ライフサイエンスコーパス: crystal

1 the c-axis orientation in the center of the crystal.

2 roven phononic crystal design, the snowflake crystal.

3 ared to standard inorganic 0.5 mm thick ZnTe crystal.

4 clusters; the second is a unique porous CdSe crystal.

5 ty at the interface of beads with the liquid crystal.

6 ed by surface deposition on a blank photonic crystal.

7 which can be realized as a defect in liquid crystals.

8 lined for the design of hand-twisted helical crystals.

9 trolled deformation and patterning of liquid crystals.

10 h relies on the availability of high quality crystals.

11 erfere with each other and create artificial crystals.

12 ither as a supramolecular hydrogel or single crystals.

13 ks through the pyrolysis of nanosized ZIF-67 crystals.

14 where the chains are mostly trans within the crystals.

15 nal orientation fields in cholesteric liquid crystals.

16 ic constants in representative van der Waals crystals.

17 k single crystals and 12% for the microscale crystals.

18 e uniform motion of baby skyrmions in liquid crystals.

19 molecular orientation widely found in liquid crystals.

20 ation pressure is maintained inside photonic crystals.

21 e text], the more uniform, with systems like crystals achieving the maximum value: [Formula: see text

22 ling prevented the induced expression of the crystal adhesion molecules, CD44 and annexin II, in tubu

23 ange order over hundreds of microns of these crystals allows them to readily exfoliate into fibers.

24 orphous blue phase III of cholesteric liquid crystals, also known as the "blue fog," are among the ri

25 choline-binding protein ChoX, as revealed by crystal and density functional theory (DFT)-optimized st

26 In the RAS wt populations of CRYSTAL and FIRE-3, patients with left-sided tumors had

27 Here, we describe crystal and nuclear magnetic resonance structures of Kai

28 anced photoluminescence from the 2D photonic crystal and the 1D nanocavities.

29 ies of approximately 20% for the bulk single crystals and 12% for the microscale crystals.

30 Larger individual ice crystals and no entrapment in control ice creams was obs

31 tivating structures such as monosodium urate crystals and zymosan was not affected by BCD.

32 f porous materials for nucleation of protein crystals, and will be useful for optimal design of such

33 approach based on combining the phase field crystal approach with classical molecular dynamics simul

34 on a tripod and revealed that the two XB co-crystals are isomorphous, with slightly different C-X...

35 The 1D elastic crystals are next modified to two-dimensional (2D) elast

36 arise from the comparison of structures in a crystal as opposed to a membrane environment.

37 urges in methylammonium lead iodide (MAPbI3) crystals as a response to environmental basicity.

38 using different types of metal oxide single crystals as reference systems.

39 ered states, including 'defective by design' crystals, as well as amorphous phases such as glasses an

40 s plant tissues through the formation of ice crystals at or below freezing temperatures.

41 ctivity materials among unexplored inorganic crystals beyond caged and layered structures.

42 or preparation of stable, macroscopic single-crystal blue-phase materials.

43 for the formation of micrometer-scale single-crystal body-centered cubic gold nanoparticle superlatti

44 ces, especially on well-defined metal single crystals but also on other flat substrates such as highl

45 s on methods available for organic molecular crystals, but mention is made wherever techniques are su

46 Phononic crystals can control the propagation of SAW, analogous t

47 (MOFs): following a single-crystal to single-crystal cation metathesis, the Ca(2+) counterions of a p

48 molybdenum ditelluride on a silicon photonic-crystal cavity.

49 Cholesterol crystals (CC) are abundant in atherosclerotic plaques an

50 ssible layer combinations are limited by the crystal chemistries of the available anions.

51 e-transitive nets are of prime importance in crystal chemistry and are regarded as ideal blueprints f

52 Nine crystal complexes were determined.

53 eveal monomeric spikes similar to one of the crystal conformations.

54 ior is also demonstrated on other MV(2+)/BU6 crystals containing either BF4(-) or Br(-) counterions.

