ライフサイエンスコーパス: symmetry

1 cture with a central trivalent O atom (C(3v) symmetry).

2 ructures and organelles that have rotational symmetry.

3 olids with arbitrary spin mixing and crystal symmetry.

4 stal and in solution with twofold rotational symmetry.

5 ssembly of heterometallic clusters with high symmetry.

6 e reversal symmetry, but preserves inversion symmetry.

7 rue potential of linkers with low electronic symmetry.

8 text] and [Formula: see text] quasi-doublet symmetry.

9 s) were used to estimate reproducibility and symmetry.

10 GRFs), stride kinematics, leg stiffness, and symmetry.

11 o sites in each unit cell related by a glide symmetry.

12 (DSMs) possess both parity and time reversal symmetry.

13 ss-beta structures, arranged with quasi-2(1) symmetry.

14 r that migrates unilaterally to break embryo symmetry.

15 ymmetry while maintaining a high crystalline symmetry.

16 vior without reliance on long-range periodic symmetry.

17 oth of which depart from strict superhelical symmetry.

18 conventional limitation imposed by intrinsic symmetry.

19 ontrast photonic crystals with cubic diamond symmetry.

20 gy for the synthesis of silver NCs with high symmetry.

21 ica have a structural order with tetrahedral symmetry.

22 its twisted molecular structure and reduced symmetry.

23 hiral charge transport as a result of broken symmetry.

24 ric anion positioning on the lowering of the symmetry.

25 al band insulators with broken time-reversal symmetry.

26 are resolved that display an unusual broken symmetry.

27 ivity that enforces the absence of geometric symmetries.

28 ion is protected by parity and time-reversal symmetries.

29 e and interaction of patterns with different symmetries.

30 jointly protected by onsite and crystalline symmetries.

31 namically coexisting patterns with different symmetries.

32 turn, near-field distributions with defined symmetries.

33 distinct orbital lattice modes of different symmetries.

34 s well as architectured, possess crystalline symmetries.

35 ttice geometry and breaking of time-reversal symmetry(14,15).

36 many such states are fully characterized by symmetries(2), interacting quantum systems can exhibit t

37 etry of the cochlear duct manifests tapering symmetry, a felicitous design principle that may have ev

38 Upon breaking the inversion symmetry, a spin splitting ('Rashba splitting') occurs i

39 gmented density functional-based approaches, symmetry adapted perturbation theory, and a supermolecul

40 ms of molecules with D(3h) symmetry and C(1) symmetry all exhibited anisotropic alignment with an edg

41 [pai2s + pai2s + sigma2s + sigma2s] reaction symmetry-allowed in the ground state, proceeding through

42 ent spectroscopy of TCNB(-) reveals selected symmetry-allowed vibronic transitions to the QBS, but th

43 ional topological states protected by onsite symmetries alone, and connectors are glues that complete

44 Density functional theory calculations and symmetry analysis of the large unit cell crystalline app

45 We perform a symmetry analysis that recalls that an individual Ising

46 bit coupling and magnetic field breaks these symmetries and can lead to a finite supercurrent even wh

47 t of superlattices with well-defined crystal symmetries and compositions.

48 dehydration (to -1.5 cm(-1)), owing to lower symmetry and a decrease in the coordination number of ir

49 ling modules and actin cytoskeleton to break symmetry and achieve a stable polarized state.

50 4 nm, suggesting the evidence of a hexagonal symmetry and beta' crystals.

51 by the simultaneous presence of crystalline symmetry and broken time-reversal symmetry, which is con

52 e brush-coated films of molecules with D(3h) symmetry and C(1) symmetry all exhibited anisotropic ali

53 The method does not rely on translational symmetry and can therefore also be applied to systems wh

54 ed in magnetic systems with broken inversion symmetry and chiral interactions, such as Dzyaloshinskii

55 citance external circuits to break inversion symmetry and create nontrivial topologically protected b

56 rived from the interplay between crystalline symmetry and dimensionality.

57 alter global properties such as the crystal symmetry and electronic structure, thereby enabling emer

58 an inherent ability of this system to break symmetry and evolve directional spindle motion.

