ライフサイエンスコーパス: symmetry

1 i (highly chiral) to L. mexicana (near-axial symmetry).

2 moving patterns with and without positional symmetry.

3 ch is characteristic of an icosahedral T = 1 symmetry.

4 c distortions resulting in pseudocubic local symmetry.

5 e-reversal symmetry (TRS) or space-inversion symmetry.

6 the locomotor pattern, but not with temporal symmetry.

7 obacterium modesticaldum exhibits perfect C2 symmetry.

8 llel spins in a singlet state with an s-wave symmetry.

9 ge triangles and small triangles with 6-fold symmetry.

10 gyre 1.5 helical turns from the dyad axis of symmetry.

11 ks time-reversal while preserving SU(2) spin symmetry.

12 P) of HH pulses can be controlled by crystal symmetry.

13 s caused by incompatible in-plane structural symmetry.

14 ve used nonlinearities to break transmission symmetry.

15 s, we develop a strategy to control assembly symmetry.

16 helices co-linear with the five-fold axis of symmetry.

17 s, Au279S84 structure has a chiral pseudo-D3 symmetry.

18 tensite phase with preserved austenite phase symmetry.

19 sic ability of the embryo to initially break symmetry.

20 the minimal number required by time-reversal symmetry.

21 s attributed to the monolayer's mirror-plane symmetry.

22 dimers losing their local 2-fold rotational symmetry.

23 ionality, topology, Coulomb interactions and symmetry.

24 m entanglement and the absence of any broken symmetry.

25 that the TE6 enzyme forms a hexamer with D3 symmetry.

26 mmetrical motion, with or without positional symmetry.

27 topological insulator without time-reversal symmetry.

28 ic materials in order to break time-reversal symmetry.

29 genides breaking the out-of-plane structural symmetry.

30 ) regulates the maintenance of somitogenesis symmetry.

31 /G9a, as a RA coactivator controlling somite symmetry.

32 ension flows that spontaneously break mirror symmetry.

33 T d-MoTe2 is determined to have 2-gap s-wave symmetry.

34 gnetic duality symmetry but broken inversion symmetry.

35 itching in prototypical BaTiO3 of tetragonal symmetry.

36 show that different phases may have the same symmetry.

37 e one of the best illustrations of embryonic symmetry.

38 iting polarization along with spatial-parity symmetry.

39 assembly into complexes that possess cyclic symmetry.

40 nt stacking motif and adopt a higher crystal symmetry.

41 of subsystems of a large system with general symmetries.

42 mbined parity (reflection) and time-reversal symmetries.

43 hat breaks both rotational and translational symmetries.

44 ructures with more than 30 different lattice symmetries.

45 due to high lattice symmetry; however, lower-symmetry 2D materials such as phosphorene and other elem

46 artificially break the structural inversion symmetry (5-8) .

47 sible because of the sensitivity to delicate symmetries: a positive Kerr effect indicates that time r

48 n the arene scaffold, here generalized to Cn symmetry, accurately describes the relationship between

49 changes in the needle complex to provide the symmetry adaptation required for the assembly of the ent

50 a strategy of entropy stabilization of high-symmetry alloys.

51 ontinuous scale symmetry into discrete scale symmetry also appears for a charged and massless Dirac f

52 Through a detailed symmetry analysis and density functional theory calculat

53 , we present band structure calculations and symmetry analysis for 6 previously synthesized organic m

54 tering (SAXS) analyses indicate that lattice symmetries and dimensions of ferritin-MOFs can be dictat

55 ous crystal phases with distinct structures, symmetries and physical properties.

56 ate Dirac nodes protected by the crystalline symmetry and 4-fold degenerate Dirac nodes protected by

57 ) require spatial control over time-reversal symmetry and chemical potential.

58 g lateral electronic modulation of hexagonal symmetry and discreet subbands.

59 New approaches on relaxing symmetry and exploring structure dynamics and heterogene

60 s specialised mechanisms for encoding mirror-symmetry and for detecting symmetric motion-directions f

61 k photovoltaic effects should lack inversion symmetry and have an optical gap matching the energies o

62 rstanding both the breaking of embryonic L-R symmetry and how the Nodal-Pitx2 pathway controls latera

63 ose synthase complex (CSC) exhibits a 6-fold symmetry and is known as a "rosette." Each CSC is believ

64 ecular machines consume free energy to break symmetry and make directed progress.