55 The crystal cross-sections possessed a symmetric, smooth lat

56 ozen water content, formation of amylopectin crystals, crumb hardening).

57 Crystal defects generated during irradiation can result

58 e, and correlate chemical order/disorder and crystal defects with material properties at the single-a

59 existing and experimentally proven phononic crystal design, the snowflake crystal.

60 In this paper, we present a photonic crystal device which performs both tasks simultaneously

61 ic-resolution scanning TEM (STEM) and single-crystal diffraction using synchrotron radiation.

62 built-in laser target projection and liquid crystal display shutters for alternate occlusion of the

63 ed field-effect transistors based on Bi2O2Se crystals down to the bilayer limit exhibit high Hall mob

64 und that the energy density generated in the crystals during depolarization in the high voltage mode

65 ted with the growing DNA strands and Mg2 PPi crystals during the rolling circle process, ultimately l

66 he propagation of SAW, analogous to photonic crystals, enabling components such as waveguides and cav

67 of controlling plastic flow in non-metallic crystals, enabling materials with a greater oxidation re

68 een developed using the design principles of crystal engineering and structure-property correlations,

69 under topochemical control to produce single-crystal extended solids.

70 tructures obtained from XFEL data mostly use crystals far larger than 1 mum(3) in volume, whereas the

71 The transformation between BPs, where crystal features arise in the submicron regime, is found

72 designed and fabricated air-silica photonic crystal fiber (PCF).

73 d physical investigations, microscale single-crystal fiber field-effect transistors were also fabrica

74 Ln ions by the highly designable 2D material crystal field provides a new method to extend their opti

75 ifold as a general consequence of a trigonal crystal field, and as such can be expected across a larg

76 nterface and results in a CYP126A1 monomeric crystal form.

77 Enamel crystals form de novo in a rich extracellular environmen

78 ry strategy based on a supramolecular liquid crystal formed by peptide amphiphiles (PAs) that encapsu

79 ulti-microsecond MD simulations of different crystal forms of ubiquitin.

80 In both crystal forms the protein is in complex with cholesterol

81 Crystal growers accomplish this by creating materials ai

82 rent crystal systems, attempts to understand crystal growth in detail have so far relied on developin

83 gantic molecules formed by self-assembly and crystal growth is challenging as it combines two conting

84 e is widely applicable and is not limited to crystal growth processes.

85 rystal lattice leads to predictably modified crystal habits.

86 The growth of T. gondii aldolase crystals in acidic conditions enabled trapping of the te

87 ive became 50-300 nm, near-spherical, single crystals in the exhaust.

88 5 nm aggregates consisting of 5-7 nm faceted crystals in the fuel additive became 50-300 nm, near-sph

89 annel inhibitor (SK&F96365) also reduced MSU crystal-induced NET release.

90 the first time to reconstruct the air-liquid crystal interface of a nematic material, namely, 4-penty

91 ze two-dimensional molecular charge transfer crystals into arbitrarily and vertically stacked heteros

92 terlayer ferromagnetism observed in the bulk crystal is restored.

93 [Formula: see text] plane of underdoped YBCO crystals is measured by means of a local optical techniq

94 An effective method to form crystals is to introduce nucleation-inducing heterologou

95 ons, we have studied the behaviour of single-crystal La2-xSrxCuO4 films through which an electrical c

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

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

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

99 A multi-layer liquid crystal (LC) spatial light modulator offers a large phas

100 nt wavelength of 800 nm in 0.26 mm thick HMB crystal leads to one order of magnitude higher THz wave

101 patterns medium-range order is detected with crystal-like motifs based on the B2 CuZr structure and i

102 lucidate the delithiation dynamics of single-crystal lithium iron phosphate microrods with long-axis

103 The resistivity of our beta-GeSe crystals measured in-plane is on the order of rho approx

104 ace plasmonic resonance (LSPR) into a quartz crystal microbalance (QCM) for studying biochemical surf

105 ne (DPPC) phospholipid mixtures using quartz crystal microbalance-based nanoviscosity measurements.

