ライフサイエンスコーパス: crystal lattice

1 would combine coherently charge, spin, and a crystal lattice.

2 ell understood how gases transport through a crystal lattice.

3 tallinity and the molecular arrangement in a crystal lattice.

4 changes resulting from contact zones in the crystal lattice.

5 il-like assembly that runs the length of the crystal lattice.

6 etaI with the hybrid domain swung out in the crystal lattice.

7 s for bringing the molecules together in the crystal lattice.

8 fluorescent dye physically integrated in the crystal lattice.

9 ach SO(3)(-) group is involved in within the crystal lattice.

10 PIM)(Ar(Tol)CO(2))(2)] (7) units in the same crystal lattice.

11 change in shape on incorporation within the crystal lattice.

12 r mobility is to introduce strain within the crystal lattice.

13 fer, and the remainder is contributed by the crystal lattice.

14 symmetric unit that are unconstrained by the crystal lattice.

15 ther within carbonate ions in the bioapatite crystal lattice.

16 homodimeric Zn3 structure that formed in the crystal lattice.

17 g resistance to conformational change by the crystal lattice.

18 ze of voids around the N(3)-N(4) bond in the crystal lattice.

19 bon dioxide to voids within the channel-free crystal lattice.

20 streptavidin loops exposed to solvent in the crystal lattice.

21 a high degree of stereocontrol provided by a crystal lattice.

22 aithfully undergo this transition within the crystal lattice.

23 and side-chain conformations observed in the crystal lattice.

24 are often incommensurate with the underlying crystal lattice.

25 with the two enantiomers alternating in the crystal lattice.

26 lel association of receptor molecules in the crystal lattice.

27 f the phosphorylated Spo0F with Spo0B in the crystal lattice.

28 radiation is efficiently transferred to the crystal lattice.

29 peded when the protein is constrained in the crystal lattice.

30 etric positioning of the subunits within the crystal lattice.

31 monomeric and without close contacts in the crystal lattice.

32 change with the water species located in the crystal lattice.

33 ising from proximate carborane anions in the crystal lattice.

34 er that breaks translational symmetry of the crystal lattice.

35 ence on the formation of a three-dimensional crystal lattice.

36 er or the 3(1) helical fiber observed in the crystal lattice.

37 tions between four Ala-10(56) trimers in the crystal lattice.

38 either mirror or inversion sites within the crystal lattice.

39 mplete allosteric transitions within another crystal lattice.

40 ent in a specific direction in the hexagonal crystal lattice.

41 ected the intermolecular interactions in the crystal lattice.

42 he D-complex into the chiral beta-CD complex crystal lattice.

43 on to proceed with minimal distortion of the crystal lattice.

44 cleosomes pack against each other within the crystal lattice.

45 essential, tunable component in the overall crystal lattice.

46 which appears to have been hydrolyzed in the crystal lattice.

47 and induce an unexpected contraction of the crystal lattice.

48 it also forms a closed octameric ring in the crystal lattice.

49 erative interactions of these cations in the crystal lattice.

50 we attribute to the hydration of the P3MEEMT crystal lattice.

51 precise deposition of fluids on the photonic crystal lattice.

52 d and their highly organized assembly in the crystal lattice.

53 e void spaces between pentacene units of the crystal lattice.

54 l rocking motion of protein molecules in the crystal lattice.

55 ve-like state, most likely stabilized by the crystal lattice.

56 and local concentration of both atoms in the crystal lattice.

57 which withstand solvent evacuation from the crystal lattice.

58 objects being investigated are embedded in a crystal lattice.

59 irpin, which assembles hierarchically in the crystal lattice.

60 hese additives are often occluded within the crystal lattice.

61 ectrons owing to their interactions with the crystal lattice.

62 related tetrameric forms of Vps75 within the crystal lattice.

63 - and postphosphotransfer states in the same crystal lattice.

64 n, the N-terminal domain only does so in the crystal lattice.

65 ion of THz radiation with optical phonons in crystal lattices.

66 ic linker molecules in these perovskite-like crystal lattices.

