ライフサイエンスコーパス: lattice

1 for the case of a two-dimensional hexagonal lattice.

2 ontiguously bound cofilin along the filament lattice.

3 ally decreasing the band gap of the expanded lattice.

4 and display a characteristic square surface lattice.

5 paces between pentacene units of the crystal lattice.

6 eV by altering hydrogen incorporation in the lattice.

7 model of interacting quantum particles in a lattice.

8 s of CA-SP1 junction helices in the immature lattice.

9 periodic translation symmetries of the chain lattice.

10 mplement a four-dimensional (4D) topological lattice.

11 tronic effects within the extended framework lattice.

12 hat together define a three-dimensional (3D) lattice.

13 ness is nearly linear in the muscle filament lattice.

14 rs of Neel antiferromagnets on the honeycomb lattice.

15 argets more gamma-TuRC along the microtubule lattice.

16 nteractions that stabilize the curved capsid lattice.

17 non frequencies in the deuterated perovskite lattice.

18 or mechanically shaping them in the photonic lattice.

19 lysis to mechanical movement along a polymer lattice.

20 ompressed (GMPCPP) dimers in the microtubule lattice.

21 ate of tubulin dimers within the microtubule lattice.

22 ssibility near integer fillings of the moire lattice.

23 ted targeting of the hantaviral glycoprotein lattice.

24 during which CA molecules are shed from the lattice.

25 itochondrial networks aligned with myofibril lattices.

26 is one of the most geometrically frustrated lattices.

27 f applications relying on coherent Bosons in lattices.

28 entered cubic (fcc) crystalline nanoparticle lattices.

29 nanoparticles (NPs) in two-dimensional (2D) lattices.

30 nces for the same polymer in the two polyMOF lattices.

31 zed Wigner crystallization on the underlying lattice(6-11).

32 n honeycomb and square-hexagonal-dodecagonal lattices(6), respectively.

33 e evidence that the pure ferromagnetic Kondo lattice(9,10) CeRh(6)Ge(4) becomes a strange metal at a

34 an illustration, we consider twisted kagome lattices(9-15), reconfigurable mechanical structures tha

35 can broadly be classified into: on- and off-lattice agent containers, finite difference diffusion fi

36 tatic energy of the dopant in the perovskite lattice and (ii) the elastic energy of the dopant due to

37 been successfully used to study a variety of lattice and continuous-space problems.

38 the absence of both geometrically frustrated lattice and inversion symmetry breaking.

39 mino)benzene linker that form a Kagome (kgm) lattice and show strong visible light absorption.

40 is used to directly image Neel-type skyrmion lattice and the stripe-like magnetic domain structures a

41 h the vRNPs were mislocalized between the CA lattice and the viral lipid envelope.

42 create topologically well-defined polygonal lattices and built-in discrete micropores and/or mesopor

43 les have been found more recently in optical lattices and two-dimensional materials(4-9).

44 The realization of a spin S = 1/2 kagome lattice antiferromagnet is of particular interest becaus

45 A few S = 1/2 kagome lattice antiferromagnets exist, typically based on Cu(2+

46 Here we directly image lattice-aperiodic valley interference between coupled at

47 permeation through defects in the graphenic lattice are still unclear and remain unobserved in actio

48 alks in new proposed quasiperiodic photonics lattices are highly controllable due to the deterministi

49 than the number of open Zr sites in the MOF lattice around each Pt NP.

50 (HIV-1) capsid (CA) protein forms a conical lattice around the viral ribonucleoprotein complex (vRNP

51 e materials depend on cooperative changes in lattice arrangements in response to external perturbatio

52 wave convergence is proposed by assembling a lattice array of concave hexagonal (CH)-shaped rods.

53 noscale proximity, within a perovskite oxide lattice as well as on its surface.

54 By modeling viral lattice assembly and recapitulating oscillations in prot

55 uss an experiment conducted on a polaritonic lattice at ambient conditions: We utilize fluorescent pr

56 ocal structural distortion of the bimetallic lattice at the nanoparticle surfaces.

57 ein-protein interactions within the HIV-1 MA lattice at the plasma membrane.