65 actility is sufficiently strong, cells break symmetry and move steadily along either straight or circ

66 uring hypoglycemia as demonstrated by T-wave symmetry and principal component analysis ratio compared

67 e these two structures have the same helical symmetry and repeat distance and nearly identical folds

68 The interplay between symmetry and topology leads to a rich variety of electro

69 classified into type-I that respect Lorentz symmetry and type-II that do not.

70 th magnetization (which breaks time-reversal symmetry) and chemical potential in ferromagnetic thin f

71 charge states, with nearly perfect Ih point symmetry, and can be viewed as an Sb@Pd12 icosahedron ce

72 organize and assemble, how the embryo breaks symmetry, and what controls timing and size in developme

73 with the prolonged adaptation in step length symmetry ( approximately 128 strides) as well as EMG mag

74 icates that time reversal and certain mirror symmetries are broken in the ordered phase.

75 These higher symmetries are obtained by executing additional geometri

76 em, we find that morphological and molecular symmetries are simultaneously broken by an emergent proc

77 When molecular motion and crystallographic symmetry are both accounted for, the J((11)B,(11)B) coup

78 Local structure and symmetry are keys to understanding how a material is for

79 parisons of the two, as tests of fundamental symmetries, are driving a vibrant programme of research.

80 ng two flexible molecules with C3v molecular symmetry as building units, a novel imine-linked COF, na

81 behavior of the TO phonon modes of B1 and B2 symmetries at low frequencies at different temperatures.

82 n diameter form around icosahedral threefold symmetry axes.

83 uch as depressions at the icosahedral 2-fold symmetry axis and surrounding the 5-fold symmetry axis,

84 carbonyl O atom positioned on the three-fold symmetry axis of the NH3(+) group (angle C(epsilon)-N(ze

85 other by a local twofold noncrystallographic symmetry axis, a conformation clearly distinct from that

86 try axis, protrusions surrounding the 3-fold symmetry axis, and a channel at the 5-fold symmetry axis

87 old symmetry axis and surrounding the 5-fold symmetry axis, protrusions surrounding the 3-fold symmet

88 ding domains are misaligned along a two-fold symmetry axis, revealing a possible mechanism by which g

89 d symmetry axis, and a channel at the 5-fold symmetry axis.

90 lop a systematic approach to expose all such symmetry-based indicators of band topology in all the 23

91 tinguishable HS-LS phase with monoclinic P21 symmetry before returning into the LS phase.

92 Rate of structural disease progression, symmetry between eyes, and test-retest variability were

93 al-organic framework (MOF) built with a high-symmetry bicyclo[2.2.2]octane dicarboxylate linker in a

94 e how active scale selection controls mirror-symmetry breaking and the emergence of a 3D inverse casc

95 at facilitate the bandwidth-scaled inversion-symmetry breaking are common to numerous materials.

96 e demonstrate nonreciprocity and spontaneous symmetry breaking between counter-propagating light in d

97 ticity, geometrical frustration, and achiral symmetry breaking can be used to fold colloidal membrane

98 ground state and an ordered HS-LS phase with symmetry breaking from monoclinic P21/n into orthorhombi

99 The in-plane symmetry breaking has little apparent connection to the

100 ean-field models, showing the possibility of symmetry breaking in the latter.

101 Spontaneous symmetry breaking is a concept of fundamental importance

102 Spontaneous symmetry breaking is a fundamental concept in many areas

103 An incommensurate phase and symmetry breaking is found within these domains resultin

104 netic phase which is preceded by local point symmetry breaking is stabilized at low temperatures, as

105 nt here unambiguous evidence for macroscopic symmetry breaking leading to robust Bain distortion in t

106 pinners, emerging as a result of spontaneous symmetry breaking of clock/counterclockwise rotation of

107 Specifically, we demonstrate that the symmetry breaking of network connectivity constitutes a

108 sponsible for diversity and spatial-temporal symmetry breaking of pattern formation.