59 By exploiting both mode symmetry and far-field properties, we reveal that the vo

60 ion as a 6-component twin due to pseudocubic symmetry and further confirmed by high-resolution synchr

61 ct constraints of a well-defined crystalline symmetry and large energy barriers separating different

62 In membrane proteins, symmetry and pseudosymmetry often have functional or evo

63 can be attributed to differences in both the symmetry and radial extension of the frontier molecular

64 with its strongly broken electronic flavour symmetry and revived Dirac-like electronic character, is

65 ss of the charge state distribution, and (4) symmetry and separation of the peak.

66 wise highly motile T cells that sustains the symmetry and stability of the T cell-APC synaptic contac

67 alcogenide multilayers with broken inversion symmetry and substantially enhanced nonlinear optical re

68 by the CoGd cap layer composition, the stack symmetry and the ferrimagnetic layer thickness.

69 ed by their characteristic spatial inversion symmetry and time inversion antisymmetry.

70 space, namely bands and Fermi surfaces, via symmetry and topology, classifying topological materials

71 Solvent-driven localization breaks the symmetry and traps the exciton in one branch.

72 is reported, given the large retentions and symmetry, and opportunity for the low lithiated phase of

73 tric species, which may have radial or polar symmetry, and the pennates, which include raphid and ara

74 well characterized, those that maintain the symmetry, and thereby the stability of the synapse, rema

75 c-axis leads to the breaking of C3 rotation symmetry, and thus, a small bandgap opens at the Dirac p

76 caused by lack of both inversion and mirror symmetry, appear to be qualitatively different from thos

77 In particular, limb angles and symmetry appeared to be the most relevant ones.

78 Unless these symmetries are broken, they can give rise to novel pheno

79 The symmetries are described in terms of order, repeated ele

80 g data required, particularly when molecular symmetries are included.

81 aving orientational and periodic translation symmetries are usually both short-range and long-range o

82 le modes of protein-protein interactions and symmetry are simultaneously achieved by selective, 'one-

83 nsional (3D) DNA meshframe with high spatial symmetry as a site-programmable scaffold, which can be p

84 first developed linkers with low electronic symmetry (as defined by large transition dipoles) and th

85 e that breaks both spatial and time-reversal symmetry, as well as the reflection parity of the static

86 hinge angle can diverge further from helical symmetry at the microtubule seam, generating a subpopula

87 These aggregates break symmetry autonomously to form elongated structures with

88 splayed outward movement with respect to the symmetry axis of the channel in the presence of the full

89 the N termini under the icosahedral fivefold symmetry axis, and forming a basket-like pentamer helix

90 the opening between the vocal folds and the symmetry axis, leading to a huge step forward towards cl

91 ting of four glutamate residues close to the symmetry axis.

92 standing the symmetry breaking from the high-symmetry bcc phase to the lower-symmetry Frank-Kasper ph

93 Third, the incompatible symmetry between the overgrowth phase and the substrate

94 are characterized by a strict time-reversal symmetry between the rates of energy coupled in and out

95 pect to the transmembrane region, indicating symmetry breakage across the channel.

96 t in TBG, the twisting and substrate induced symmetry breaking allow an out of plane orbital magnetiz

97 t/heavy-metal interfaces, owing to inversion symmetry breaking and spin-orbit coupling by a heavy met

98 We demonstrate the persistence of inversion symmetry breaking and spontaneous, switchable polarizati

99 oupling, interband pairing and time reversal symmetry breaking are also present.

100 Studies of both the concept of chiral symmetry breaking as well as the subsequent chiral ampli

101 sential to control skyrmion properties, with symmetry breaking at interfaces offering the greatest fl

102 Electronic symmetry breaking by charge disproportionation results i

103 show that mitochondria also contribute to symmetry breaking by producing hydrogen peroxide at the

104 We show that local, pattern-induced symmetry breaking can account for dynamically coexisting

105 action (DMI), originating from the inversion symmetry breaking combined with the strong spin-orbit co

106 35+/-10 meV, and identify the main inversion symmetry breaking direction perpendicular to the MQW pla

107 ts are usually preceded by and influenced by symmetry breaking events and cell polarization.