58 ence of CLIP-170 remnants on the microtubule lattice at the rear of comets.

59 of interaction to state transitions using a lattice-based model of the thylakoid membrane based on e

60 endogenous nanoparticles and the perovskite lattice become reciprocally strained and seamlessly conn

61 n formation, with a geometrically frustrated lattice being considered essential in this case.

62 ucing the energy bandwidth of electrons in a lattice below the long-range Coulomb interaction energy

63 These chains stack to form 2D matrix lattices below the membrane surface.

64 further assemble into tetrameric spikes, the lattice building blocks.

65 rolytes for batteries, not only the periodic lattice but also the non-periodic features that disrupt

66 u(2)Si(2) without a geometrically frustrated lattice by means of resonant X-ray scattering and Lorent

67 Here we present a three-dimensional lattice called the hyper-hyperkagome that enables spin l

68 n, centrosymmetric magnets with a triangular lattice can also give rise to skyrmion formation, with a

69 and ~250 nm height, that provides a rhombic-lattice canvas of a thousand pixels each, with pitch of

70 a reversible phase transformation with a 7% lattice change and dramatic modulation in chemical, elec

71 exhibit a first-order PIPT accompanied by a lattice change.

72 odes, suggesting a strong coupling among the lattice, charge and spin in two-dimensional CrI(3).

73 The kagome lattice, composed of a planar array of corner-sharing tr

74 A class of antiferromagnetic honeycomb lattices compounds, A(4)B(2)O(9) (A = Co, Fe, Mn; B = Nb

75 scopic, and theoretical analyses reveal that lattice compression under a mild pressure within 1.6 GPa

76 elastic and can be thermally excited between lattice configurations reversibly.

77 ction, protein-MOFs possess extremely sparse lattice connectivity, suggesting that they might display

78 As the dimensionality of SCO is reduced, the lattice constant elongates over 10% along the growth dir

79 hrates are energetically stable with relaxed lattice constants matching the experimental data.

80 ystem can be directly tuned by adjusting the lattice constants of the phases.

81 ces(6) because of the difference between the lattice constants of the two materials.

82 ns of the interacting surfaces are free from lattice contacts and therefore accessible to fragments d

83 n(2+)(0.5-8.0%) are introduced, resulting in lattice contraction as well as phosphorescence from five

84 The alpha-Ti phase shows a lattice contraction which is invariant with cooling rate

85 ismatic Basal interfaces which establish the lattice correspondence of the twin with a minor deviatio

86 kyrmions and ordered and disordered skyrmion lattices could also give rise to many fascinating physic

87 Curvature of the graphenic lattice crucially defines the direction of permeation fr

88 microtubule-associated protein CLASP repairs lattice damage by regulating GTP-tubulin incorporation i

89 ss can be attributed to the in situ tailored lattice defects and the strain-induced highly curved mic

90 first time that non-equilibrium atomic-scale lattice defects can be detected in nanoparticles by pure

91 The resulting elastic lattice deformation that follows scanning irradiation of

92 n generate phase-dependent transient elastic lattice deformation.

93 Lattice degrees of freedom are found to be crucially imp

94 The coupling between spin, charge, and lattice degrees of freedom plays an important role in a

95 reflects a coupling among charge, spin, and lattice degrees of freedom that differs not only from th

96 We further obtained the lattice dependent frequency response and damping offered

97 cture calculations reveal that the resulting lattices (direct and inverse) have promising optical pro

98 phosphorylation of membrane lipids can drive lattice disassembly.

99 The lattice discrete particle model also works.

100 ver, the connection between the atomic-scale lattice distortion and macro-scale mechanical properties

101 HEAs and 2) the ambiguity in describing the lattice distortion and related measurements and calculat

102 attice structure, causing measurable crystal lattice distortion in powder X-ray diffraction patterns.

103 cally and quantitatively studied in terms of lattice distortion using a theoretical model, first-prin

104 anisotropy stays the same despite the large lattice distortion.

105 ex interplay between ordering tendencies and lattice distortion.

106 cture instability that leads to Jahn-Teller (lattice) distortion in an octahedral ligand field is the

107 but possibly important differences in size, lattice distortions, and defects, which can only be unde

108 layers, whereas this effect is limited in BP lattices due to their spring-shaped space structure.