106 protein (heavy meromyosin, HMM) using quartz crystal microbalance; and motor bioactivity with ATPase

107 hispering gallery microcavities and photonic crystal microcavities, both of which have been developin

108 wed for rapid prototyping and testing of new crystal mounting designs, with a resin cost of 0.2 cent

109 in concentration inside pores, which enables crystal nucleation even under conditions where heterogen

110 zation measurements of a high quality single crystal of Cr1/3NbS2 over three magnetic field regions.

111 es on an atomic level, we investigate single crystals of CH3NH3PbI3 with a narrow transition ( 5 K) n

112 olutions of the salts afforded X-ray quality crystals of five compounds with hydroxyl groups forming

113 Following this line, we show here that crystals of membrane proteins display systematically hig

114 The single crystals of tetragonal structure are easy to cleave into

115 Crystals of the CRD in complex with a mammalian-type hig

116 Here we show that single crystals of thiolate-protected clusters can be grown in

117 overcome these challenges and obtain single crystals of three zirconium phosphonates that are suitab

118 the difficulty in obtaining well-diffracting crystals of transient and heterogeneous noncovalent prot

119 Here we show that single crystals of uranium dioxide subjected to strong magnetic

120 ext modified to two-dimensional (2D) elastic crystals, of the type 4-bromophenyl 4'-nitrobenzoate whe

121 uildup of radiation damage in ion-irradiated crystals often depends on the spatial distribution of at

122 red crystalline film exfoliated from In2 Se3 crystals on a graphene bottom electrode, it is shown tha

123 rvations of deposition growth of aligned ice crystals on feldspar, an atmospherically important compo

124 ompound undergoes a single-crystal-to-single-crystal one-electron reduction to give (Cp2Co)1.43(Me2NH

125 For example, few single-crystal organic monomers react under topochemical contro

126 dy of the cracking behavior as a function of crystal orientation in a laser 3D-printed DL125L Ni-base

127 t the induced monoclinic phase preserves the crystal orientation of the original hexagonal phase.

128 Here we probe how the crystal packing alters microsecond dynamics, using solid

129 le 7 and hypothesized that disruption of the crystal packing would improve solubility, which led to a

130 mitting InGaAsP/InP two-dimensional photonic crystal (PC) Bragg laser with triangular lattice.

131 Since crystal plasticity varies systematically with imposed co

132 re broadly observed on partially delithiated crystals, providing direct evidence for a concurrent nuc

133 nough to grow a thick AlN template with high crystal quality and very few threading dislocations, all

134 ng superconducting band gaps in the dominant crystal regions, which lead to both higher overall T c a

135 Exploiting the properties of two-dimensional crystals requires a mass production method able to produ

136 s scars, pleats, folds, blisters, and liquid crystal ripples.

137 Using a crystal scanning approach, we determine the high-resolut

138 bservations allow us to understand how ZIF-8 crystals self-assemble and the subsequent influence of i

139 arising from the interface region of single-crystal semi-insulating GaAs that has been coated and pa

140 on propagation distance based on crystalline crystal silver at low temperature.

141 cific applications include controlling their crystal size and shape.

142 relation between the increased percentage of crystal size and the concentration of SDF.

143 e amount of intracellular ice as well as ice crystal size played a role in determining whether or not

144 s were performed on URu2 - x Fe x Si2 single-crystal specimens in high magnetic fields up to 45 T (DC

145 novel and takes place for relatively higher crystal stability reasons.

146 e low-temperature incommensurately modulated crystal structure (for Sm2Ru3Ge5 as a representative) ha

147 ermophilum RIOK-2 protein kinase (Ct-RIOK-2) crystal structure 4GYG as a template.