108 ning furnishes a basis for understanding the symmetry breaking from the high-symmetry bcc phase to th

109 e regulatory networks arise from a fibration symmetry breaking in the network structure.

110 2)Se(3) and Cu(x)Bi(2)Se(3) reveal that this symmetry breaking occurs at [Formula: see text] above [F

111 sent crystallographic evidence as to how the symmetry breaking occurs on a crystallographic and, ther

112 observed morphological changes are caused by symmetry breaking of the irreducible building blocks, wi

113 moons, the ice shell can undergo hemispheric symmetry breaking only if the mean shell thickness is ar

114 he passive parity-time ([Formula: see text]) symmetry breaking transition in the underlying non-Hermi

115 emists' perspective of autocatalysis, chiral symmetry breaking, absolute asymmetric synthesis and its

116 polymorphic aggregates, aggregation-induced symmetry breaking, and cluster excitons are only identif

117 These fundamental processes of symmetry breaking, axiation, patterning, and morphogenes

118 erization corresponding to chemically-driven symmetry breaking, is observed.

119 a new principle of spontaneous translational symmetry breaking, providing a general route towards des

120 orbit interaction, and optical non-Hermitian symmetry breaking, we demonstrate an OAM-tunable vortex

121 substantiating this picture of a cascade of symmetry breaking.

122 ometrically frustrated lattice and inversion symmetry breaking.

123 l communication across the cell required for symmetry breaking.

124 e of the simplest paradigms in which angular symmetry-breaking assemblies of mechanical sensors are s

125 This observation offers insights into charge-symmetry-breaking forces acting in atomic nuclei.

126 actions with lead bromide-based layers cause symmetry-breaking helical distortions in the inorganic l

127 ment interaction, nematic bands show a local symmetry-breaking instability within their high-density

128 oupling generating interfacial DMI at mirror symmetry-breaking interfaces.

129 e type-II multiferroics induced by inversion-symmetry-breaking of spin order.

130 low-temperature orders and the parent flavor symmetry-breaking orders.

131 xhibit the rare and counterintuitive inverse-symmetry-breaking phenomenon(3).

132 chemical symmetry can be tuned by creating a symmetry-breaking rotational bulk polarisation in the el

133 nteractions, yet crucial for the spontaneous symmetry-breaking, affording the remarkably efficient st

134 mental technique can be generalized to study symmetry-broken states and low energy magneto-optical pr

135 The magnetic order breaks time reversal symmetry, but preserves inversion symmetry.

136 hanism that actively promotes T-cell synapse symmetry by generating cytoskeletal tension in the plane

137 t this finding to synthesise a family of low-symmetry cages containing heteroatoms, illustrating that

138 e stands out as unable to assemble into high-symmetry cages-and the same aldehyde generates low-symme

139 f simulated data, in which we show how scale symmetry can be identified and how the associated conser

140 Here, we show how effective chemical symmetry can be tuned by creating a symmetry-breaking ro

141 s observed distance restraints and/or cyclic symmetry (Cn symmetry) found in most homo-oligomeric tra

142 sing this fabrication workflow produced good symmetry, color match, and prosthesis fit.

143 earching the construction space for all such symmetry-combination materials (SCMs).

144 However, symmetry conditions generally restrict spin polarization

145 rmation, and reveal an inter-ring nucleotide symmetry consistent with the absence of negative coopera

146 as well as breaking of fourfold spin-valley symmetry, consistent with spin-orbit coupling induced in

147 ing of inelastically scattered light through symmetry control in atomically thin chromium triiodide (

148 can also induce strain but providing dynamic symmetry control is restricted to specific materials und

149 ng a generalized linear model (with compound symmetry correlation structure), accounting for the corr

150 Even an antigen with dihedral symmetry could be displayed.

151 Symmetries crucially underlie the classification of topo

152 nrose tiling retains the M(54) kernel's high symmetry (D(5h)).

153 Broken-symmetry density functional theory (BS-DFT) calculations

154 By varying ligand symmetry, denticity, and orientation, we explore how fiv

155 However, available symmetry detection methods have not been tested systemat

156 he solid solutions (y = 1 to 7) retain cubic symmetry down to 1.5 K.