67 vivax and Plasmodium falciparum in different crystal lattices.

68 -hexamer stacking as visualized in classical crystal lattices.

69 m inspection of 14 independent Hh-containing crystal lattices.

70 s dimers in A33 crystals with five different crystal lattices.

71 nalogous to substitutional doping of ions in crystal lattices.

72 perovskites due to their mobile and fragile crystal lattices.

73 ement of the molecules within the respective crystal lattices.

74 ient interaction between the protons and the crystal lattices.

75 a complete match of the parameters of their crystal lattices.

76 In the crystal lattice, 2a further assembles into a left-handed

77 phenol is lost, was the only tautomer in the crystal lattice according to single-crystal X-ray diffra

78 Heat is transported out of the crystal lattice (across the solid-liquid interface) by a

79 rangement of nanocrystals, strengthening the crystals lattice against phase transitions induced by he

80 int-atoms, random sphere packings, or simple crystal lattices; all of these models assume central-for

81 he adsorbed molecule relative to the Cu(110) crystal lattice, allowing one to witness changes in the

82 Their inherently soft crystal lattice allows greater tolerance to lattice mism

83 All three crystal lattices also include solvated Mg(II) and perchl

84 suggest that fluoride incorporation into the crystal lattice alters the crystal surface to enhance am

85 as been achieved in an organic semiconductor crystal lattice (although a pi-pi distance of 3.04 A has

86 interaction, the extended environment in the crystal lattice and a temperature-dependent pentane rear

87 the red form is devoid of solvent within the crystal lattice and contains complexes stacked with a ne

88 tant mixtures result in a nearly defect-free crystal lattice and high uniformity of nanowire diameter

89 the GGGGTTTTGGGG DNA also packing within the crystal lattice and interacting with the telomere end bi

90 The crystal lattice and protein core are conserved compared

91 ows like a viscous fluid while retaining its crystal lattice and remaining a strong and stiff metal.

92 n is important for minimizing defects in the crystal lattice and results in a substantial increase of

93 sible four dimeric conformations seen in the crystal lattice and strongly implicate one as the biolog

94 without consideration of the effects of the crystal lattice and thermal motion.

95 active site of a neighboring molecule in the crystal lattice and thus serves as an excellent model fo

96 were observed to react with NaMN within the crystal lattice and undergo the phosphoribosyl transfer

97 o determine the strain tensor of a distorted crystal lattice and we measure the critical dislocation

98 h AcMNPV and CPV polyhedra possess identical crystal lattices and crystal symmetry.

99 lphaL I domain determined in seven different crystal lattices and in solution, and which are present

100 ively.Mg(2+)and Ca(2+)generate different DNA crystal lattices and stabilize different end-to-end over

101 insensitivity of skyrmions to the underlying crystal lattices and thus the possible more ubiquitous p

102 n the normal state are commensurate with the crystal lattice, and the intensity is peaked around the

103 tion, the In(3+) ions diffuse out of the CIS crystal lattice, and the remaining copper sulfide adopts

104 onship between these structures, captured in crystal lattices, and hemoglobin structure in solution r

105 the Mg(2+)and Ca(2+)-forms, duplexes in the crystal lattice are surrounded by 13 magnesium and 11 ca

106 ity, sharp phonon modes (oscillations in the crystal lattice) are exchanged between electrons within

107 o different inhibitor molecules bound in the crystal lattice, as determined by X-ray crystallography.

108 hylene vibrations as the anhydrous milk fats crystal lattice became more ordered.

109 More importantly, static, crystal-lattice bound complexes do not address the influ

110 ys-26 and Arg-79, on tiling, not only in the crystal lattice but also in the bacterial cytoplasm.