148 etic and orbital degrees of freedom with the crystal structure across the MIT in rare-earth nickelate

149 Co-crystal structure analysis revealed a dual active site-d

150 Crystal structure analysis revealed that FePYR1 recogniz

151 razing incident X-ray diffraction to observe crystal structure and chemical transition of perovskites

152 A recent crystal structure and in vitro experiments highlighted p

153 range of applications owing to their unique crystal structure and optoelectronic properties.

154 Both the high-temperature average crystal structure and the low-temperature incommensurate

155 The crystal structure at 1.9 A resolution deciphered that S1

156 The crystal structure at 2.19 A resolution shows a large dis

157 terin synthase association pathways and near-crystal structure complexes from protein-protein associa

158 A crystal structure is reported for 3.DQ(PF6)2.

159 s described and rationalized using the X-ray crystal structure of 6 bound to human IDO-1, which shows

160 250-550, we report here the 2.3A resolution crystal structure of a complex containing Sac3 residues

161 ...H-C interaction was observed in the X-ray crystal structure of a fluorinated triterpenoid.

162 This first crystal structure of a monocot CAD combined with enzyme

163 We determined a 2.76 A-resolution crystal structure of a mycobacterial transcription initi

164 Here, we present the crystal structure of a prokaryotic TMEM175 channel from

165 Here, the authors present the crystal structure of a Pseudomonas MDC and give insights

166 We report a 3.4-A resolution X-ray crystal structure of a sigma(N) fragment in complex with

167 Here, we have solved the X-ray crystal structure of an EBNA1 DNA-binding domain (DBD) a

168 We recently published the crystal structure of an unusual (S)P species [(MeAN)2Cu(

169 The crystal structure of Bacillus subtilis NrnA reveals a dy

170 We determined a crystal structure of CaM bound to a peptide encompassing

171 A crystal structure of CYP2C9 in complex with a TCA1 analo

172 The NhaA crystal structure of Escherichia coli has become the par

173 We illustrate how the crystal structure of Fe14 Pd17 Al69 provides an example

174 part in Streptomyces griseus We obtained the crystal structure of FNO in complex with NADP(+) at 1.8

175 The crystal structure of GLIC shows R-ketamine bound to an e

176 Here we describe the crystal structure of GS-5745.MMP9 complex and biochemica

177 Here, we report the crystal structure of hRSV NS1 protein, which suggests th

178 Here, we report the crystal structure of human XPNPEP3 with bound apstatin p

179 Here we report the crystal structure of kinesin-6 Zen4 in a nucleotide-free

180 We investigated the small molecule crystal structure of lead molecule 7 and hypothesized th

181 A third crystal structure of LmFBPase complexed with its alloste

182 using sulfur-SAD phasing, we determined the crystal structure of m4-1BB to 2.2-A resolution.

183 Here we report the 2.7-A X-ray crystal structure of MazF-mt6.

184 Here we report the crystal structure of MyRF DBD.

185 The crystal structure of NCS-1 bound to FD44 and the structu

186 Here, we report the first crystal structure of ObgE at 1.85-A resolution in the GD

187 Here, we report the crystal structure of one of the allergens from Blo t, re

188 tallization properties, we obtained a 2.24-A crystal structure of pig-tailed macaque APOBEC3H with bo

189 Here, we describe the crystal structure of PRL-1 in complex with the Bateman m

190 We present here the X-ray crystal structure of the ADAM10 ectodomain, which, toget

191 on cross-linking-coupled mass spectrometry, crystal structure of the CPSF160-WDR33 subcomplex and bi

192 Here, we report the 2.25 A resolution crystal structure of the GAPDH1 holoenzyme in a quaterna

193 Here, we describe the crystal structure of the Gn glycoprotein ectodomain from

194 We report the crystal structure of the human Chk1 KA1 domain, demonstr

195 By solving the crystal structure of the IL-1alpha/aptamer, we provide a

196 linking data were compared directly with the crystal structure of the isolated N-terminal extracellul

197 The crystal structure of the leptospiral PerR revealed an as

198 The crystal structure of the metal-ion dependent esterase MG

199 A crystal structure of the mitochondrial Hsp90, TRAP1, rev

200 Here, we report the crystal structure of the MOB1/NDR2 complex and define ke

201 Here, we determined the crystal structure of the N-terminal half of a conserved

202 Here we report the crystal structure of the N-terminal IMS domain of Toc75

203 A crystal structure of the p107 CTD bound to E2F5 and its

204 ed at the interface between protomers in the crystal structure of the PCNA-K20ac ring.