157 using three independent methods: analysis of symmetry eigenvalues, numerical calculations of the nest

158 Here we demonstrate that one of the two symmetry elements of olanzapine crystals, an inversion c

159 A mirror symmetry emerges from this isobaric-spin formalism: nucl

160 Manipulating symmetry environments of metal ions to control functiona

161 hether the constituent layers have inversion symmetry, exhibit a mechanical response to out-of-plane

162 chemoreceptors organize into a hexagonal (P6 symmetry) extended array.

163 ural network assigned importance to the same symmetry features that a crystallographer would use for

164 Thus, symmetry fibrations describe how complex networks are bu

165 nic generation (SHG) study revealed Kleinman symmetry-forbidden nonlinear optical properties.

166 stance restraints and/or cyclic symmetry (Cn symmetry) found in most homo-oligomeric transmembrane pr

167 rom the high-symmetry bcc phase to the lower-symmetry Frank-Kasper phases, wherein the reconfiguratio

168 and autonomous identification of the crystal symmetry from EBSD patterns.

169 ations-that can be used to distinguish scale symmetry from scale freeness in empirical data.

170 of bosonic TCSs protected by several onsite symmetry groups and each of the 17 wallpaper groups in t

171 Molecular knots of high symmetry have previously been synthesized by using non-c

172 blocks with cyclohexanediamine to access low-symmetry imine cages.

173 ilters, the distance-restraints (DR) and the Symmetry-Imposed Packing (SIP) filters.

174 nchmark set of both quaternary- and internal-symmetries in membrane protein structures.

175 ucture with unexpected three-fold rotational symmetry in a single two-dimensional layer of crystallin

176 al hollow crystals with broken translational symmetry in crystalline molecular bottlebrush (mBB) poly

177 ensity, manifested as a spontaneously broken symmetry in distinct domains of opposite polar orientati

178 cted nature of topology, dimensionality, and symmetry in electronic systems.

179 However, whether this symmetry in host responses between PAMPs and DAMPs exten

180 Patients showed loss of symmetry in measures of hand motor resting-state connect

181 of the main flight muscles while maintaining symmetry in most major aspects of wing motion, including

182 The absence of inversion symmetry in non-centrosymmetric materials has a fundamen

183 ological defects are a consequence of broken symmetry in ordered systems and are important for unders

184 otein family are known to regulate bilateral symmetry in single flowers.

185 reversible method of manipulating effective symmetry in solids.

186 s 40 mm or less from the IHM region, loss of symmetry in strength of resting-state connectivity was c

187 The removal of time-reversal symmetry in such systems further extends the variety of

188 capsid environments while maintaining strict symmetry in the rest of the structure.

189 e effects counterintuitively stabilize polar symmetry in the ultrathin regime.

190 iously unknown topological phases, including symmetry-indicated magnetic semimetals, three-dimensiona

191 bles like circular dichroism, by introducing symmetry indicators in amorphous systems.

192 on conduction in MOF/IL blends, whereas pore symmetry is a less stringent condition.

193 ions of Onsager's theorem when time reversal symmetry is broken at zero applied field.

194 When this symmetry is broken in anisotropic materials a wide array

195 hies and embryonic lethality, yet how tissue symmetry is broken to specify trabecular cardiomyocytes

196 etal-halide perovskites with defined crystal symmetry is desired to control the spin-splitting in the

197 Such a broken symmetry is found to strongly enhance the vdW interlayer

198 magnetic materials only when the crystalline symmetry is reduced.

199 order that can be described with the Fm - 3m symmetry is reliably detected, (2) the coherence length

200 in bilayer and bulk hBN, where the center of symmetry is restored.

201 Bilateral symmetry is the predominant body plan in the animal king

202 of TCNB(-) (A(u) symmetry) to the QBS (A(g) symmetry) is triply forbidden by the electric and magnet

203 nt requirements of anti-commuting reflection symmetries, it is challenging to achieve higher-order qu

204 ifractal spectrums with different degrees of symmetry, locations, support and shapes.

