ライフサイエンスコーパス: bilayer

1 and oligomeric states of proteins within the bilayer.

2 e numbers of phospholipids from the membrane bilayer.

3 e and after reconstitution into phospholipid bilayer.

4 ts direct contact with the peroxisomal lipid bilayer.

5 functional states within the membrane lipid bilayer.

6 energetics of an isolated side chain in the bilayer.

7 or IL-1beta transport across an intact lipid bilayer.

8 els' hydrophobic cores and that of the lipid bilayer.

9 ty of the TMD in bicelles that mimic a lipid bilayer.

10 iented single channels within the same lipid bilayer.

11 slocation of the transducer across the lipid bilayer.

12 teral diffusion of PI(4,5)P2 along the lipid bilayer.

13 to study vesicle fusion to a tethered lipid bilayer.

14 ities in thickness to a typical phospholipid bilayer.

15 all stability of the Env TMD trimer in lipid bilayer.

16 is connected to its neighbor through a lipid bilayer.

17 t pathway reconstituted on a supported lipid bilayer.

18 gral membrane proteins into the phospholipid bilayer.

19 surface, HZ induces a local thinning of the bilayer.

20 brane, HDL becomes integrated into the lipid bilayer.

21 o, and regulates transport across, the lipid bilayer.

22 een 80 as edge activators (EAs) in the lipid bilayer.

23 d one in which it penetrates deeply into the bilayer.

24 e extraction of biotinylated lipids from the bilayer.

25 in separate oligomers in the two-dimensional bilayer.

26 rotein function can be modulated by the host bilayer.

27 se from partitioning of anesthetics into the bilayer.

28 s form a pore that penetrates the cell lipid bilayer.

29 Oldenlandia affinis when embedded in a lipid bilayer.

30 , and the mechanical properties of the lipid bilayer.

31 namically propagate through biological lipid bilayers.

32 high-melting phospholipid in liquid-ordered bilayers.

33 assembly into mycolic acid-containing lipid bilayers.

34 that gA subunits can exchange between lipid bilayers.

35 bacteriorhodopsin molecules in native lipid bilayers.

36 nerated channels was studied in planar lipid bilayers.

37 ing values as large as 0.2 eV in the case of bilayers.

38 coated with one or several concentric lipid bilayers.

39 conformational dynamics within native lipid bilayers.

40 sor allylamine hydrochloride (AH) with lipid bilayers.

41 asure bound-cholesterol orientation in lipid bilayers.

42 mbrane domain of BamA is greatest in thicker bilayers.

43 ion that gA monomers do not exchange between bilayers.

44 A, a pH-gated bacterial channel, in membrane bilayers.

45 n packing order were detected in mixed-lipid bilayers.

46 yR1 channels reconstituted into planar lipid bilayers.

47 ompartments, and are usually formed by lipid bilayers.

48 nvolves the burial of side chains into lipid bilayers.

49 rticles smaller than 6 nm can embed in lipid bilayers.

50 envelope via insertion of nanopores into the bilayers.

51 in bilayer with magnetic field, which makes bilayer a promising platform for spin-valley quantum gat

52 In IrMn/FeCo bilayers, a structural phase transition in the IrMn laye

53 Thus, ubiquitin and the substrate lipid bilayer act synergistically to induce a conformational r

54 ns between the two leaflets of the supported bilayers affected SNARE-mediated fusion.

55 5)P2] precursor phosphatidylinositol between bilayers, allowing replenishment of PI(4,5)P2 hydrolyzed

56 A novel polypyrrole (PPy)-based bilayer amperometric glucose biosensor integrated with a

57 lating an entire mammal red blood cell lipid bilayer and cytoskeleton as modeled by multiple millions

58 mposition and physical state of the membrane bilayer and glucose transport activity via the glucose t

59 ition and brightening of the dark exciton in bilayer and monolayer WSe2, respectively.

60 ydrophobic surface on VP5* with the membrane bilayer and on a large-scale conformational change.

61 ned by combining a one-dimensional loss/gain bilayer and one or two thin polarization-converting comp

62 On the contrary, the presence of the bilayer and semi circled DDA on the MPA and cysteamine l

63 affected by the physical state of the lipid bilayer and specific lipid-protein interactions.

64 rate and co-substrate Na(+) across the lipid bilayer and the transport cycle, respectively.

65 e systematically studied with twist angle in bilayer and trilayer graphene sheets.

66 A mathematical equivalence between bilayers and curved monolayers simplifies the inverse pr

67 a structured region that inserts into lipid bilayers and disrupts their integrity.

68 e membranes leading to an indentation of the bilayers and increase in water permeation.

69 ified and unmodified tiles bind to gel-phase bilayers and produce arrays of new organized morphologie

70 a membrane SNARE-containing planar-supported bilayers and purified neuroendocrine dense core vesicles

71 dsorption of the molecular motors onto lipid bilayers and subsequent activation of the motors using u

72 Interactions between lipid bilayers and the membrane-proximal regions of membrane-a

73 Equilibrium structural properties of fluid bilayers and various thermodynamic quantities can then b

74 al organization of GPCRs within the membrane bilayer, and consequently can tune chemokine receptor si

75 ation, resolution into the mature epithelial bilayer, and lumen formation.