205 We have determined the crystal structure of the PPARgamma ligand-binding domain

206 Here the authors present the crystal structure of the retinoic acid receptor beta-ret

207 Here, we present the crystal structure of the SNX5-PX:IncE complex, showing I

208 e panel and allowed us to obtain an X-ray co-crystal structure of the synthetic secondary metabolite

209 We present a comprehensive study of the crystal structure of the thin-film, ferromagnetic topolo

210 Here we present the crystal structure of the trimeric, prefusion ectodomain

211 The crystal structure of this ANbP in complex with human HGP

212 The crystal structure of this inactivated assembly provides

213 We solved the crystal structure of UbV.7.2 and rationalized the molecu

214 Its crystal structure revealed the self-assembly of two Pt-c

215 The Axl crystal structure revealed two distinct conformational s

216 The crystal structure shows that the hydrogen bonding intera

217 y a templated clipping reaction and an X-ray crystal structure shows that the squaraine gem-dimethyl

218 ghly organized capsules is shown by an X-ray crystal structure which features the assembly of two XB

219 on to form MV(+*) radical cations within the crystal structure with half-lives of several hours in ai

220 The combination of our crystal structure with solution state analysis of recomb

221 solving the high-resolution channelrhodopsin crystal structure, and by structural model-guided redesi

222 Based on its crystal structure, the RNA polymerase domain contains tw

223 A new crystal structure, together with molecular dynamics and

224 ther, by comparing solution binding data and crystal structure, we gained insight on how the probe se

225 ent accessibility-related parameters both by crystal structure-based calculations of solvent-accessib

226 deprotonated closely resembles the available crystal structure.

227 Dirac cone for the ideal, perfectly ordered crystal structure.

228 r with no permanent voids or channels in its crystal structure.

229 this stabilization with an atomic resolution crystal structure.

230 nodes are a consequence of the orthorhombic crystal structure.

231 Crystal structures and accompanying solution data confir

232 The crystal structures and mass spectrometry also show that

233 Here we report crystal structures at up to 2.6 A resolution of the yeas

234 ypeptides has remained challenging, with few crystal structures available to show their overall struc

235 Crystal structures of affimers bound to their cognate ch

236 Crystal structures of alphaIIbbeta3 and alphaVbeta3 have

237 We determined crystal structures of an anaerobically prepared fragment

238 The crystal structures of apo PllA and complexes with three

239 Crystal structures of AspRedAm in complex with NADP(H) a

240 Here, we report crystal structures of B. multivorans HpnN, revealing a d

241 High-resolution crystal structures of CARM1 in complex with these compou

242 In this paper, we describe the crystal structures of CCT5 and the CCT5-H147R mutant, wh

243 The crystal structures of CusB, CusC, CusF, and the CusBA co

244 Previous crystal structures of cytochrome P450cam complexed with

245 Crystal structures of enzymes are indispensable to under

246 This questions whether the available x-ray crystal structures of EPOR truly represent active or ina

247 om Arabidopsis thaliana We observed that the crystal structures of free, Mg(2+)-bound, and berylloflu

248 Here, we report the crystal structures of full length Escherichia coli RapZ

249 n and propagation of dislocations within the crystal structures of HOIPs and IP.