111 shared between two amylase molecules in the crystal lattice, but also occupying a portion of the sub

112 n forms the physiological 2-dimensional (2D) crystal lattice, but full-length protein crystallizes mu

113 s related by a screw axis, can be fit in the crystal lattices, but model refinement will require accu

114 hat originate from their non-centrosymmetric crystal lattice-but also lend their crystalline mechanic

115 ificant lattice distortion and decreases the crystal lattice by 1.07% in the a axis and 3.18% in the

116 manner and was observed as a tetramer in the crystal lattice by size exclusion chromatography, dynami

117 inder of the sugar is then modelled into the crystal lattice by superimposing the appropriate oligosa

118 alone; a large thermal agitation inside the crystal lattice can trigger the irreversible displacemen

119 ine, and characterized by a less substituted crystal lattice compared with benign samples.

120 , corroborating the noncentrosymmetry of the crystal lattice composed of chiral cholesterol molecules

121 A crystal lattice comprising uniformly staggered C5H5 ring

122 uent simulations of both structures in their crystal lattices confirmed this conclusion.

123 The crystal lattice consists only of PAK4-PAK4 contacts, whi

124 tional behavior of the LBD in the absence of crystal lattice constraints, and thus better to apprecia

125 mylase structure we report is independent of crystal lattice contact restraints and represents the th

126 constructing a point mutant that destroys a crystal lattice contact stabilizing the wild-type polyme

127 Furthermore, an integrase tetramer formed by crystal lattice contacts bears structural resemblance to

128 mmetric unit contains only a single monomer, crystal lattice contacts bring two monomers together to

129 The effect of altered crystal lattice contacts on segment flexibility becomes

130 ng site at one end of the beta-barrel whilst crystal lattice contacts suggest a model for the full-le

131 tin-2.IP(6) complex was solved to 2.9 A with crystal lattice contacts suggesting two sites on a prote

132 emoglobin tetramers where it participates in crystal lattice contacts unique to the pH 5.4 structure.

133 haperone surfaces participate extensively in crystal lattice contacts, we speculate that the observed

134 urface flexibility, and potential to mediate crystal lattice contacts.

135 turally conserved and which are perturbed by crystal lattice contacts.

136 The asymmetric unit of the crystal lattice contains a dimer comprised of two differ

137 The crystal lattice contains an unprecedented trimeric arran

138 However, contacts in the crystal lattice could have stabilized a conformation whi

139 accommodating both As(5+) and As(3+) in the crystal lattice coupled with simple chemistry and easy c

140 In the crystal lattice, CTLA-4 and B7-1 pack in a strikingly pe

141 the reaction pathway along which the DNO(2)A crystal lattice deforms to finally become the crystal la

142 rstitial sites and fluctuate position in the crystal lattice demonstrates the dynamic behavior of H2

143 A variety of different crystal lattices diffracted up to 1.85 nm by electron mi

144 rystal lattice structure, causing measurable crystal lattice distortion in powder X-ray diffraction p

145 modulating the spin-orbit interaction or the crystal lattice, driving the system through a topologica

146 ate that, despite the small variation in the crystal lattice during lithiation, pronounced structural

147 ties unintentionally introduced into the ZnS crystal lattice during synthesis, which act as deep trap

148 particle-connecting DNA duplexes within the crystal lattice, essentially transforming them from loos

149 der diffraction measurements reveal that its crystal lattice expands along the c axis of its trigonal

150 growth orientation of crystal plane, and the crystal lattice expands as Fe replaces Ga site.

151 a larger supramolecular state that spans the crystal lattice, featuring a steric-zipper motif that is

152 The role of the crystal lattice for the electronic properties of cuprate

153 y Diffraction analysis revealed the wurtzite crystal lattice for ZnO-NPs with no impurities present.

154 It appears that the crystal lattice forces overcome the weak edge-to-face in

155 gnetically confined fermions diffracted by a crystal lattice has remained beyond the reach of laborat

156 mixing and structural distortions within the crystal lattice have been quantitatively measured near t

157 was determined that the water species in the crystal lattice have restricted motional dynamics.

158 ning the protein-protein interactions in the crystal lattice, HinP1I could be dimerized through two h

159 in addition to trapping both products in the crystal lattice, implicate one magnesium ion, previously

160 ive site of an adjoining protein unit in the crystal lattice in a presumed enzyme-product complex.

