systems.

286 aterial systems and push a new generation of topological technologies.

287 cidic microenvironment specifically inducing topological transformation from nanoparticles to organel

288 cult due to the lack of control over defined topological transformation of self-assembled structures.

289 son to de novo synthesis, this metal-induced topological transformation provides control over the for

290 ate for iron-based superconductors where the topological transition associated with creation of a Bog

291 and the math and physical science behind the topological transition on surface, thus can be used to c

292 to elliptical dispersion (corresponding to a topological transition), various intriguing phenomena ar

293 stigate theoretically and experimentally the topological transition, the polaritonic coupling and the

294 Topological transitions between considerably different p

295 We experimentally observe tunable topological transitions from open (hyperbolic) to closed

296 al decomposition via the sequential onset of topological transitions.

297 Topological transport phenomena usually appear at very l

298 Here, we propose a different topological understanding of metal and dielectric.

299 ical construction method yields an efficient topological way to control both the number of connected

300 Here we introduce the topological Weaire-Thorpe class of models, which are def