ライフサイエンスコーパス: crystal lattice

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

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

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

4 change in shape on incorporation within the crystal lattice.

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

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

7 symmetric unit that are unconstrained by the crystal lattice.

8 ther within carbonate ions in the bioapatite crystal lattice.

9 homodimeric Zn3 structure that formed in the crystal lattice.

10 g resistance to conformational change by the crystal lattice.

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

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

13 streptavidin loops exposed to solvent in the crystal lattice.

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

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

16 are often incommensurate with the underlying crystal lattice.

17 with the two enantiomers alternating in the crystal lattice.

18 lel association of receptor molecules in the crystal lattice.

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

20 radiation is efficiently transferred to the crystal lattice.

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

22 etric positioning of the subunits within the crystal lattice.

23 monomeric and without close contacts in the crystal lattice.

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

25 ising from proximate carborane anions in the crystal lattice.

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

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

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

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

30 either mirror or inversion sites within the crystal lattice.

31 mplete allosteric transitions within another crystal lattice.

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

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

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

35 cleosomes pack against each other within the crystal lattice.

36 essential, tunable component in the overall crystal lattice.

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

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

39 been determined at 2.4 A resolution in a new crystal lattice.

40 ormation, but instead stack to stabilize the crystal lattice.

41 e conformationally different subunits in the crystal lattice.

42 which withstand solvent evacuation from the crystal lattice.

43 objects being investigated are embedded in a crystal lattice.

44 irpin, which assembles hierarchically in the crystal lattice.

45 hese additives are often occluded within the crystal lattice.

46 ectrons owing to their interactions with the crystal lattice.

47 related tetrameric forms of Vps75 within the crystal lattice.

48 - and postphosphotransfer states in the same crystal lattice.

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

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

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

52 ell understood how gases transport through a crystal lattice.

53 tallinity and the molecular arrangement in a crystal lattice.

54 changes resulting from contact zones in the crystal lattice.

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

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

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

58 fluorescent dye physically integrated in the crystal lattice.

59 vivax and Plasmodium falciparum in different crystal lattices.

60 -hexamer stacking as visualized in classical crystal lattices.

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

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

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

64 ement of the molecules within the respective crystal lattices.

65 mined the structures of intact sCD4 in three crystal lattices.

66 s that serve as synthons for the assembly of crystal lattices.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

81 The crystal lattice and protein core are conserved compared

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

100 n assembles into a trimer in three different crystal lattices, burying 1880 angstrom2 of accessible s

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

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

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

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

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

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

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

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

109 In the crystal lattice, capsid molecules assemble into continuo

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

111 s in the ciliate Tetrahymena thermophila are crystal lattices composed of multiple proteins.

112 A crystal lattice comprising uniformly staggered C5H5 ring

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

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

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

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

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

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

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

120 ed in the other subunit (subunit 2), because crystal lattice contacts lock it in an "open" conformati

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

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

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

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

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

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

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

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

129 The crystal lattice contains an unprecedented trimeric arran

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

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

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

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

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

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

136 otein may originate from crystal packing and crystal lattice disorder.

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

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

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

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

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

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

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

144 as nucleation sites for generating different crystal lattices for the two complexes.

145 Since the crystal lattice forces are fairly weak, it appears that

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

176 V endonuclease bound to 5'-CGGGATATCCC, in a crystal lattice isomorphous with the cocrystallized unde

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

233 In the crystal lattice, the interacting domains are contributed

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

262 main is rotated in the molecules of a second crystal lattice, which suggests a model of conformation-

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

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

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

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

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

268 gms that are needed for systematic design of crystal lattices with predictable structure and desirabl

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

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

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