109 The resulting roadmap to symmetry breaking paves the way for deterministic engine

110 ond cross-coupling reactions based on remote symmetry breaking processes in diarylmethine substrates.

111 p (PG) state and its related intra-unit-cell symmetry breaking remain the focus in the research of cu

112 ions among them can be explained by Landau's symmetry breaking theory.

113 esults presented suggest employing dynamical symmetry breaking to engineer quantum spin liquids and a

114 ealizing a much larger coupling of inversion-symmetry breaking to itinerant surface electrons than is

115 zeroth LL mode observed in the time reversal symmetry breaking type II Weyl semimetal YbMnBi2.

116 Furthermore, we observe a statistical symmetry breaking upon varying the cavity loss.

117 Pb(BrxI1-x)3 alloys, which we associate with symmetry breaking within the perovskite unit cell.

118 equence of spin-orbit coupling and inversion symmetry breaking, leading to a valley analog of the Zee

119 -that is, a kinetic-energy-coupled inversion-symmetry breaking, the energy scale of which is a substa

120 lows are not equivalent because of inversion symmetry breaking.

121 mouse embryos is responsible for left-right symmetry breaking.

122 rder associated with spontaneous point-group symmetry breaking.

123 The idea of using local symmetry-breaking cues to improve the realism of organoi

124 omain on one side of the cell in response to symmetry-breaking cues.

125 g is deterministic only in the presence of a symmetry-breaking in-plane field.

126 at intraspecific competitions or alternative symmetry-breaking mechanisms can promote biodiversity to

127 The dominant role of symmetry-breaking nO((pi))-sigma*CC interactions between

128 We identify the parity-time symmetry-breaking phase transition occurring in spin-tra

129 r realization in spontaneously time-reversal-symmetry-breaking phases of strongly correlated material

130 r the realization of versatile time-reversal symmetry-breaking physics.

131 Structural symmetry-breaking plays a crucial role in determining th

132 easts and demonstrate that models describing symmetry-breaking polarization can be classified into si

133 excitations in weakly correlated, inversion-symmetry-breaking semimetals.

134 ikely to be relevant for the G-protein-based symmetry-breaking systems of higher eukaryotes.

135 large variety of systems undergoing the U(1) symmetry-breaking transition.

136 ssue identity markers are impaired from the "symmetry-breaking" periclinal cell divisions during the

137 predictions and discoveries of novel Landau-symmetry-broken phases in correlated electron systems, t

138 Moreover, we show that symmetry-broken superlattices can sustain switchable nan

139 otonic crystals with electromagnetic duality symmetry but broken inversion symmetry.

140 odes, owing to the breaking of time-reversal symmetry by Earth's rotation.

141 symmetric waveforms indicating that waveform symmetry can be used to tune the relative sizes of rever

142 odified, the means by which flower shape and symmetry can change, and the ways in which floral organ

143 are most profound if the underlying lattice symmetry changes.

144 The particle-hole symmetry characteristic to the BDI symmetry class stems

145 icle-hole symmetry characteristic to the BDI symmetry class stems from the distinct behaviour of the

146 .35, SE=0.03; symmetry factor=0.39, SE=0.03; symmetry class=0.38, SE=0.10).

147 l processes that result in formation of high-symmetry clusterfullerenes, which attract interest for u

148 ign approaches, a complete list of allowable symmetry combinations that can be used for construction

149 at the proposed arrangements are in size and symmetry compatible with experimentally observed Abeta a

150 plifiers in the microring resonators, the PT-symmetry condition can be achieved by a precise manipula

151 s has useful applications in spintronics but symmetry constraints can limit the control over spin pol

152 posite materials with unique properties, but symmetry control of assembled structures remains a chall

153 trons pairing with a p-wave or chiral d-wave symmetry, depending on the position of the Fermi energy

154 We found that symmetry detection thresholds were (a) significantly hig

155 agreement with the ones calculated by broken symmetry DFT calculations.

156 maxima located away from any particular high-symmetry direction.

