ライフサイエンスコーパス: singularity

1 lly decreased, which may lead to a "chemical singularity".

2 ed filaments are vortices (nodal lines/phase singularities).

3 of a disk through a "neck-pinching" boundary singularity.

4 hich transitions to two disks through a bulk singularity.

5 tional rate-limiting step responsible for OR singularity.

6 nvasively tracked in 3-dimension using phase singularity.

7 ude in the area surrounding the spiral phase singularity.

8 , competition between clusters would promote singularity.

9 ntal band associated with the E(22) van Hove singularity.

10 be neglected produces an exceptional form of singularity.

11 imental measurements of a collapsing surface singularity.

12 ts whose k-plane X-ray transform has a point singularity.

13 entrant arrhythmias via a mechanism of phase singularity.

14 e initiated or annihilated via a folded-node singularity.

15 ilation, the system becomes free of any band singularity.

16 ns for the physics of fluids converging to a singularity.

17 ribbons along closed loops around a central singularity.

18 disorganization, locations occupied by phase singularities.

19 breakdown of cyclotron motion near van Hove singularities.

20 eate light modes with phase and polarization singularities.

21 ion of the polarisations of the core and the singularities.

22 flows such as coalescence that also exhibit singularities.

23 the apex velocity and the curvature exhibit singularities.

24 s quickly and accurately, despite the corner singularities.

25 more sharpening near orientation preference singularities.

26 rify the dynamics of fluids approaching such singularities.

27 of slow wavefronts of reexcitation and phase singularities.

28 esent an episode of fibrillation by locating singularities.

29 rrupted by sharp jumps (fractures) and point singularities.

30 the phenomenon of reconnection of line-like singularities.

31 t with the energy separation of the van Hove singularities.

32 the form of a grating comprising a series of singularities.

33 points have been sampled precisely from the singularities.

34 tivation/feedback scheme suffice to generate singularity?

35 cal structures such as vortices(2), magnetic singularities(3) or skyrmion lattices(4).

36 At the center of a collapsing hole lies a singularity, a point of infinite curvature where the gov

37 , for example, involves a particular type of singularity-a ray catastrophe-in which light rays become

38 trains yields the material just ahead of the singularity, allowing it to propagate, leaving a furrow-

39 epresent functions that are smooth away from singularities along k-planes in Rn.

40 We find that this singularity also underlies knife-edge behaviour in alloc

41 We study spectral singularities and critical field enhancement factors ass

42 cs, such as its the Fermi velocity, van Hove singularities and electronic localization.

43 y large to enable identification of van Hove singularities and flat band segments in momentum space.

44 ion between the locations of orientation map singularities and local ocular dominance peaks similar t

45 stimulate extremely large field-intensity at singularities and then form two circular hotspots around

46 by simulations in one dimension that display singularities and topology and in part by two further de

47 allowing experimental access to the quantum singularity and a direct probe of the competition betwee

48 o that amplitude recovery is slower near the singularity and faster near the limit cycle; (iii) a dir

49 otated graphene layers introduces a van Hove singularity and flat bands near the Fermi energy that ca

50 au-level states are bound to the topological singularity and have energies that are universal functio

51 , no matter how small, cuts off this form of singularity and produces an unexpectedly long and slende

52 stochastically chosen OR may account for the singularity and robustness in OR transcription.

53 The link between this edge singularity and the states wrapping a three-dimensional

54 s for the formation and termination of these singularities, and represent an episode of fibrillation

55 we give a description of the structure, the singularities, and the divisor class group of all finite

56 of deprived-eye patches with pinwheel center singularities, and the selective loss of orientation tun

57 en the Fermi level passes through a Van Hove singularity, and open the possibility that the highly st

58 final Stokes dynamics that dominate near the singularity- and demonstrate that the crossover hole rad

59 In mice, this striking singularity appears to be ensured by a negative feedback

60 The polarization singularities are directly generated by using plasmonic

61 However, it remains unclear whether these singularities are generic to the REFeAsO-type materials

62 ide compelling evidence that pinwheel center singularities are important for cortical plasticity.

63 nderstanding of earlier work in which squirt singularities are ruled out; in this case, a positive vo

64 an easy and fast deployment with Docker and Singularity are also provided on GitHub.

65 Claims of singularity are therefore not well supported by the avai

66 a bilayer, it reveals a dominating van Hove singularity arising from interlayer coupling.