250 Two crystal structures of Japanin, an 18 kDa immune-modulato

251 Crystal structures of P- and E-selectin suggest a two-st

252 We report six crystal structures of Pfs25 in complex with antibodies e

253 Here, we report the crystal structures of PopP2, a YopJ effector produced by

254 High-resolution crystal structures of reconstructed homodimeric receptor

255 Crystal structures of the BAF component BAF45C indicate

256 ction, and ligand recognition, we determined crystal structures of the D4 dopamine receptor in its in

257 Crystal structures of the large terminase nuclease from

258 Crystal structures of the muPA:nanobody complexes and hy

259 Here we solve the crystal structures of the N-terminal domains of PHF1 and

260 re we present the syntheses, activities, and crystal structures of the p53-MDM2/MDMX inhibitors based

261 n, we present two additional high-resolution crystal structures of the same RNA duplex containing fou

262 Furthermore, we present the crystal structures of the Seb1 CTD- and RNA-binding modu

263 Here, we present the crystal structures of the SHR-SCR binary and JACKDAW (JK

264 We also determined crystal structures of these compounds bound to PARP1 or

265 mined electron cryo-microscopy (cryo-EM) and crystal structures of unbound and H1-bound nucleosomes a

266 Crystal structures showed that pT1471 binds the canonica

267 X-ray crystal structures were obtained for five of the designs

268 ssess different melting points, NMR spectra, crystal structures, and stacking patterns in the solid s

269 n intermediates agree well with the relevant crystal structures, validating the computational protoco

270 Using the recently resolved hCB1 receptor crystal structures, we also performed a modeling study t

271 ie2 dimers in solution and modeling based on crystal structures, we suggest that Ang1 binding may cro

272 leaving only a small number of protein-ssNA crystal structures, while forcing solution investigation

273 itions and predicting compositions for known crystal structures, with notable successes.

274 easured distances were compared to available crystal structures.

275 s, and so enables the determination of their crystal structures.

276 espectively, possibly due to their different crystal structures.

277 A crystal superlattice structure featuring nonlinear layer

278 The mean dissolution rate of the (000-1) crystal surface is more than 4 times that of the (10-10)

279 e of the complexity and variety of different crystal systems, attempts to understand crystal growth i

280 mperature in optimally cobalt-doped BaFe2As2 crystal (T c = 23 to 25 K) by precipitating-out the coba

281 proves Neel-ordering temperature in BaFe2As2 crystal (T N = 132 K to 136 K) by improving in-plane ele

282 Our method utilizes double-layer colloidal crystal templates in conjunction with site-specific elec

283 usion coefficients in natural olivine single crystals that were determined at upper mantle conditions

284 The crystals then continue to grow to develop morphologies c

285 The synthesis of bulk crystals, thin films and nanostructures plays a seminal

286 rganic frameworks (MOFs): following a single-crystal to single-crystal cation metathesis, the Ca(2+)

287 on of Cp2Co, the compound undergoes a single-crystal-to-single-crystal one-electron reduction to give

288 of Te(4+) is reduced and emitted from the M1 crystals under catalytic operating conditions, without c

289 e retrieval algorithms for imaging defective crystals using BCDI.

290 A 66% spin polarization of the BZA single crystal was obtained by Andreev reflection spectroscopy

291 Intriguingly, the crystals we observe do not readily form in previously va

292 Dimers formed when crystals were grown in the presence of the non-cyclizabl

293 Preformed poly(ethylene oxide) (PEO) single crystals were used as the template to direct the crystal

294 and fabricate frequency tailorable phononic crystals with an order-of-magnitude increase in attenuat

295 o the emergence of lipid bicontinuous single crystals with unprecedented swelling capacity.

296 characterized by multinuclear NMR and single-crystal X-ray diffraction analysis.

297 Single-crystal X-ray diffraction confirmed structures that rese

298 aman spectroscopy and low-temperature single-crystal X-ray diffraction, and in the gas phase by quant

299 field (57)Fe Mossbauer, magnetometry, single crystal X-ray diffraction, XAS, and EXAFS for 6.

300 Knowledge of their single-crystal X-ray structures has been instrumental to enable