ライフサイエンスコーパス: crystal

1 dy yields 50% ferrous iron in a heme protein crystal.

2 ear with the amount of mass deposited on the crystal.

3 iferromagnetic chain along the a-axis of the crystal.

4 and the Kerr nonlinearity of the constituent crystal.

5 limited due to challenges in obtaining thin crystals.

6 ergy barriers separating different states in crystals.

7 sion from solution, resulting in fluorescent crystals.

8 assembly and nanosegregation of these liquid crystals.

9 rocycle and coronene form selectively two co-crystals.

10 of the twinning nucleation mechanism in HCP crystals.

11 both CH(3)NH(3)PbI(3) thin films and single crystals.

12 while retaining useful properties of perfect crystals.

13 r structure of benzamide form II needle-like crystals.

14 Administration of SCFAs reduced renal crystals.

15 nsition metal oxides(1,2), layered molecular crystals(3) and trapped-ion arrays(4) are a few examples

16 fractions that range from generalized Wigner crystals(7) to charge density waves.

17 c crystal growth theory is used to show that crystals accelerated from an initial growth rate of 10(-

18 In the un-doped crystal all iron ions, sitting in five different crystal

19 es of a uniaxial antiferromagnetic Cr(2)O(3) crystal and a heavy metal (Pt or Ta in its beta phase).

20 d electron microscopy measurements of single-crystal and bicrystal gold microscale devices.

21 chemical shielding calculations of Li-P-O/N crystals and ab initio molecular dynamics-generated amor

22 que, we harvest some centimeter-sized single crystals and achieved high device performance.

23 ily fabricated from single vapor-phase grown crystals and exhibit reversible 8-fold changes in conduc

24 are well dispersed on the surface of the MOF crystals and have a narrow size distribution.

25 n the films both in the form of longitudinal crystals and microglobules.

26 tory cytokines, oxidized lipids, cholesterol crystals and other factors.

27 ctance measurements were performed on single crystals and thin films, and theoretical predictions wer

28 ed fats in SFF of powders with large lactose crystals and vice-versa.

29 ide particles, dispersed in a nematic liquid crystal, and contained within a microfluidic channel.

30 cterizing the chiroptical properties of bulk crystals, and also due to the difficulty in separating (

31 elucidating the phase transition from gel to crystal are highly important for the development of vari

32 Some crystals are suitable for screening for entry-blocking i

33 After cell death, these crystals are trapped into sediments that remove iron fro

34 that the fast-mode frequency increases with crystal area as expected for an edge supercurrent.

35 y was the analysis of the characteristics of crystal arrangement in different corneal layers and the

36 This review summarises the use of CaCO(3) crystals as versatile carriers to host, protect and rele

37 atoms substitute molybdenum sites in MoS(2) crystals, as confirmed by transmission electron microsco

38 along (110) crystallographic plane of the Li crystals because of the fine in-plane lattice matching b

39 Near the critical drive, time crystal behavior emerges, in which the period of the lim

40 axial crystal growth enlarged the perovskite crystals by 10-fold with a reduced defect density and st

41 ccessfully embedded into the channels of the crystals by diffusion from solution, resulting in fluore

42 alculations, the selenium vacancy in ReSe(2) crystal can enhance its electroactivity for both NRR and

43 Laser irradiation of the molecular crystal can generate phase-dependent transient elastic l

44 h demonstrates that the handedness of chiral crystals can be used to control the sign of their Chern

45 in devices are overcome, adaptive molecular crystals can have far-reaching implications for emerging

46 Advantageously, upon activation the crystals can undergo guest exchange in a single-crystal-

47 inclusions (CCaI) either as calcium oxalate crystals (CaOx) or amorphous calcium carbonate cystolith

48 analyses of the dated units characterize the crystal cargo, and Advanced-InSAR analysis highlights ac

49 elength volume of a single, silicon photonic crystal cavity.

50 ymph gland: plasmatocytes, lamellocytes, and crystal cells, which are analogous to vertebrate myeloid

51 stigate bulk mosaicity within as-cast single crystal CMSX-4 and CMSX-10 Ni-base superalloys.