161 The crystals grew with a type II crystal lattice in contrast to the typical type I packin

162 tures of Co2+, Ni2+, and Zn2+ share the same crystal lattice in different proportions to allow the fo

163 These results show both the effects of a crystal lattice in limiting quaternary structural transi

164 se negligible distances through the pristine crystal lattice in minerals: this is a fundamental assum

165 imply that the magnetic interaction with the crystal lattice in MnBi is considerably more complex tha

166 ound to NaMN because it is hydrolyzed in the crystal lattice in the absence of the second substrate D

167 n-field theory to show the importance of the crystal lattice in the breakdown of the correlated insul

168 her by DNA "bonds", offers a route to design crystal lattices in a way that nature cannot: through al

169 es of the actin x-ray structure, outside the crystal lattice, in an aqueous environment with profilin

170 HER4 form similar chains in their respective crystal lattices, in which N-lobe dimers are linked toge

171 e arrangement of protein monomers within the crystal lattice: in a looser packing, the one-bond-flip

172 mulation of the biotin-liganded streptavidin crystal lattice, including cryoprotectant molecules and

173 nic bonding nature results in highly dynamic crystal lattices, inherently allowing rapid ion exchange

174 An unusual crystal lattice interaction of dsRNA with its symmetry m

175 physiological crystallization conditions and crystal lattice interactions, the crystal structures ref

176 nt and not merely a consequence of different crystal lattice interactions.

177 The behaviour of electrons and holes in a crystal lattice is a fundamental quantum phenomenon, acc

178 to protein-protein contact formation in the crystal lattice is a major obstacle to predicting and op

179 Accumulation of M intermediate within the crystal lattice is confirmed by time-resolved visible ab

180 anism that also requires the rotation of the crystal lattice is demonstrated.

181 ctures reveals that isomer preference in the crystal lattice is due to general shape selectivity.

182 s of beta2-microglobulin native state in the crystal lattice is in keeping with what observed in solu

183 water molecules through channels within the crystal lattice is observed, yet the average water densi

184 nvolving the IRMOF-74 series assume that the crystal lattice is rigid.

185 A Na+ ion in the crystal lattice is water bridged to two N1 atoms of symm

186 ductors, the distribution of dopant atoms in crystal lattices is often random.

187 water intermolecular interactions in the two crystal lattices is possible.

188 ead-to-head NS1(172-352) dimer we observe in crystal lattices is supported by multiangle light and sm

189 ervation of structure in the three different crystal lattices is very high, binding of MES is correla

190 how the conserved biological phenotype, the crystal lattice, is maintained in the face of extreme en

191 ctions an electron experiences from the host crystal lattice, lattice defects and the other approxima

192 r induces a reorganization of the monoclinic crystal lattice leading to a disorder-order transition o

193 ordering of metal atoms within the selenium crystal lattice, leading to a large separation between m

194 oncanonical base-pairing interactions in the crystal lattice leads to predictably modified crystal ha

195 ion entities and anions, and for stabilising crystal lattices, like in coordination polymers.

196 Dyn2 homodimers are arrayed in the crystal lattice, likely mimicking the arrayed architectu

197 omers in the asymmetric unit may result from crystal lattice limitations since atmospheric oxygen bin

198 lar flexibility was increased to disturb the crystal lattice, lower the melting point, and thereby im

199 Two symmetry mates within the crystal lattice make a contact that likely represents th

200 , DM-mediated coupling between chirality and crystal lattice may give rise to a new kind of spin-Peie

201 ucing defective microstructures into a metal crystal lattice may induce distortions to form non-face-

202 e-earth intermetallics with highly symmetric crystal lattices may ubiquitously host nanometric skyrmi

203 itional factors, possibly contributed by the crystal lattice, may strongly impact mesoscale ET mainly

204 noacrylate intermediate, suggesting that the crystal lattice might prevent a ligand-induced conformat

205 Longitudinal packing in the crystal lattice mimics packing observed by EM of in-vitr

206 quisite control over the patterned substrate/crystal lattice mismatch, something not yet realized for

207 romatic-aromatic interactions that mimic the crystal lattice of benzene.