67 ic tree topology is scale-invariant due to a singularity arising from large niche construction fluctu

68 tions made it possible to create topological singularities as powerful templates for the precision as

69 n is given to the detection and treatment of singularities as well as discontinuities of the derivati

70 f electrons with momentum k and -k has a log singularity as the temperature decreases.

71 This method circumvents singularities associated with black holes and includes i

72 nonlinear optical systems, and gravitational singularities associated with black holes.

73 in which resonances arise from the van Hove singularities associated with the one-dimensional band [

74 this strong magnetism arises from a van Hove singularity associated with the direct Fe-Fe c-axis chai

75 m to maximize the distance between the phase singularities at each longitudinal plane, facilitating m

76 ction of low-temperature isokoms without any singularity at finite temperature.

77 The observation of the spectroscopic singularity at finite temperatures over a wide doping ra

78 thesis that liquid water's properties have a singularity at or near 228 K at ambient pressures.

79 Here, we report an antagonistic singularity at T(c) in the spectral weight of Bi2Sr2CaCu

80 rmi surface topology separated by a Van-Hove singularity at the Lifshitz transition point.

81 in the form of topological defects, or phase singularities, at a few sites.

82 n in failing ventricles, the number of phase singularities (baseline versus apamin, 4.0 versus 2.5),

83 Circadian singularity behavior (also called suppression of circadi

84 dian clock gene frequency (frq), can trigger singularity behavior in this organism.

85 Together, these data suggest that the singularity behavior is due to a circadian negative feed

86 Our results further suggest that the singularity behavior is due to the loss of rhythm in all

87 nduction of FRQ expression alone can trigger singularity behavior, indicating that FRQ is a state var

88 l stability, and temporal stability of phase singularities between the epicardial and the endocardial

89 intersections of these structures, magnetic singularities-Bloch points-occur.

90 the Muskat problem, we rule out the "splash singularity" blow-up scenario; in other words, we prove

91 We show that the location of singularities (bulk or boundary) may depend on the path

92 nd experimental study of the generation of a singularity by inertial focusing, in which no break-up o

93 tone demethylation can indeed produce robust singularity by separating two timescales: slow OR activa

94 These singularities, called dehydrons, are solvent-exposed int

95 describe how Art Winfree's ideas about phase singularities can be used to understand the response of

96 it remains a long-standing mystery how this singularity can be achieved despite intrinsic stochastic

97 We show that high-order van Hove singularity can be generally achieved by tuning the band

98 remains unclear at a quantitative level how singularity can be initiated in the first place.

99 Examples include singularities capable of damaging optical fibres and las

100 fluid systems, the formation of finite-time singularities cause spray and air-bubble entrainment, pr

101 During reentry, phase singularities clustered preferentially at sites of incre

102 compatibility in mind, and thus utilizes the Singularity container solution, which can be run on Linu

103 e this limitation by taking advantage of the Singularity container technology.

104 and line tool for Linux, based on Docker and Singularity containers; the core algorithms were written

105 We further argue that occurrence of these singularities correlates with the maximum superconductin

106 shifting the location of the embedded phase singularity (dark core) within the optical vortex beam.

107 more than one apical domain, resembling the singularity defect observed in yeast.

108 tected drivers than elsewhere, both in phase singularity density (2.3+/-2.1 versus 1.9+/-1.6; P=0.02)

109 om media the polarization orientation around singularities describe 1/2 or 3/2 Mobius strips.

110 s are irreversible, but not strongly so, the singularity disappears in the form found here and unlimi

111 Such singularities dramatically affect the low-energy electro

112 c system, the emergence of exceptional point singularities dramatically alters their overall response

113 The phase singularity drifted slowly across the tissue ( approxima

114 Singularities driven by surface tension have been studie

115 Phase singularities during pacing-induced reentry clustered sp

116 Burst Intensification by Singularity Emitting Radiation (BISER) is proposed.

117 xed type, free-boundary problems, and corner singularity, especially when an elliptic degenerate curv

118 a bubble is an example of the formation of a singularity, exhibiting a characteristic separation of l

119 hat are instead localized near a 2D van Hove singularity explains the anomalous transport observed in

120 vior when the Fermi level crosses a van Hove singularity for semiconducting species.

121 The proof takes advantage of the delayed singularity formation which occurs for solutions of quas

122 show that, besides the core, there are four singularities formed at the corners of the pattern.

123 We present a singularity-free self-interaction for a tube in the cont

124 monstrate a universal mapping of topological singularities from momentum to real space.

125 le Euler equations can develop a finite-time singularity from smooth, finite-energy initial data.