52 Ferroelectric domain walls in single-crystal complex oxide thin films are found to be orders

53 To date, binary crystals composed of spherically symmetric particles at

54 protein-MOFs) as chemically designed protein crystals, composed of ferritin nodes that predictably as

55 The quadrangle-shaped co-crystal constitutes a unique material that exhibits two-

56 able concentrations through the use of mixed crystals containing the secondary 1,4-phenylene pillar.

57 ) to 1-10 m day(-1)), indicating meter sized crystals could have formed within days, if these rates a

58 Crystal defects called <c> loops, routinely seen no smal

59 Typically, ion migration for crystal deformation or connection with other nanocrystal

60 Mean crystal density of the anterior and posterior stroma of

61 progressive kidney disease, characterized by crystal deposits, tubular injury, inflammation, and fibr

62 terms of change in CCCS, IVCM score, corneal crystal depth, and photophobia score; however, local adv

63 ring heterogeneous and transient flow of fat crystal dispersion demonstrated that local constitutive

64 erimental geometry resembling that of liquid crystal displays.

65 tifreeze proteins restrict the growth of ice crystals during recrystallization and therefore find app

66 Liquid crystal elastomers (LCEs) are an attractive platform for

67 CO molecules at well-defined Pt(hkl) single-crystal electrode surfaces is a key step towards address

68 y in separating (sub)micrometer-scale chiral crystal enantiomers.

69 so the opportunities one can exploit using a crystal engineering approach, for example, the design of

70 acceptor substrate binding obtained using a crystal engineering approach.

71 tions will be of particular relevance to the crystal engineering community, whose goal is the design

72 ase the scope of possibilities for colloidal crystal engineering with DNA.

73 in tissue-like phantoms beyond the phononic crystal evanescent zone and Fresnel zone of the emitter.

74 ecular mechanics (QM/MM) calculations of the crystals evidence the crucial role of specific asymmetri

75 also induced by the differential affinity of crystal facets to water molecules in the first solvation

76 ilica has grown on highly conductive Si(110) crystal facets, the silica-silicon conversion becomes re

77 heses of NiO particles exposing a variety of crystal facets.

78 es which are highly sensitive to bonding and crystal field environments.

79 that two of these design principles are weak crystal fields and the presence of structural distortion

80 thick two-dimensional layered semiconducting crystals for reliable vertical diodes showing excellent

81 de-bridge and domain-swapped interfaces from crystal formation in Bti to dissolution in the larval mo

82 Magnetic crystals formed by 2D layers interacting by weak van der

83 stic monopoles to a zoo of unusual colloidal crystals formed by high-order multipoles like hexadecapo

84 evealed key differences in the nature of DOX crystals formed inside LTSLs based on the loading buffer

85 ages atomic/molecular configurations in thin crystals from charge density projections, and uncovers t

86 defy the intuitively simple idea of forming crystals from oppositely charged partners, instead formi

87 UA crystal granulomas surrounded by proinflammatory M1-like

88 ssible new model for biological control over crystal growth during amelogenesis, and hint at implicat

89 The slow heteroepitaxial crystal growth enlarged the perovskite crystals by 10-fo

90 matin inhibitors is not reflected in current crystal growth models.

91 Synergism between two crystal growth modifiers is expected, but the antagonist

92 Directed crystal growth on designer substrates has the potential

93 hat we can predict the activation energy for crystal growth rates, including activation energies sign

94 Kinetic crystal growth theory is used to show that crystals acce

95 utilized extrinsic doping techniques or bulk crystal growth, detrimentally affecting uniformity, scal

96 ould add new fundamentals to the insights of crystal growths of nanocrystals and would also help in o

97 ve description of wrinkle patterns as liquid crystals [H.

98 The results reveal that the crystals have an unusually large semigap of ~16 eV and a

99 Crystals having orientational and periodic translation s

100 ble approach to producing wafer-scale single-crystal hBN paves the way to future 2D electronics.