157 l insulator Bi2Te3 is canted out of the high-symmetry directions of the surface unit cell resulting i

158 neral switching of polyhedral distortions at symmetry-disallowed transitions in perovskites that may

159 ements) reveal electron density peaks at two symmetry-distinct interstitial sites.

160 charge-ordered phases, broken translational symmetry emerges from couplings between charge, spin, la

161 -based phenotypes across analyses: symmetry (symmetry, evening up, checking obsessions; ordering, arr

162 Although enforcing symmetry facilitates reaching near-atomic resolution wit

163 ificant (disinhibition factor=0.35, SE=0.03; symmetry factor=0.39, SE=0.03; symmetry class=0.38, SE=0

164 films exhibited a single diamond topology of symmetry Fd3m (Q227) which was verified by Small angle X

165 domains form a central hub (twofold axis of symmetry) flanked by two Cas1 lobes and two Cas3 lobes.

166 es of particle-hole pairs generated by SU(2) symmetry fluctuations.

167 antum system is broken into a discrete scale symmetry for a critical value of a control parameter.

168 The second strategy exploits statistical symmetry for a further reduction of [Formula: see text]

169 tion of the LCP structure, which was of Pn3m symmetry for all the formulations studied.

170 We observe that homomers from different symmetry groups are significantly enriched in distinct f

171 plified NMR Detector (WAND) with cylindrical symmetry has been fabricated and non-surgically inserted

172 Because PT-symmetry has been thought of as fragile, experimental re

173 n (Env) mimetics displaying ordered trimeric symmetry has ushered in a new era in HIV-1 vaccination.

174 2D materials, which is characterized by low symmetry having 1D metallic chains within the planes and

175 hibit isotropic behavior due to high lattice symmetry; however, lower-symmetry 2D materials such as p

176 s on mass-independent isotope effects due to symmetry, ignoring smaller mass-dependent effects.

177 perate by breaking time-reversal and spatial symmetries in the direction of transport through applica

178 ructures of bilayer MoS2 and produce two new symmetries in their bandgaps and offset crystal momentum

179 e fluids break both parity and time-reversal symmetries in their non-equilibrium steady states.

180 Owing to the inversion symmetry in bilayers, the photoluminescence helicity sho

181 rid period, grid orientation, and rotational symmetry in close association with changes in environmen

182 Shape symmetry in dual-mode planar electromagnetic resonators

183 The first obvious sign of bilateral symmetry in mammalian and avian embryos is the appearanc

184 ngle longitudinal mode operation based on PT symmetry in millimeter long edge emitting lasers having

185 cted ions with a greater or lesser degree of symmetry in order to isolate spectral signals of interes

186 s into proper alignment and to improve nasal symmetry in patients with cleft lip and palate.

187 nd graphite due to the absence of reflection symmetry in puckered phosphorene.

188 ring and enhancing the breaking of inversion symmetry in solids-that is, allowing electrons to differ

189 egional coregulation of opioid genes: broken symmetry in spinal circuits.

190 that A-site cation ordering lifts inversion symmetry in the superlattice and produces a polar compou

191 tals in space, the breaking of translational symmetry in time and the emergence of a 'time crystal' w

192 was due to the lack of broken translational symmetry in two dimensions-doubting the existence of 2D

193 f the same sequence were observed, either as symmetry-independent molecules within the same unit cell

194 CI, 113-138]; P=0.029) and more symmetrical (symmetry index, 0.84 [95% CI, 0.8-0.89] versus 0.77 [95%

195 Broken continuous scale symmetry into discrete scale symmetry also appears for a

196 suggest a triplet ((3)A2) ground state in D3 symmetry involving two degenerate Sc-N2-Sc bonding orbit

197 Bilateral symmetry is a striking feature of the vertebrate body pl

198 Our study reveals that tuning magnetic symmetry is an effective route to enhance the magnetoele

199 Symmetry is broken by motile cilia-generated asymmetric

200 When the time-reversal symmetry is broken, it may introduce a topologically non

201 The observations suggest that electronic symmetry is of greater importance for triplet state delo

202 a range of asymmetries to determine whether symmetry is the energetically optimal strategy for walki

203 mbly process and determines the superlattice symmetry, leading to the tetragonal superlattice that be

204 s, which pack into a previously unknown, low-symmetry lyotropic liquid crystalline Frank-Kasper sigma

205 llerenes, the breaking of the cage spherical symmetry makes super atomic molecular orbital (SAMO) sta

206 By describing how energy- and symmetry-matched impurity orbitals, at low concentration

207 using the Interpercentile Range Adjusted for Symmetry method and statements that passed consensus for

208 Lattice mismatch for 3 uc of BTO and symmetry mismatch for 10 uc of BTO, both associated with

209 substrates in order to elucidate the role of symmetry mismatch.