109 Here, we report a comprehensive study of the lattice dynamics and superionic diffusion in [Formula: s

110 esults settle unresolved questions about the lattice dynamics and thermal conduction mechanism in [Fo

111 ughly investigated the atomic structures and lattice dynamics by combining neutron scattering techniq

112 the correlation between chemical bonding and lattice dynamics in intrinsically low thermal conductive

113 between Halo and SNAP proteins and verified lattice dynamics in purified VLPs incorporating 10% Gag-

114 Here we combine the nonaffine theory of lattice dynamics valid for disordered condensed matter s

115 iquid water alone can predict the densities, lattice energies, and vibrational properties of the ices

116 ow significant differences in the respective lattice energies.

117 Lattice energy calculations, supported by nanoindentatio

118 t-driven structural transformation, and spin-lattice entanglement in strongly correlated materials.

119 nd illuminated conditions, the mechanism for lattice expansion is in fact fully consistent with heat-

120 67) report a uniform light-induced lattice expansion of metal halide perovskite films under

121 lumination and claim to exclude heat-induced lattice expansion.

122 llatory kinetics associated with the dynamic lattice expansion/shrinking, ordering/disordering, and f

123 ther contribute in preparing the microtubule lattice for future rescues at these predetermined sites.

124 The role of the crystal lattice for the electronic properties of cuprates and ot

125 EDT molecules with spin-1/2 on a triangular lattice form layers which are separated by a sublattice

126 Displacement of the protective 2-dimensional lattice formed by annexin V on trophoblast surfaces by a

127 ibit motional dynamics with respect to rigid lattice-forming crystallization domains.

128 ting of a paracrystalline array of repeating lattice-forming proteins.

129 ed by adjusting the width and spacing of the lattice from 2-100 um.

130 A5 self-assembly into lattices further stabilizes and likely structures the me

131 er systems, such as bosons and fermions in a lattice, gauge theories, high-temperature superconductor

132 Chern quantum phases owing to their unusual lattice geometry and breaking of time-reversal symmetry(

133 ixed dynamics to structured populations on a lattice grid.

134 imulations reveal the spatial constraints on lattice growth and the role of membrane localization and

135 In addition, standard lattices have well known shear and fatigue weaknesses du

136 feature that is characteristic of dynamical lattices, high anharmonicity, and dissipative vibrations

137 se diagram of the two-dimensional triangular-lattice Hubbard model by studying angle-aligned WSe(2)/W

138 ion physics that are described by triangular-lattice Hubbard models.

139 de from the Fe(3+) precursor had an expanded lattice in the Fe(0) body-centered-cubic (BCC) structure

140 ization on the intrinsic stability of the CA lattice in vitro and fates of viral core components in i

141 design multicomponent systems that can form lattices in solution or on the membrane, and we predict

142 for understanding and engineering rich moire-lattice induced phenomena in angle-twisted semiconductor

143 The crystalline lattice insulates mobile electrons from oxidation by O(2

144 The lattice interference and perturbation of atomic periodic

145 -ray diffraction to identify the sequence of lattice interstitial sites preferred by Li-ions to high

146 The observed lattice is composed of three antiferromagnetically coupl

147 ith the ASCII code within a programmable 6x6 lattice is demonstrated to demosntrate the versatility o

148 eveals that isomer preference in the crystal lattice is due to general shape selectivity.

149 a2-microglobulin native state in the crystal lattice is in keeping with what observed in solution.

150 The 2-dimensional Ising model on a square lattice is investigated with a variational autoencoder i

151 l characterization showed that the inorganic lattice is not significantly perturbed even though the l

152 for PIP2 clustering, formation of a regular lattice is not.

153 tudy, we show that destabilization of the CA lattice leads to premature dissociation of CA from viral

154 Importantly, destabilization of the CA lattice led to premature dissociation of CA from vRNPs i

155 issue light-sheet microscopes and reflective lattice light-sheet microscopes.

156 alization, PALM super-resolution imaging and lattice light-sheet microscopy.