101 The obtained single-crystal hBN, incorporated as an interface layer between

102 l materials from layered van der Waals (vdW) crystals hold great promise for electronic, optoelectron

103 h-and-transfer method for fabricating single-crystal hybrid perovskites on arbitrary substrates, with

104 us on polycrystalline materials(5-7), single-crystal hybrid perovskites show improved carrier transpo

105 out, with the additional benefit of improved crystal identification.

106 a sputtered thin film Ag cathode on a Ge ATR crystal in CO(2)-saturated 0.1 M KHCO(3) over a range of

107 fraction from cellulose and epicuticular wax crystals in cell walls.

108 asymptomatic hyperuricemia or uric acid (UA) crystals in CKD progression are unknown.

109 discussion of the prospects of beyond 2D TMD crystals in optoelectronics, catalysis, and quantum info

110 caused by buildup of monosodium urate (MSU) crystals in the joints.

111 Here we form ionic colloidal crystals in water through an approach that we refer to a

112 Medium-sized crystals induced a particular reparative process that we

113 volved in the pathogenesis of other types of crystal-induced nephropathies.

114 oparticle occlusion in natural and synthetic crystals is a topic of wide-ranging interest owing to it

115 The high quality of the PdSe(2) crystals is confirmed by low-frequency Raman spectroscop

116 end-on bonding of the N(2) unit in the same crystal, [K(crypt)](2){[(R(2)N)(3)Gd](2)[mu-eta(x):eta(x

117 ctic silverfish[Pleuragramma antarctica] and crystal krill[Euphausia chrystallorophias]) responses to

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

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

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

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

122 rt a facile method to disassemble vdW single crystals layer by layer into monolayers with near-unity

123 We demonstrate the growth of single-crystal layers of hexagonal boron nitride (BN) and molyb

124 Liquid crystals (LCs) are omnipresent in living matter, whose c

125 high-quality, electrically insulating single crystals, leading to anomalous transport properties well

126 results in the formation of gel-like or even crystal-like structures in the bacterial plasma membrane

127 ility was confirmed by formation of formazan crystals, live-dead staining and caspase-3 activity assa

128 nd their spatial distribution in the zeolite crystal may have a significant effect on the product sel

129 ques including CV and electrochemical quartz crystal microbalance (EQCM) in sulfuric acid and phospha

130 Here, a time-resolved quartz crystal microbalance with dissipation monitoring (QCM-D)

131 ate label-free immunosensing, using a quartz crystal microbalance with dissipation monitoring (QCM-D)

132 cular-beam epitaxy (MBE), a series of single crystal Mn(x) Fe(3-) (x) O(4) thin films with controlled

133 Addition of UBA I seed crystals modified this pathway such that only UBA I was

134 throughput techniques for exfoliating single-crystal monolayers with sufficient size and high quality

135 cation conditions on the variation in single crystal mosaicity was investigated.

136 developed late in this process of chronic UA crystal nephropathy and contributed to the progression o

137 mouse model of hyperuricemia and chronic UA crystal nephropathy with granulomatous nephritis.

138 the cathodic corrosion of a spherical single crystal of platinum in an aqueous alkaline electrolyte,

139 cted photochemical intermediate trapped in a crystal of the hIDO1-CO-Trp complex, where CO is photoly

140 The well-formed habit of large crystals of challacolloite indicates slow growth from so

141 ermoelectric performance in the rhombohedral crystals of GeSe, which is stabilized at ambient conditi

142 Two-dimensional colloidal crystals of submicrometer microspheres provide a conveni

143 tride (BN) and molybdenum disulfide (MoS(2)) crystals on single-walled carbon nanotubes (SWCNTs).

144 on, there was no accumulation of cholesterol crystals or signs of toxicity.

145 through the promotion of PCET by tuning the crystal orientation and correlated proton diffusion.