210 riately decomposing the input and exploiting symmetries of the Fourier transform we are able to deter

211 ique POMT-dependent mechanism that maintains symmetry of a developing system affected by chiral force

212 The symmetry of a homodimer is broken in heterodimeric react

213 alized in graphene.When the continuous scale symmetry of a quantum system is broken, anomalies occur

214 f anomalies occurs when the continuous scale symmetry of a scale-free quantum system is broken into a

215 shed non-trivial interconnection between the symmetry of bi-directional light propagation properties

216 matic feature that arises from the head-tail symmetry of cell-to-cell interaction).

217 4(+) within its solvent cage and then to the symmetry of hydrogen bonds.

218 The Td point group symmetry of rare earth (RE(3+)) metal clusters RE4(mu3-O

219 We quantified the symmetry of short-term control of gait parameters and ob

220 The higher symmetry of the ACI perovskites is expressed in their ph

221 Substrate binding breaks the six-fold symmetry of the complex, allowing five of the six VAT su

222 (2varphi), breaking the four-fold rotational symmetry of the crystal.

223 ered as a precursor state with the preserved symmetry of the cubic austenite phase.

224 A near symmetry of the data about the angle of -40 degrees and

225 The tetragonal symmetry of the dianionic template creates a nanoscale v

226 coarse-grained protein corresponding to the symmetry of the dimeric protein; this model relaxes this

227 ghted by interactions that disrupt the cubic symmetry of the GaAs lattice, resulting in quadrupolar s

228 til they become strong enough to restore the symmetry of the ground state.

229 The dynamic geometry and the symmetry of the hybrid macroions are largely affected by

230 ic amphiphiles due to the monodispersity and symmetry of the hydrophobic dendritic block, which signi

231 raction data, we re-evaluate the space group symmetry of the intermediate-temperature phase to R3 .

232 ross speeds also correlated with the spatial symmetry of the locomotor pattern, but not with temporal

233 rities are intimately related to the spatial symmetry of the nonlinear media.

234 al transition without losing the crystalline symmetry of the parental phase and provides an effective

235 Relying on the symmetry of the problem, we extracted the 3-dimensional

236 ble morphological outcomes, depending on the symmetry of the propagating solidification front and its

237 The 12-fold rotational symmetry of the quasicrystal is broken in sublayers, for

238 hysical mechanism that ensures the bilateral symmetry of the spinal column.

239 ed by an electric field without breaking the symmetry of the structure of the thin film, and realize

240 We find that the energy and the symmetry of the surface polariton phonon modes depend on

241 g is influenced by both the crystallographic symmetry of the system and the presence of dynamics.

242 reviously presented where the global crystal symmetry of the system plays the major role.

243 ond terminal ethynyl group that restores the symmetry of the system, the triplet state is again found

244 ation and the two-dimensional spatial-parity-symmetry of the transverse single-photon field.

245 terface, caused by epitaxial strains, broken symmetry, off-stoichiometry and charge transfer, can gen

246 To determine the symmetry on retinal image grading of fellow eyes for ret

247 The influence of electronic symmetry on triplet state delocalization in linear zinc

248 bond type, stereochemistry, ring membership, symmetry, or molecular size.

249 pendent superlattice does not change lattice symmetry over the course of continuous growth, whereas t

250 ral change without disrupting the pentameric symmetry (pCRP*).