126 In this study C(r) and multifractal singularity function f(alpha) have been used to study va

127 The demonstrated polarization singularities generated from the geometric metasurfaces

128 , disordered magnet, and that the associated singularity grows to an anomalous divergence at T(C).

129 The polarisation of these singularities has a direct relation to the vortex core,

130 The reason for the existence of these singularities has remained elusive, suggesting that they

131 Splash singularities have been shown to hold for the free bound

132 lusters (most easily by invoking a dedicated Singularity image).

133 In particular we classify evolutionary singularities in a geometrical fashion.

134 that apoptotic cell extrusion is provoked by singularities in cell alignments in the form of comet-sh

135 ontrivial and consists of multiple band-edge singularities in close proximity to the Fermi level.

136 ures Dirac fermions, flat bands and van Hove singularities in its electronic structure.

137 of generating and controlling optical phase singularities in laser beams.

138 Topological defects are singularities in material fields that play a vital role

139 Singularities in multi-stream flows of emitting media ca

140 4), Singularities in state variable formulations are removed

141 We also observed phase singularities in the coherent exciton gas.

142 ion) and were often found at pinwheel center singularities in the cortical map of orientation prefere

143 Thus, pinwheel centres truly represent singularities in the cortical map.

144 traditional PCE that can effectively capture singularities in the DFBA model response due to the occu

145 Van Hove singularities in the electronic density of states of TMD

146 handedness imply the existence of degenerate singularities in the engineering mechanism.

147 robust to noise and the occurrence of phase singularities in the image domain, as we show on differe

148 ated Peierls chain, exhibiting van Hove type singularities in the one-dimensional density of states a

149 Exceptional points are branch point singularities in the parameter space of a system at whic

150 s disclinations arise as critical points and singularities in the phase field.

151 llations, spin-momentum locking and Van Hove singularities in the transition density of states.

152 ctionalization needed to affect the van Hove singularities in the UV/vis/NIR spectra.

153 gregate formation corresponds to finite time singularities in which the bacterial density diverges at

154 hat unlimited ultrasensitivity arises from a singularity in a novel "invariant" that summarises the a

155 to as the pI-can be defined as the point of singularity in a titration curve, corresponding to the s

156 The van Hove singularity in density of states generally exists in per

157 ntum electrodynamic interactions that have a singularity in media with hyperbolic dispersion.

158 ars to be tied to the presence of a van Hove singularity in the band structure.

159 wheel pattern with an orientation preference singularity in the center of the pattern.

160 h gain media increases dramatically due to a singularity in the density of optical states.

161 The singularity in the dipole-dipole coupling, referred to a

162 w that this behavior arises from a power-law singularity in the distribution of transition rates due

163 rops coalesce are intimately coupled to this singularity in the dynamics.

164 This edge state lies near the Van Hove singularity in the edge band structure and can be classi

165 A simultaneous dielectric singularity in the in plane permittivity, with respect t

166 We report a paramagnetic singularity in the magnetic susceptibility at low magnet

167 associated with the frequency of a van Hove singularity in the phonon density of states.

168 We introduce a new type of van Hove singularity in two dimensions, resulting from high-order

169 should prepare for the coming 'technological singularity' in sequencing, when this technology becomes

170 e completely uniform mixing, as predicted by singularity-induced diffusion, but only for oscillation

171 possible through a resonant mechanism called singularity-induced diffusion; this is thought to be the

172 , a unique family of MHC-like proteins whose singularity is a hydrophobic antigen-binding groove.

173 h theoretical calculations confirms that the singularity is a signature of competition between the or

174 eptor from a large family of genes, and this singularity is an essential feature in models of olfacto

175 ional formation of two buds, suggesting that singularity is enforced by rapid competition between Cdc

176 It is not yet understood whether the type of singularity is generally a consequence of the surface to

177 To assess whether singularity is linked to the specific Cdc42 feedback loo

178 eishmania, we find evidence that such origin singularity is maintained in the face of chromosome fusi

179 of the Fermi surface are destroyed, this log singularity is suppressed, raising the question of how p

180 The singularity is universal to the entire family, largely i

181 re typically effective at representing point singularities, it may be expected that these new systems

182 type of a dynamical system evolving toward a singularity, it has always been described in idealized t

183 Branch-point singularities known as exceptional points (EPs), which c

184 s reversal is mediated by a pair of magnetic singularities, known as Bloch points, and leads to the t

185 d popular rhetoric extolling this event as a singularity lacks rigorous evidential and statistical su

186 Although progress has been made in defining singularities like the RNA pseudoknot near this AUG, the

187 organized as a scroll wave rotating around a singularity line called the filament.