208 lectrodynamic properties are dictated by the crystal lattice of h-BN.

209 ur design exploited the observation that the crystal lattice of Hcp1 contains rings stacked in a repe

210 urally occurring, two-dimensional triangular crystal lattice of hundreds of spin-half particles (bery

211 e of LFS particles, but also enters into the crystal lattice of LFS.

212 ors are probed within the scaffolding of the crystal lattice of Phe-131-->Val carbonic anhydrase II.

213 ntrolled introduction of impurities into the crystal lattice of solid-state compounds is a cornerston

214 e dimeric forms, but it was unclear from the crystal lattice of the activated protein precisely which

215 rystal lattice deforms to finally become the crystal lattice of the AQ product.

216 d, fully coherent precipitates (that is, the crystal lattice of the precipitates is almost the same a

217 xes, which revealed over 400 cases where the crystal lattice of the target in the free form is such t

218 both environments but forms two-dimensional crystal lattices of different symmetries.

219 ypothesized to occur via a match between the crystal lattices of the salt and the growing oxide.

220 essure exerted by the gaseous product in the crystal lattices of these materials.

221 separate parallel dimers are observed in the crystal lattice, offering intriguing models for receptor

222 ework shape and metal-metal distances in the crystal lattice opens up unparalleled prospects for mate

223 andscapes are computed in the context of the crystal lattice or multimer.

224 E assembles as an antiparallel dimer in the crystal lattice organized in a highly similar fashion as

225 atory-based methods both to determine the Ih crystal lattice orientation relative to a surface and to

226 In the crystal lattice, oxalic acid is H-bonded directly to the

227 structure around Ag and evaluate changes in crystal lattice parameters and structure as a function o

228 of ice: ice does not readily cleave along a crystal lattice plane and properties of ice grown on a s

229 The discrete nature of crystal lattices plays a role in virtually every materia

230 Concurrent measurements of the crystal lattice point to a critical transition that is c

231 We have shown that the crystal lattice preorganizes the reactant molecules towa

232 esolution EM image of these particles in the crystal lattice produced phases accurate enough to locat

233 fy that mobile dopants weakly coupled to the crystal lattice provide a means of imbuing a reversible

234 e molecular constraints inherited within the crystal lattice provide an optimal environment that lead

235 Synthetic crystal lattices provide ideal environments for simulati

236 Differences among 10 molecules in crystal lattices provide unprecedented information on in

237 parent phase involving the symmetry-lifting crystal lattice rearrangement of the product phase.

238 e colors, by changing the orientation of the crystal lattice relative to the incident light using mag

239 e through nuclear-nuclear collision with the crystal lattice remains largely unaddressed.

240 s reveal distinctive laser-fluence dependent crystal lattice responses, which are not described by pr

241 Diffraction from an ideal crystal lattice results in an identical copy of this con

242 cals along a <100> direction (a axis) of the crystal lattice results in the transition temperature (T

243 domains of MAdCAM in a previously described crystal lattice revealed two alternative conformations o

244 as species of 'zero charge' incorporated at crystal lattice sites.

245 also demonstrate a method for measuring the crystal lattice spacing in a single shot that contains o

246 Following determination of the crystal lattice spacing of 3.5 nm and of a phase transit

247 anges and the extensive rearrangement of the crystal lattice structure allow the alpha heme group of

248 s remain in the hexagonal close-packed (hcp) crystal lattice structure, accompanied by a monotonic in

249 is frequently bound to the Pb(II) phosphate crystal lattice structure, causing measurable crystal la

250 Analysis of multiple crystal lattices suggests modes by which the ligand-bind

251 ns using Bragg peak patterns, but only up to crystal lattice symmetry.

252 n twinning (the sudden re-orientation of the crystal lattice), takes over as the dominant mode of dyn

253 el, and it forms a tight tetramer within the crystal lattice that has circular 4-fold symmetry.