251 etrical motion per se does not contribute to symmetry perception, limiting the lifetime of pattern el

252 any system with a twofold degenerate broken-symmetry phase, including electronic nematic order assoc

253 t, the electronic properties of these broken symmetry phases are extremely difficult to control due t

254 The symmetry phenotype correlated with Tourette syndrome pol

255 the second principle is correlated activity symmetry planes that exist on many levels within a singl

256 rge number of degrees of freedom and lack of symmetry pose a challenge to studying the chemical detai

257 axes and 30 turrets with apparent hexameric symmetry positioned on the icosahedral 2-fold axes.

258 ichalcogenide (TMDC) with a broken inversion symmetry possesses two degenerate yet inequivalent valle

259 origin of this periodicity is rooted in the symmetry presented in wurtzite hexagonal lattice structu

260 ons are analyzed, which are distinguished in symmetry properties and polarization conversion regime o

261 ory principles we show that these states are symmetry-protected against the information loss and thus

262 s are generally symmetric, and, accordingly, symmetry provides a powerful guide for developing new de

263 phase shift is determined by the interaction symmetry rather than the precise experimental parameters

264 is only approximately 0.017%, the concurrent symmetry reduction results in an optical second harmonic

265 /p(0) orbital mixing with d(10) orbitals and symmetry reduction upon cupriphication of cyclic trinucl

266 gest that proton channels are established at symmetry-related locations in four subunits of the membr

267 With the transverse spin cone symmetry restricted to be two-fold, the one-step sharp m

268 the molecular control of embryonic bilateral symmetry.Retinoic acid (RA) regulates the maintenance of

269 antum band insulators, our theory identifies symmetry settings with previously hidden forms of band t

270 o full angular and spatial search within the symmetry space.

271 itation at frequencies related to the broken-symmetry state.

272 leading to a complex phase diagram of broken symmetry states.

273 thermal fluctuations overcome them, and high-symmetry structures are realized.

274 gy for the preparation of large, hollow high-symmetry structures.

275 er symptom-based phenotypes across analyses: symmetry (symmetry, evening up, checking obsessions; ord

276 zes a new rhombohedral structure with higher symmetry that leads to a multivalley Fermi surface and a

277 ance solid/liquid/gas phases) have different symmetries, the phase transitions among them can be expl

278 tensite (T1) phase with preserved cubic-like symmetry through an isostructural phase transition.

279 entral boundary of leaves defines an axis of symmetry through the centre of the organ separating the

280 are proposed which take advantage of higher symmetries to vastly reduce the dispersion.

281 We used the permutation test of symmetry to assess differences between NRS and non-NRS p

282 tals in the presence of broken time-reversal symmetry (TRS) or space-inversion symmetry.

283 cally they require breaking of time-reversal symmetry, typically achieved using magnetic materials an

284 y ordered states that break various discrete symmetries, verify the high-fidelity preparation of thes

285 thesis of a nanographene propeller with a D3-symmetry was obtained starting from 7,8-dibromo[5]helice

286 cks, which are able to pack with icosahedral symmetry, we examine how stable these highly symmetric s

287 methane compounds 7 depicting broken/reduced symmetry were successfully isolated and fully characteri

288 zations, which generates an expanded helical symmetry when compared to other dynamins.

289 llic surface states protected by crystalline symmetry, which are a versatile platform for exploring t

290 r-weight oligomers with an apparent two-fold symmetry, which are efficient inhibitors of non-fibrilla

291 cal field inhomogeneity due to reduced field symmetry, which can be further elevated by artificially

292 onstrate spin-orbit effects with a different symmetry, which could help generate arbitrary spin polar

293 d metal helix slat structures with four-fold symmetry, which exhibits nonresonant Drude-like response

294 ginary fields on a lattice exhibiting chiral symmetry, which form two strands that interleave along t

295 ipolar phase spontaneously breaks rotational symmetry while preserving translational invariance.

296 ngements and their interplay break inversion symmetry, while informatics tools learn from available d

297 tal dichalcogenides as a result of their low symmetry, with a characteristic in-plane anisotropy due

298 ugates is organized according to a hexagonal symmetry, with ZnPcs hosted in the interstices of the pe

299 ed with a new metastable phase of monoclinic symmetry within bulk KNbO3 is reported.

300 ering interaction, that breaks time-reversal symmetry within the waveguide-resonator system.