146 The dense crystal packing of CQDs in the layered fashion suppresse

147 Here, we show that the chiral crystal palladium gallium (PdGa) displays multifold band

148 Semiconductor III-V photonic crystal (PC) laser is regarded as a promising ultra-comp

149 gies which have been designed to achieve the crystal phase control in TMDs, and the chemical mechanis

150 erned by a competition between two different crystal phases with free energies that depend on the cry

151 We explore and discuss the liquid crystal photonics in the prototype that has a novel opti

152 spatial mappings over large areas of single crystal platelets demonstrate the co-existence of both f

153 use of these features, magnetosome magnetite crystals possess specific properties in comparison to ab

154 lm growth while maintaining epitaxy and high crystal quality.

155 In physical crystals, regardless of the initial distribution of defe

156 ting-point depression in deformed or damaged crystals relative to their pristine counterparts.

157 Atom probe tomography of these crystals revealed the presence of heterogeneous spatial

158 DFT analysis of Y6 crystals reveals hole/electron reorganization energies o

159 4155 m s(-1), comparable to GaAs, but single crystals show very low lattice thermal conductivity of a

160 Upon laser exposure, MOF crystals shrank while metal oxide nanoparticles formed g

161 We achieve this stress by bending single-crystal silicon microbeams using an in situ thermomechan

162 tallic glass is established by analyzing the crystal size distribution using x-ray diffraction, trans

163 cavities slightly larger than the unit cell crystal size of MHs (1.2 nm), as exemplified in the expe

164 phases with free energies that depend on the crystal size.

165 eld and with dimensions limited only by bulk crystal sizes.

166 photoreduction of six different heme protein crystal species by X-ray radiation.

167 X-ray co-crystal structure analysis and ultracentrifugation exper

168 Crystal structure analysis of 1 shows a strong pai...pai

169 e X-ray analysis (EDX) elemental mapping and crystal structure analysis via SAED.

170 Due to the complexity of the crystal structure composed of heavy elements, the report

171 ing colloidal particles in the cubic diamond crystal structure could potentially be used to make mate

172 allization methods to understand and explore crystal structure in pharmaceuticals and minimize the ri

173 s further corroborated by obtaining an X-ray crystal structure of a derivative.

174 Here, we report the crystal structure of a posttermination Thermus thermophi

175 The X-ray co-crystal structure of an early lead (12) revealed a poten

176 The crystal structure of an EZH2-EED binary complex indicate

177 We present a crystal structure of BchL in the nucleotide-free form wh

178 Biochemical studies and the co-crystal structure of CLK1 in complex with AB1 show that

179 We solve the crystal structure of CxD7L1 in complex with ADP to 1.97

180 Here, we present the crystal structure of GP38, which revealed a novel fold w

181 osphoprotein is tetrameric, and we solve the crystal structure of its tetramerization domain.

182 Here, we present the crystal structure of M(1)AChR in complex with MT7, a sub

183 Determination of the co-crystal structure of M-808 in complex with menin provide

184 The first crystal structure of mammalian ER Glu I will constitute

185 We first report the crystal structure of mouse DHX36 bound to ADP.

186 We determined the X-ray crystal structure of N2, combined with monitoring secret

187 The crystal structure of olmesartan-bound human AT1R (PDB:4Z

188 Here, we report the crystal structure of PDE5 complexed with the sole second

189 Therefore, we determine the crystal structure of Sulfolobus acidocaldarius soluble F

190 Furthermore, the crystal structure of the amino analogue reveals an inter

191 We previously determined the X-ray crystal structure of the bacterial RNA polymerase engage

192 We report a crystal structure of the bifunctional FEN/EXO-POL apoenz

193 ct of ATP through a 2.5- angstrom-resolution crystal structure of the BRAF(KD)-14-3-3 complex, in whi

194 We previously defined and solved the crystal structure of the C-terminal domain of NP (NP-Ct)

195 The 1.38 angstrom crystal structure of the CypA/PreNAC complex displays a

196 Here, we report a crystal structure of the DNA-binding domain of a model A

197 The crystal structure of the ERK7-AC9 complex reveals that A

198 Here, we present the crystal structure of the Escherichia coli Hfq Core bound

199 Here we present the first crystal structure of the extracellular domains of human

200 A 2.1 angstrom X-ray crystal structure of the FigC N-citrylornithine decarbox

201 We determined the crystal structure of the HA protein of the avian H7N9 in

202 icular HCV-infected individuals, we solved a crystal structure of the HCV E2 ectodomain in complex wi