188 Finite-time singularities--local divergences in the amplitude or gra

189 A shift of up to 4 mm in the phase singularity location was observed in V(opt) maps when co

190 diffraction of light on a metasurface, with singularity marks then revealed by high-magnification in

191 ed VEPs may reinduce arrhythmias via a phase-singularity mechanism.

192 angle, the energy separation of the van Hove singularities must decrease with increasing charge densi

193 compelling evidence that the band-structure singularities near the Fermi level in the iron-based sup

194 Correlation effects from high-order van Hove singularity near Fermi level are also discussed.

195 The new solution has no singularities, no event horizons, and a global time.

196 Rewired cells violated singularity, occasionally making two buds.

197 A small (<128 mum) phase singularity occurred at the center of the spirals, about

198 to reveal the properties of the polarization singularities of C-points and L-lines, and the orbital a

199 Our results highlight the singularities of desert truffles with respect to other m

200 the layout of orientation preferences around singularities of different signs and the cardinal axes o

201 Disclinations are topological singularities of molecular arrangement in liquid crystal

202 Exceptional points are singularities of open systems, and among their many rema

203 The detailed structure of singularities of ordered field represents a fundamental

204 Singularities of passage times near the obstacles, dicta

205 width-at-half-maximum) and the generation of singularities of phase of reflected light.

206 putationally, and theoretically the route to singularities of soap films with different topologies, i

207 hen the energy interval between the van Hove singularities of the conduction and valance bands matche

208 track the field-features passing through the singularities of the distribution of the Poynting vector

209 mogeneous state of polarizations and optical singularities of the light beam.

210 patches were located on the pinwheel center singularities of the orientation map and consisted of ne

211 cal calculations to show that a hydrodynamic singularity of a given topological charge can nucleate a

212 d typical JVP pulses contours except for the singularity of an unknown "u" wave occurring after the c

213 p53 circuit and TRIM37 as an enforcer of the singularity of centrosome assembly.

214 not only a higher-order EP but also the cusp singularity of multiple exceptional arcs (EAs).

215 oding region of OR genes are involved in the singularity of OR gene expression.

216 and disruption of OR aggregates perturbs the singularity of OR transcription and disrupts the targeti

217 observe excitons associated with a van Hove singularity of rather unique nature.

218 phylogenomics that focuses attention on the singularity of species histories and away from the idios

219 Next we discuss singularity of stationary Yang-Mills connections and com

220 trajectories in the system and identify the singularity of the deflection angle at the photon sphere

221 composite materials, which have a broad-band singularity of the density of photonic states.

222 triggering correlated phenomena by placing a singularity of the density of states near the Fermi ener

223 phenomenon can be associated to a curvature singularity of the emergent metric.

224 Herschel-Bulkley exponent characterizing the singularity of the flow curve near the yield stress Sigm

225 Due to the singularity of the L(1)-norm, the L(1)-norm SVM has the

226 his result further highlights the remarkable singularity of the valence behavior in compressed YbCu5-

227 The singularity of VgrG-5 as a detected T6SS-5 substrate, ta

228 istency in the so-called anomaly zone, (iii) singularity on the likelihood surface, and (iv) deterior

229 The vorticity is observed to develop a ring-singularity on the solid boundary with a growth proporti

230 feedback, to achieve the observed extent of singularity (only 2% of neurons express more than one OR

231 in iso-orientation domains that converge at singularities or pinwheel centres.

232 sional (2D) dark hole resulting from a phase singularity or an amplitude depression in their optical

233 edback drives the shape toward a finite-time singularity or blow-up of apex curvature that is cut off

234 lly demonstrate a method using non-Hermitian singularities, or exceptional points, to enhance the Sag

235 and complexity (6.6+/-7.7 to 0.6+/-0.8 phase singularities; P<0.0001).

236 of Alu-mediated genetic disorders, represent singularities, places where behavior changes suddenly.

237 water retention curves (WRC) instead of the singularity point at air-entry suction in the pore-solid

238 eased the variance of AFCL, had no effect on singularity point density (0.048+/-0.011 to 0.042+/-0.01

239 before converting to sinus rhythm, decreased singularity point density from 0.070+/-0.007 to 0.039+/-

240 d partly to decreased dominant frequency and singularity point density, and prolongation of AFCL.

241 Reentrant activity was identified by singularity point recognition in raw signals and in sign

242 mapping that enables identification of phase singularity points (PSs), which flank individual wavelet

243 We used singularity points analysis to quantify the incidence of

244 tion patterns, phase generated nonrotational singularity points and false rotors.