157 in low light environments and do not possess lattice-like cone mosaics are congruent with this claim.

158 that are often organized as highly patterned lattice-like distributions.

159 The corollary is that lattice-like patterning of the cone mosaic may improve v

160 parable to those of goldfish, a species with lattice-like periodicity in its cone mosaic.

161 On the microtubule lattice, loads also exponentially decreased the run leng

162 that, beyond Vonnegut's connection with the lattice match to ice, three new microscopic factors help

163 specific heterostructures predicted here are lattice-matched, show no detrimental electronic instabil

164 the Li crystals because of the fine in-plane lattice matching between Li and the rGO substrate, resul

165 havior that can be generated out of the same lattice material by changing the building block into dom

166 between water and biomimetic self-assembled lattice materials (composed of sodium dodecyl sulfate an

167 hydrogen-bond interactions in self-assembled lattice materials is crucial for preparing such material

168 termolecular interactions for self-assembled lattice materials.

169 intermetallics with highly symmetric crystal lattices may ubiquitously host nanometric skyrmions of e

170 factors, possibly contributed by the crystal lattice, may strongly impact mesoscale ET mainly by incr

171 BS is a fluorescently-labeled, ultra-thin FN lattice-mesh with spatial resolution tailored by adjusti

172 We propose a novel hourglass shaped lattice metastructure that takes advantage of the combin

173 , such as hierarchical composites and atomic lattice-mimicking architectures, have achieved optimal c

174 control over the patterned substrate/crystal lattice mismatch, something not yet realized for any epi

175 challenge, owing to the absence of suitable lattice-mismatched epitaxial substrates.

176 6-8), is fundamentally unavoidable in highly lattice-mismatched epitaxy(9-11).

177 the same time, conventional heteroepitaxy of lattice-mismatched systems produces dislocations above a

178 idiagonalization are provided for nontrivial lattice model Hamiltonians, exemplifying convergence ove

179 Here, we consider a lattice model of itinerant spin-[Formula: see text] ferm

180 The theoretical analyses of the coupled map lattice model reveal the underlying instabilities and bi

181 We propose a lattice model that roughly accounts for proteins' attrac

182 opological feature, we use a one-dimensional lattice model with a nearest-neighbor interaction betwee

183 tically study the phase diagram of the Kondo lattice model with a nonmagnetic valence bond solid grou

184 Here we use lattice-model simulations and analytical calculations to

185 metal transition mediated by fully symmetric lattice modes can find extensive application in a pletho

186 the coherent condensate in distinct orbital lattice modes of different symmetries.

187 and three-state majority-vote model on cubic lattice networks.

188 Initially, the molecule binds to a lattice O(2)(-) ion through a photomediated adsorption p

189 I(2) monolayers with the underlying graphene lattice occurs, leading to a phase shift from the 1 T to

190 Optically-refrigerating the lattice of a dielectric resonator has the potential to i

191 can achieve rapid rearrangement of the whole lattice of a metal-organic framework through a domino al

192 rovirus capsid consists of a variably curved lattice of capsid protein (CA) hexamers and pentamers.

193 predetermined positions along the hexagonal lattice of graphene-derived polycyclic aromatic hydrocar

194 ation analysis, and show dynamics within the lattice of immobilized VLPs in the timescale of 10-100 s

195 ch revealed over 400 cases where the crystal lattice of the target in the free form is such that larg

196 for competing magnetic orders in the kagome lattice of this compound.

197 , or interference techniques such as optical lattices of cold atoms.

198 We generated crystalline lattices of Small Tetraheme Cytochromes (STC) forming we

199 xerted by the gaseous product in the crystal lattices of these materials.

200 e-dimensional droplets or in two-dimensional lattices on membrane surfaces, have emerged as another i

201 The Cu-O-Ce site with activated lattice oxygen anchors deposited Pt sub-nanoclusters, le

202 However, lattice oxygen loss and derived structure distortion wou

203 Furthermore, irreversible lattice oxygen loss and structure distortion are effecti

204 , in which water molecules take the place of lattice oxygen of alpha-MoO(3).

205 rease is dominantly a result of the enhanced lattice oxygen participation.