205 In theory, nickel ions in octahedral symmetry meet all the criteria for optical readout of sp

206 complex of the Dot/Icm T4SS that includes a symmetry mismatch between distinct structural features o

207 ts of both the OMC and the PR and bridge the symmetry mismatch between these regions.

208 However, symmetry mismatch can prohibit vaccine nanoassembly.

209 structure of portal morphs to compensate for symmetry-mismatch, forming similar interactions in diffe

210 ClpX and ClpP rings, it remains unknown how symmetry mismatched ClpX and ClpP work in tandem for pro

211 nar, heptameric ClpP surface with the empty, symmetry-mismatched IGL pocket maintained at the seam.

212 ractions between portal and capsid, across a symmetry-mismatched interface.

213 However, the symmetry modulation at interfaces and the resultant effe

214 tructures(1,2), which in a few cases exhibit symmetries not present in the native material(3-5).

215 The symmetries of a crystal are notoriously uncorrelated to

216 Here we show how dualities can enhance the symmetries of a dynamical matrix (or Hamiltonian), enabl

217 Our theory predicts a set of symmetries of barcode covariance that serves as a consis

218 Here we first define and compute the symmetries of multilayer networks, and then study the em

219 The observed symmetries of the anomalous Josephson effect in the vect

220 g the orientational and periodic translation symmetries of the chain lattice.

221 ates the mismatch between the 3- and 10-fold symmetries of the F(1) and F(o) motors.

222 topological insulators are protected by the symmetries of the nontrivial bulk electronic states.

223 ons spontaneously break the time-translation symmetry of a driven oscillator.

224 By considering the symmetry of contact map, we reduced the number of matric

225 ctional theory (DFT) the structure and local symmetry of each prototypical silicene phase on Ag(111)

226 nterobserver reproducibility and interocular symmetry of GCC and evaluated candidate determinants.

227 Accordingly, the symmetry of ordered states is a dynamical property in ac

228 Because of the symmetry of period-tripling, the zero-amplitude state re

229 The symmetry of such flow is then spontaneously broken throu

230 pectroscopy analysis, determines the overall symmetry of the bambusuril structure.

231 strain in the Te film that breaks the screw symmetry of the crystal.

232 the TSC1 coiled-coil backbone, breaking the symmetry of the dimer.

233 er efficiency due to improved uniformity and symmetry of the induced index modification.

234 lly, videoendoscopy is applied to assess the symmetry of the oscillation and evaluated subjectively.

235 s in the assembly are closely related to the symmetry of the particle, and a "quadruple-gear-like" in

236 to become non-symmetric despite the complete symmetry of the problem.

237 scribed as a loss of the [Formula: see text] symmetry of the solutions corresponding to stationary lo

238 Cut-off points for interocular symmetry of the superior and inferior quadrants and tota

239 tch pits are formed, which reflect the local symmetry of the surface: square pits on (100) facets, tr

240 able differences in the extent, location and symmetry of wing surface loss among species, with smalle

241 Jellyfish, with their tetraradial symmetry, offer a novel paradigm for addressing patterni

242 chiral field, which breaks the time-reversal symmetry on a nanometre spatial scale and a 20-femtoseco

243 ation for systems with and without inversion symmetry on an equal footing.

244 The influence of symmetry on the electronic properties of TATBPs was stud

245 materials, including imprints of the crystal symmetry on the large-scale flow pattern.

246 electron-intensity distribution and a chosen symmetry operation applied to that distribution.

247 Here, we report an alternative symmetry (P2) of the chemotaxis apparatus that emerges f

248 ystems with only a few variants of the lower symmetry phase.

249 Striking examples are broken symmetry, phase transitions and collective excitations(2

250 servation is SO(3) invariant in the relevant symmetry plane in real space per the SU(2) invariance of

251 Parity-time symmetry plays an essential role for the formation of Di

252 Methods of generating lower symmetry pores are thus required to maximise the binding

253 Conservation laws are deeply related to any symmetry present in a physical system(1,2).

254 ower-dimensional topological phases and host symmetry protected zero-dimensional corner states.