254 he structure also reveals a dPC dimer in the crystal lattice that is mediated by residues specificall

255 lu44 from a symmetry-related molecule in the crystal lattice that mimics the binding of methotrexate

256 self-trapping due to a local heating of the crystal lattice, that can be described as a collective p

257 We find that in both crystal lattices the oligonucleotide forms an antiparall

258 In the crystal lattice, the carbonyl oxygen of the central glyc

259 or removal of interstitial solvent from the crystal lattice, the channels within enzyme crystals are

260 In the crystal lattice, the interacting domains are contributed

261 -to-groove packing interactions occur in the crystal lattice, the latter positioned in the minor groo

262 In the crystal lattice,the periodic arrangement of GpIbalpha-th

263 biradical precludes its penetration into the crystal lattice; therefore, intimate contact of the mole

264 r-helix bundle of the M-fragment, and in the crystal lattice these domains exist as dimers.

265 and poor tendency to form highly ordered 3D crystal lattices, they have evaded high-resolution struc

266 In the crystal lattice, three dimers associate around a 3-fold

267 two molecular-layer spacings, distorting the crystal lattice to a larger extent.

268 D6 exhibits sufficient elasticity within the crystal lattice to allow the passage of compounds betwee

269 quire the coupling between electrons and the crystal lattice to be taken into account.

270 V-1 strains, as well as the engineering of a crystal lattice to enable structure determination of the

271 Two trimers associate face-to-face in the crystal lattice to form a hexamer; four trimers in a tet

272 w zinc-binding domain self-associates in the crystal lattice to form a homodimer with a head-totail a

273 associates with a neighboring protein in the crystal lattice to form an extra beta-strand.

274 tanding of the molecular interactions in the crystal lattice to improve both cellular potency and sol

275 he hammerhead ribozyme by using a reinforced crystal lattice to trap the complex prior to dissociatio

276 n the physiological reaction occurred in the crystal lattice to yield nicotinate and alpha-ribazole-5

277 xes connect the helices and help to knit the crystal lattice together.

278 croscopic structural analysis shows that the crystal lattice twist is consistent with the geometric t

279 The migration of point defects, for example, crystal lattice vacancies and self-interstitial atoms (S

280 d into oligomers and form long fibres in the crystal lattice, via coiled-coil interactions in the N-t

281 n probes intermolecular interactions through crystal lattice vibrations, allowing the characterizatio

282 arameters to the correct oxygen sites in the crystal lattice was achieved with the aid of DFT calcula

283 nesium (MgATP) and trap both products in the crystal lattice, we asked here whether calcium could tra

284 By trapping both products in the crystal lattice, we now have a complete resolution profi

285 ynamics of swimming bacteria in microfluidic crystal lattices, we show that hydrodynamic gradients hi

286 s are incorporated into the molecule and the crystal lattice where they neutralise positive charges o

287 mmetric electron density distribution in the crystal lattice whereas radical 11 is the only monomeric

288 owever, the difficulty in obtaining periodic crystal lattices which are needed for X-ray crystal anal

289 aries between six degenerate states of their crystal lattice, which are locked to both ferroelectric

290 ggests incorporation of the TT unit into the crystal lattice, which is accompanied by an increase in

291 The role of the crystal lattice, which is important in conventional supe

292 ons arise from defects within a CuAl(5) S(8) crystal lattice, which supports the experimental observa

293 defined by dislocations-line defects in the crystal lattice whose motion results in material slippag

294 included angle (60 degrees ), while a quasi-crystal lattice with 12-fold rotational symmetry yields

295 ntational motion of protein molecules in the crystal lattice with an 3-5 degrees amplitude on a tens-

296 In the same spirit, deformations of the crystal lattice with light may be used to achieve functi

297 raction measurements to study the changes in crystal lattice with temperature.

298 The two complexes crystallized in different crystal lattices with respective crystal data of space g

299 rol-bound NPC2 were observed within the same crystal lattice, with an asymmetric unit containing one

300 e protein exists as a dimer of dimers in the crystal lattice, with two spatially separated active sit