203 Here we present the 1.9- angstrom crystal structure of the human PD-1H extracellular domai

204 Here, we present the crystal structure of the LRP6 E1E2-SOST complex with two

205 A 3.0- angstrom crystal structure of the LRR-RK GSO1/SGN3 regulating Cas

206 nd not just histones, we have determined the crystal structure of the LSD1/CoREST complex bound to a

207 Here, we report the crystal structure of the prototypical SEDS protein RodA

208 Here, we report the crystal structure of the Reduced Potassium Dependency3/H

209 In this study, we describe the crystal structure of the RSV surface glycoprotein G in c

210 The 1.65- angstrom resolution X-ray crystal structure of YaaA reveals that the protein posse

211 We combine state-of-the-art computational crystal structure prediction (CSP) techniques with a wid

212 The crystal structure revealed an EF domain with two Ca(2+)-

213 We present an LRH-1 crystal structure that illuminates striking mechanistic

214 The fabricated silver nanorods show single-crystal structure with a low resistivity of 8.58 x 10(-5

215 We report the synthesis, X-ray crystal structure, and molecular recognition properties

216 th of the charge carriers and is affected by crystal structure, scattering from boundaries and defect

217 In this paper we report the synthesis, crystal structure, spectroscopic properties and redox in

218 e core/P1 domains than suggested in the SurA crystal structure.

219 gages in extended H-bond interactions in its crystal structure.

220 erated from synthetic NaCl solutions and the crystal structures and morphologies of manganese oxides,

221 hesized 12 manganese oxides having different crystal structures and particle sizes and measured the p

222 e mSAA1 at pH~7.4 agreed in details with the crystal structures but also showed important differences

223 JH2, and JH2 V617F domains, as well as five crystal structures for JH2 complexes.

224 though ultra-high-resolution opioid receptor crystal structures have revealed a specific Na(+) bindin

225 The crystal structures of (Ss)RidA-1 and (Ss)RidA-2 provided

226 Models generated based on crystal structures of 5' and 3' exonuclease oligonucleot

227 Here, Travis et al. report two crystal structures of a yeast tethering factor, the Dsl1

228 The crystal structures of AaTPS and FgGS provide insights in

229 Partial or complete crystal structures of all MSC constituents have been rep

230 Crystal structures of arsenic-bound p53 mutants reveal a

231 anism for this activity based on a series of crystal structures of bound complexes.

232 Crystal structures of Ca(2+)-free and Ca(2+)-bound EhAct

233 ROESY and DFT studies, aided by crystal structures of carboxylic acids bound by the cata

234 Although the crystal structures of dark- and light-adapted states hav

235 Crystal structures of delta revealed novel pentameric fo

236 Here, we present the crystal structures of four functionally distinct plant A

237 Crystal structures of GPCRs provide snapshots of their i

238 Crystal structures of human and mouse SCD1 were reported

239 sm of substrate cleavage, we have solved the crystal structures of human GGT1 (hGGT1) with glutathion

240 and inhibitory mechanism, we report 11 x-ray crystal structures of human VKOR and pufferfish VKOR-lik

241 High-resolution crystal structures of inactive MCR lacking the modified

242 The crystal structures of mammalian DXO with 3'-FADP or CoA

243 Here we report X-ray crystal structures of MEK bound to the scaffold KSR (kin

244 We present the first crystal structures of NRAS and KRAS ITD at 1.65-1.75 ang

245 By comparing crystal structures of paralogous complexes, we provide a

246 tilizing an ionic liquid strategy, we report crystal structures of salts of free anionic nucleobases

247 Here, we report crystal structures of substrate mimetic bearing ACPs in

248 Here, we present crystal structures of Teneurin-Latrophilin complexes tha

249 Crystal structures of tetrameric PfISN1 reveal complex r

250 forms that inhibit seeding differently, and crystal structures of the M204-scFv monomer, dimer, and

251 We have solved the crystal structures of the NTD core and EXO domains of Nb

252 Crystal structures of TrtA in apo and holo form were sol

253 Here, we describe the crystal structures of two distinct isoforms of ligand-fr

254 X-ray crystal structures of variously modified ASL(Arg1)(ICG)

255 mprehensive X-ray crystallographic study (12 crystal structures), involving both CA II and a soluble

256 ent of the RNAP active center that, based on crystal structures, has been proposed to cycle between a

257 Together with previous ultrahigh-resolution crystal structures, these findings enable us to follow t

258 tantially different from the organization in crystal structures, which feature flat hexamers.