206 The presence of lattice oxygen species with strong Bronsted basicity is

207 ed from their high proportion of surface non-lattice oxygen, through occupying surface oxygen-vacant

208 )O(33,) however, with a significantly larger lattice parameter allowing for the cages that result fro

209 reproduced the nonlinear dependence of the c lattice parameter and have shown that the mixed metal/B

210 lationship between C/Zr atomic ratio and the lattice parameter is critically assessed: it is found th

211 ablished relationship that suggests that the lattice parameter value attains a maximum value at a C/Z

212 bon to zirconium atomic ratio (C/Zr) and the lattice parameter, in contrast with a more established r

213 ur incorporation extended the nano-Fe(0) BCC lattice parameter, reduced the Fe local vacancies, and l

214 the substrate composition-and therefore its lattice parameter-a compressive strain as high as 2.4 pe

215 s, insights into changes in crystallographic lattice parameters, water siting information and water-i

216 ccupy preferably octahedral coordination MgO lattice positions under step-edges, hence highly confine

217 ovide a new class of quasiperiodic photonics lattices possessing both on- and off-diagonal determinis

218 to its strike, suggesting the development of lattice-preferred orientations by substantial stress.

219 mobile dopants weakly coupled to the crystal lattice provide a means of imbuing a reversible and dyna

220 mbered rings that pack within a pseudosquare lattice provide the best agreement with experimental dat

221 e regression algorithm is demonstrated for a lattice quantum chromodynamics simulation data using a D

222 n accelerated 3D mono and biexponential spin-lattice relaxation time in the rotating frame (T(1rho))

223 is an MRI scan that measures the proton spin-lattice relaxation time T(1).

224 The spin-lattice relaxation time T(1rho) values for (1)H, (13)C,

225 Chemical shift anisotropy parameters, spin-lattice relaxation, and molecular correlation times obta

226 at satisfies local detailed balance that the lattice remains elastic and can be thermally excited bet

227 ng procedures to achieve ultranarrow surface lattice resonances (SLRs) with full-width at half-maxima

228 hat introducing N and Mo atoms into C and Ru lattices, respectively, triggers electron accumulation/d

229 y strong C-C and Si-C bonds on the honeycomb lattices, respectively.

230 lters the bond connectivity in the hexagonal lattice, results in a non-Kekule nanographene with an un

231 The EES and electron-lattice scattering are intertwined resulting in breaking

232 critically important factors for crystalline lattice self-assemblies--shedding light on engineering i

233 ynamics of DNA objects constructed using off-lattice self-assembly principles, i.e. wireframe DNA obj

234 ossible route to creating local melting of a lattice (similarly one can create local melting by creat

235 recognizes specific geometries of the curved lattice, simultaneously interacting with three CA protom

236 Raman spectra show lattice softening with increasing size of the A-site cat

237 characterized by about 8% contraction of the lattice spacing and switching of the intercalated ions.

238 topological modes are delocalised over many lattice spacings.

239 rease the level of commensuration in the two lattice spacings.

240 structural parameters of adjacent "breathing lattice" SrCuO(2) (SCO).

241 Here we discover a square skyrmion lattice state with 1.9 nm diameter skyrmions in the cent

242 Our findings highlight the concept of lattice strain and geometry modified nanoreactors, which

243 controlled stoichiometry, 0 <= x <= 2.3, and lattice strain are grown, and the cation site-occupation

244 Separately, lattice strain between thin film oxides and a substrate

245 The dynamic temporal response of the lattice strain change during transient operation was res

246 The lattice strain component predominantly affects the glide

247 er at the Spallation Neutron Source, and the lattice strains in both the cylinder block and head were

248 uently bound to the Pb(II) phosphate crystal lattice structure, causing measurable crystal lattice di

249 the circular holes in a hexagonal or square lattice structure.

250 rectional properties and non-centrosymmetric lattice structure.

251 ellar structure and the template's hexagonal lattice structure.

252 tube assemblies possess a similar underlying lattice structure.