76 ive to membrane undulations, unlike in lipid bilayers, and it strongly affects both lipid-packing def

77 o crystal structures embedded in model lipid bilayers, and steered their transport domain toward thei

78 ely pattern domains of phase-separated lipid bilayers, and the patterning is also observed for four-a

79 At ambient temperature and in a lipid bilayer, Aqy1 adopts a closed conformation that is globa

80 ts suggest that supported fluid phospholipid bilayers are not homogenous at the nanoscale, but specif

81 We have created a 4 x 4 droplet bilayer array comprising light-activatable aqueous dropl

82 man splitting, however, persists in 2H-MoTe2 bilayers, as a result of an additional degree of freedom

83 e membrane protein reconstitution in a lipid bilayer at high concentrations.

84 site chiralities in a graphene electron-hole bilayer at moderate magnetic fields.

85 d heterogeneous deformations of the membrane bilayer at the surface of the protein, specific interact

86 lope, which can be modeled as a double lipid bilayer attached to a viscoelastic gel (lamina) whose el

87 Here, we present a droplet interface bilayer-based approach to quantify pep-1-mediated beta-g

88 phase diagram was constructed for the single bilayer binary lipid system.

89 The PPy-GOx/PPy-Cl bilayer biosensor was effective in rejecting 98% of asco

90 easure fusion of liposomes to a planar lipid bilayer (BLM).

91 hell around the channel in the dC16:1+dC24:1 bilayer, but no significant redistribution (50 +/- 4% dC

92 d mere building blocks of the membrane lipid bilayer, but the subsequent realization that phospholipi

93 indeed positioned close to the center of the bilayer, but, surprisingly, can exchange rapidly with wa

94 ctuations at the interfacial region of lipid bilayers by using a combination of ultrafast time-resolv

95 g helical states, the graphene electron-hole bilayer can be used to build new 1D systems incorporatin

96 uniquely, physical transformations of lipid bilayers can be monitored on a length scale of micromete

97 ow-melting phospholipid in liquid-disordered bilayers can be much stronger than the attractive forces

98 opy was used to determine the heights of the bilayer catalysts.

99 For the same channel thickness, the bilayer channels exhibit up to two orders of magnitude h

100 aded silicasome carrier that comprises lipid bilayer-coated mesoporous silica nanoparticles (MSNPs);

101 between dense-core particles, liquid-filled, bilayer-coated vesicles/liposomes, and gas-filled bubble

102 s of this setup include tight control of all bilayer components, which is compelling for the investig

103 ed the action of Aurein 1.2 in charged lipid bilayers composed of DMPC/DMPG.

104 position, to quantify the influence of lipid bilayer composition on protein-glycolipid binding in vit

105 mportant in producing a compact structure in bilayer conical, as well as pyramidal, MN, as confirmed

106 rane (OM) of Gram-negative is a unique lipid bilayer containing LPS in its outer leaflet.

107 the interaction of zetacyt with planar lipid bilayers containing mixtures of acidic and neutral lipid

108 Remarkably, bilayer CrI3 displays suppressed magnetization with a me

109 concentration of the planar-supported lipid bilayers, CTxB was (12 +/- 4)x more concentrated on the

110 the channel, which partially alleviates the bilayer deformation energy associated with channel forma

111 10-fold greater affinity than C461 for lipid bilayers, despite both solutes having similar hydrophobi

112 Steeper gradients caused lipid bilayer destabilization and pore instability, limiting t

113 ously cross synthetic lipid bilayers without bilayer disruption.

114 min (DNP-BSA) or mobile in a supported lipid bilayer (DNP-SLB).

115 ne and PIP2) to make PI3Kalpha competent for bilayer docking, as well as for subsequent binding and p

116 mentally observed noncrystalline cholesterol bilayer domain.

117 ors was enhanced by increasing the number of bilayers due to the increment of the enzyme surface cove

118 s for subnanomolar miRNA quantification with bilayer-embedded porins.

119 extracellular nanosized vesicles with lipid bilayers encapsulating nucleic acids and proteins, both

120 Microparticles are lipid bilayer-enclosed vesicles produced by cells under oxidat

121 scL channels are sensitive to changes in the bilayer environment and are, therefore, an ideal test ca

122 le with various techniques, and due to their bilayer environment and increased stability, they are of

123 site-specific measurements of allostery in a bilayer environment, and highlight the power of describi

124 aracterize MscL gating kinetics in different bilayer environments under the influence of alcohols.

125 s reveal that the VCMA of ultrathin FeRh/MgO bilayers exhibits distinct linear or nonlinear behavior

126 olic acids (MAs), which, in part, render the bilayer extremely hydrophobic and impermeable to externa

127 are co-entrapped on paper in a "wafer"-like bilayer film of polyelectrolytes (Poly (allyl amine hydr

128 n by analyzing the interfacial energy of two bilayer foam systems with varying liquid fractions.