259 Studies using single crystals suggest a polycrystalline surface should displa

260 lming accumulation of adsorbed dimers on the crystal surface, where it is complemented by dimerizatio

261 imeter and most of the deep traps located at crystal surfaces.

262 erties of n-type Te-doped Mg(3) Sb(2) single crystals, synthesized by a combination of Sb-flux method

263 This orientational ordering of cellulose crystals, termed texturing in materials science, represe

264 The chiral aspect of inorganic crystals that crystallize in chiral space groups has bee

265 Defect-free crystals that exhibit the glassy trend of low thermal co

266 ials and methods provide access to colloidal crystals that incorporate particles with the well-establ

267 iday junction sequence allowed us to produce crystals that provided unprecedented atomic detail.

268 This is the first example of molecular crystals that show complex oscillatory behavior under co

269 2) surfaces (either nanostructured or single-crystal TiO(2)(110)) was found to be highly dependent on

270 stals can undergo guest exchange in a single-crystal-to-single-crystal transformation generating a se

271 guest exchange in a single-crystal-to-single-crystal transformation generating a series of isoskeleta

272 ed hematite (1102) surface was studied using crystal truncation rod (CTR) X-ray diffraction coupled w

273 ter-sized layered [Formula: see text] single crystals under high oxygen pressures of 120-150 bar by t

274 The trap densities in single crystals varied by five orders of magnitude, with a lowe

275 eport a photobactericidal polymer containing crystal violet (CV) and thiolated gold nanocluster ([Au(

276 Resazurin and crystal violet assays indicated that 8a decreases triple

277 n these developments, the adaptive molecular crystals warrant particular attention as an alternative

278 coupling into a six-way crossing of photonic crystal waveguides.

279 ene with the top and/or bottom boron nitride crystals), we observe prominent and robust hysteretic be

280 Some hexagonal crystals were observed in two subjects.

281 A Pt/Beta crystal with no observable internal interfaces can be 18

282 er extrinsic mechanisms, we find that liquid crystals with high anchoring strengths can ensure smooth

283 metals that freeze into face-centered cubic crystals with little to no activation energy, are discus

284 dition characterized by formation of 2,8-DHA crystals within renal tubules.

285 orms the structure and dimensionality of TMD crystals without lithography.

286 Single-crystal X-ray analyses on MOF-1 showed that Cu(+2) ion w

287 In addition, single-crystal X-ray analysis was used to elucidate the structu

288 o product types was corroborated by a single-crystal X-ray analysis.

289 Single crystal X-ray crystallography showed that in some cases,

290 oscopically and, in many cases, using single-crystal X-ray crystallography.

291 scopic techniques in conjunction with single-crystal X-ray diffraction analysis.

292 recently reported SrB(3) C(3) ,([1]) single-crystal X-ray diffraction and computational modelling in

293 ce group I4 2m was solved by means of single crystal X-ray diffraction as a 6-component twin due to p

294 icene 1(2-) has been characterized by single-crystal X-ray diffraction as a solvent-separated ion tri

295 Single-crystal X-ray diffraction reveals that Y6 molecules cofa

296 Herein, based on results of in situ single-crystal X-ray diffraction studies up to 27 GPa, we repor

297 A combination of single-crystal X-ray diffraction studies, solution and solid-st

298 exes (1 and 2) was substantiated with single crystal X-ray diffraction study.

299 and (13)C NMR spectrometry as well as single-crystal X-ray diffraction.

300 Single-crystal X-ray structures of Re[Cl(8)TpCF(3)PC](O), Re[Cl