253 These core NECs serve as a hexameric lattice-structured platform for capsid docking and recru

254 he stress-strain responses of 3D-printed LCE lattice structures are shown to have 12 times greater ra

255 bling that found in some heavy-fermion Kondo lattice systems in the vicinity of an antiferromagnetic

256 scaffold-supported ferroelectric crystalline lattice that enables self-healing and a reprogrammable s

257 and each sublattice is a triangular skyrmion lattice that is fractionalized into two parts with an in

258 the sound velocity of SnTe to give glasslike lattice thermal conductivities.

259 Intrinsically low lattice thermal conductivity ([Formula: see text]) in su

260 Here, we discover intrinsically ultralow lattice thermal conductivity (kappa(L)) in the single cr

261 We show ultralow lattice thermal conductivity (kappa(L)) of 0.74-0.47 W/m

262 ven to liquid-like TE materials that exhibit lattice thermal conductivity at lower than the amorphous

263 ined with phonon-anharmonic-induced ultralow lattice thermal conductivity in alpha-MgAgSb.

264 K(-1) for thermoelectric semiconductors with lattice thermal conductivity of 0.4-1.5 W m(-1) K(-1).

265 e to GaAs, but single crystals show very low lattice thermal conductivity of about 4 W m(-1) K(-1) at

266 the PbSe matrix work together to reduce the lattice thermal conductivity, resulting a record high av

267 scattering, but has negligible influence on lattice thermal conductivity.

268 larger sound speeds usually exhibits higher lattice thermal conductivity.

269 The lattice-tip catheter can deliver focal PF to durably iso

270 A novel lattice-tip catheter could safely and rapidly ablate atr

271 d (PF) and radiofrequency energy from a 9-mm lattice-tip catheter.

272 es efficient resonant heat transfer from the lattice to coherent magnons.

273 induces instability causing iodide from the lattice to move away toward grain boundaries.

274 , however, requires structuring beyond their lattices, to interface the functionality at the molecula

275 Consequently, lattice transformations associated with dehydration/deso

276 The outer capsid forms a hexagonal lattice (triangulation number T = 277) composed of 8,280

277 c structural analysis shows that the crystal lattice twist is consistent with the geometric twist of

278 cid) (pbdc) polymers in two archetypical MOF lattices (UiO-66 and IRMOF-1).

279 itin nodes that predictably assemble into 3D lattices upon coordination of various metal ions and dit

280 nature of phase transitions is linked to the lattice V(3+)/V(5+) concentrations of stoichiometric VO(

281 hich forms a highly stable 3D supramolecular lattice via strong intermolecular interactions.

282 At temperatures below ~ 100 K, C(60) lattice vibrational damping is mitigated and the quantum

283 Exciton dynamics can be strongly affected by lattice vibrations through electron-phonon coupling.

284 ritons (PhPs)-infrared (IR) light coupled to lattice vibrations-offering an unprecedented platform fo

285 order groupings of dimers discernible in the lattices we predict early assembly intermediates, and in

286 ing behind a partially unoccupied perovskite lattice, which explains the unusual regenerative propert

287 litates a phase transition in the WO(3) bulk lattice, which further promotes Ir ex-solution at the ox

288 xis forces and forces across the microtubule lattice, which has implications for a range of cellular

289 bonucleoprotein complexes outside the capsid lattice, which led to premature degradation of the viral

290 nce is due to the softness of the perovskite lattice, which permits separation of electrons and holes

291 e from defects within a CuAl(5) S(8) crystal lattice, which supports the experimental observation of

292 purely manganese-based ferromagnetic kagome lattice with atomic resolution.

293 Quantum particles on a lattice with competing long-range interactions are ubiqu

294 ss of models, which are defined on amorphous lattices with fixed coordination number, a realistic fea

295 Lattices with magnetic ions in triangular or tetrahedral

296 ange in regular hexagonal close-packed (hcp) lattices with the least fraction of defects.

297 Furthermore, artificial skyrmion lattices with various arrangements can be patterned usin

298 omb (pseudospin-1/2) and Lieb (pseudospin-1) lattices with vortex beams of topological charge l, opti

299 e the Heisenberg model describing spins on a lattice, with fully adjustable anisotropy of the nearest

300 Clathrin-coated vesicles lose their clathrin lattice within seconds of pinching off, through the acti