245 e maps were visually analyzed to study phase singularity points and rotors.

246 Phase mapping computes singularity points and visually highlights rotors.

247 We identified WBs as singularity points in AP phase movies and sites of condu

248 measured as the number of epicardical phase singularity points, remained approximately constant duri

249 the initial concentration provide a non-zero singularity pole of inverse Laplace transform.

250 ls of plasmonic systems, which eliminate the singularities predicted by classical theories.

251 anomechanical slow-down and a zero-frequency singularity predicted by theorists.

252 ontinuous formation and destruction of phase singularities (PS) in cardiac fibrillation.

253 tional drivers (RDs) rotating around a phase singularity (PS).

254 unstable spiral waves rotating around phase singularities (PSs) in the heart, i.e., ventricular fibr

255 y a 3-fold reduction in the density of phase singularities (PSs) on the ventricular epicardial surfac

256 Phase singularities (PSs)-locations of ambiguous activation st

257 talytic trans-hydrogenation is by no means a singularity: rather, the underlying principle is also ma

258 We show that singularities reduce the length of intracortical neurona

259 reshock electrical activity and create phase singularities, regardless of the preshock phase distribu

260 We therefore conclude that singularity regulation by Cdc42 is conserved between yea

261 than later phases or that the appearance of singularity results from information loss through time.

262 a graph, turn over, and collapse in a splash singularity (self-intersecting curve in one point) in fi

263 is a complex electromagnetic field in which singularities serve as the marks on the scale.

264 ndstill in an atomic medium can cause a wave singularity similar to that associated with black holes.

265 ventricular fibrillation and show that Im at singularity sites was monophasic and positive with a sig

266 ecomes indistinguishable from a leading-edge singularity, so that excited states are no longer quasip

267 at an expansion of the Universe arose from a singularity some 15 billion years ago.

268 Such singularity structures are widely seen in natural and ar

269 equivalent mapping occurs for 3D topological singularities such as Dirac-Weyl synthetic monopoles, ac

270 the cortical surface, with the exception of singularities such as pinwheels and fractures.

271 ectivity and vectorisation in key regions of singularities, such as vortexes and saddle points, due t

272 based on the functionalization of the polar singularities that must form when a curved surface is co

273 trate that conventional devices possessing a singularity - that is, the requirement of an infinite re

274 TIP, in which the origin is an evolutionary singularity, the invasion boundaries and trade-off curve

275 t in the framework of so-called "finite-time singularities." The singular behavior associated with ac

276 grew model by applying bifurcation analysis, singularity theory, and numerical simulation.

277 Using singularity theory, classification diagrams of parameter

278 because the energy spent in radiation has a singularity there.

279 tially at the rim of the drop because of the singularity there.

280 here [Formula: see text] is the pinch-off or singularity time and [Formula: see text], in close agree

281 e key idea in nsPCE is to use a model of the singularity time to partition the parameter space into t

282 ts approximately 0.0035056 is the estimated singularity time.

283 with the fine-tuning of one of the band-edge singularities to within a fraction of the superconductin

284 ic tracking of propagation vectors and phase singularity trajectories revealed discordant activity ac

285 tallic material with two degenerate van Hove singularity transitions that can rehybridize to form int

286 Singularities underlie many optical phenomena.

287 spectral weight associated with the Van Hove singularity (VHS) to shift rapidly and nearly linearly t

288 between different layers to create van Hove singularities (vHSs) at adjustable binding energy.

289 The emergence of saddle-point Van Hove singularities (VHSs) in the density of states, accompani

290 We observe two distinct van Hove singularities (VHSs) in the local density of states arou

291 of rotors and spiral waves, including phase singularities, wavefront curvature, and dominant frequen

292 Under some assumptions on D and its singularities we give a description of the structure, th

293 Using our method of identifying phase singularities, we can elucidate the mechanisms for the f

294 ng a theoretical model based on hydrodynamic singularities, we capture quantitatively the instability

295 Points of phase singularity were created by the shock in the intersectio

296 nce of unique twist-angle-dependent van Hove singularities, which are directly revealed by spatially

297 f twisted bilayer graphene develops van Hove singularities whose energy depends on the twist angle be

298 geodesic is linked to the boundary, then the singularity will occur at the boundary, whereas if the t

299 if the two are unlinked initially, then the singularity will occur in the bulk.

300 be characterized by their relation to phase singularities within local nerve cell networks.