255 ls are topological semimetal candidates with symmetry-protected Dirac crossings near the Fermi level

256 rystal, Ta(21)Te(13), reveal the presence of symmetry-protected nodal crossings in the quasicrystalli

257 pathways primarily dependent on nanoparticle symmetry rather than size.

258 d, coupling patterns are not resolved, or if symmetry reasons preclude interpretation.

259 Strategies rooted in hidden symmetry recognition, C-H functionalization, and radical

260 ul subassembly across each interface between symmetry-related VP monomers; and at the capsid-scale, w

261 In the present study, by symmetry relaxation and subparticle reconstruction, we h

262 ortunately, materials must satisfy stringent symmetry requirements to be classified as piezoelectric.

263 nductor that lacks both mirror and inversion symmetries, resulting in complex band structures with We

264 ine pai system since breaking of the orbital symmetry results in allowed transitions (e = 2800 M(-1)c

265 ral networks requires materials with tunable symmetry, retention, and speed at low power consumption.

266 MainOutcomeMeasures: Prosthesis symmetry, skin tone match, comfort of wear, and appearan

267 ry cages-and the same aldehyde generates low-symmetry socially self-sorted cages when combined with a

268 or for this simple model, featuring a broken-symmetry striped phase that is disrupted at both high an

269 rally exhibit a high degree of regularity or symmetry, structural defects might be expected because o

270 which lack any type of (geometric or hidden) symmetry, such as complex networks, buildings, or vessel

271 Dirac fermions and broken electronic flavor symmetry; superconductivity and correlated insulators em

272 Growing single-crystal hBN on such high-symmetry surface planes as Cu (111)(5,8) is widely belie

273 inspiration from quantum (e.g., parity-time) symmetries that are eliciting growing attention in the e

274 cribed as a bilateral disease with inter-eye symmetry that presents on short-wavelength fundus autofl

275 The key ingredients for topology are certain symmetries, the inert pair effect of the outer electrons

276 By breaking spatial inversion symmetry, the stator defines the unique sense of rotatio

277 ted cylinders rotate along a central axis of symmetry to form circular hoops.

278 At the onset of cell locomotion, cells break symmetry to form well-defined cell fronts and rears.

279 ition from the ground state of TCNB(-) (A(u) symmetry) to the QBS (A(g) symmetry) is triply forbidden

280 3 conjugation enables nanodisplay of diverse symmetries towards generation of potent vaccines.

281 ackscattering is suppressed by time-reversal symmetry (TRS).

282 Their symmetry under permutation of orbitals allows us to anal

283 nterobserver reproducibility and interocular symmetry using optical coherence tomography (OCT)-based

284 ifference of SE and superior and total mRNFL symmetry values (p = 0.047 and p = 0.040, respectively).

285 etwork and of the violation of time-reversal symmetry via a magnetic field; thus establishing CPA bey

286 Cut-off points for symmetry were defined as the 95th percentile of the abso

287 In study 3, measured facial averageness and symmetry were weakly negatively related to 8-OHdG levels

288 namic theory for agents with mixed alignment symmetries, which captures the experimentally observed p

289 xploit wavefunctions relying on crystal band symmetries, which tunneling interactions are inherently

290 rystalline symmetry and broken time-reversal symmetry, which is confirmed using three independent met

291 ngular spin structure creates a low magnetic symmetry while maintaining a high crystalline symmetry.

292 ing layers with icosahedral and dodecahedral symmetries, while open network liquids like silica have

293 controls interparticle distance and crystal symmetry, while the magnetic field leads to anisotropic

294 The energy required for breaking symmetry with chiral bias is compared for this near-equi

295 .7 angstrom) structure containing R3 crystal symmetry, with a slight subsequent improvement (2.6 angs

296 nce Tomography (OCT) and to study topography symmetry within eyes and between eye pairs.

297 viations in the polyhedral coordination/site-symmetry within the 4-fold coordinated Li1/24d sites (ra

298 icroscopy (STEM) that derives from the local symmetry within the specimen.

299 interesting target guest molecules have low symmetry, yet most methods for synthesising hosts result

300 Reprocessing the image data using two-fold symmetry yielded a cryo-EM map in which both DNA ends ap