129 As an example, the deformation of a membrane bilayer following the gel-to-fluid phase transition in a

130 gnetic labeling, and reconstitution in lipid bilayers) for both ssNMR and DEER.

131 A separate lipid bilayer formed at the interface between each droplet and

132 rted by protein nanopores spanning the lipid bilayer formed at the interface of the encapsulated aque

133 virus (HCV) p7 protein into supported lipid bilayers formed from physiologically relevant lipids (PO

134 dency to partition preferentially into lipid bilayers from aqueous solution.

135 ed within the lumen as a fragment upon lipid bilayer fusion.

136 The misorientation angle of the bilayer GBs is determined from a quantitative analysis o

137 n-orbit torques in a heavy metal/ferromagnet bilayer geometry, showing in general both field-like and

138 re, we report the observation of excitons in bilayer graphene (BLG) using photocurrent spectroscopy o

139 or spin quantum numbers.The phase diagram of bilayer graphene at high magnetic fields has been an out

140 The electronic band structure of twisted bilayer graphene develops van Hove singularities whose e

141 high magnetic field electronic structure of bilayer graphene is enhanced by the spin, valley isospin

142 raphene multilayer system as well as vHSs in bilayer graphene over a wide range of twist angles (from

143 In bilayer graphene, the resistance exhibits a monotonic de

144 acellular compartments surrounded by a lipid bilayer, have been recently shown to target the surface

145 The thermodynamic origins of these bilayer heights were investigated using molecular dynami

146 10), the peptide became perpendicular to the bilayer, however no pore was detected by neutron in-plan

147 viously we reported a whole protein water-to-bilayer hydrophobicity scale using the transmembrane bet

148 the important role of the surrounding lipid bilayer in the delicate conformational coupling of the i

149 tal evidence ruling out a role for the lipid bilayer in their ion channel effects.

150 enabled the formation of two adjoining lipid bilayers in a controlled manner, a requirement for the r

151 2-dioleoyl-sn-glycero-3-phosphocholine lipid bilayers in different saline solutions, that ions can lo

152 observed two binding modes of zetacyt to the bilayers in dynamic equilibrium: one in which zetacyt is

153 Mechanical properties of the lipid bilayer influence their neighbouring membrane proteins,

154 insert their apolar "wedge" domains into the bilayers, initiating the lipid rearrangements of fusion.

155 l membranes and upon landing on phospholipid bilayers instantaneously (seconds) convert into rapidly

156 ar dynamics simulations showed a stronger MA-bilayer interaction in the presence of Chol, and a large

157 properties and their alteration of the MscL-bilayer interface.

158 ilic peptides embedded near the polar/apolar bilayer interface.

159 dgroup region and solvated in the acyl chain bilayer interior, respectively.

160 SNARE-domain zippering draws the bilayers into immediate apposition and provides a platfo

161 um elastic model for gramicidin A in a lipid bilayer is shown to describe the sensitivity to thicknes

162 n vitro, we show that cholesterol within the bilayer is sufficient for constitutive Smoothened activa

163 ethanol's effect on vesicles fusing to lipid bilayers is not known.

164 ving unspecified interactions with the lipid bilayer known as the unitary lipid-based hypothesis of a

165 ion channel function result from changes in bilayer lateral pressure that arise from partitioning of

166 cattering to probe lipid distribution across bilayer leaflets in lipid vesicles.

167 istors based on Bi2O2Se crystals down to the bilayer limit exhibit high Hall mobility values (up to 4

168 (DMPC) and POPC/POPS 3:1 liposomes retain a bilayer macroscopic phase even at the highest peptide co

169 Molecular bilayers made by successive reduction of different diazo

170 on was present close to and inside the lipid bilayer magnetosome membrane.

171 nonvesicular lipid transport between the two bilayers mediated by lipid transfer proteins.

172 etic effects on ion channel function are not bilayer-mediated but rather involve direct protein inter

173 This includes the new paradigms emerging for bilayer-mediated channel mechanosensitivity and how this

174 The surfactant permeabilizes the lipid bilayer membrane to facilitate release of an encapsulate

175 olecular transducer from one side of a lipid bilayer membrane to the other.

176 e skeleton attachment to the fluidlike lipid bilayer membrane, including a specific accounting for th

177 structure and regulated deformation of lipid bilayer membranes are among a cell's most fascinating fe

178 Multicomponent lipid bilayer membranes display rich phase transition and asso

179 haracterizing thermodynamic phases of single bilayer membranes has not been possible due to their ext

180 proteins transduce information across lipid bilayer membranes in response to extra-cellular binding

181 plification of chemical signals across lipid bilayer membranes is of profound significance in many bi

182 reveals the transport of water across lipid bilayer membranes with a relative water permeability as

183 gulfs the forespore, surrounding it with two bilayer membranes.

184 re stages of phase separation in model lipid bilayer membranes.

185 stallization, as well as reconstitution into bilayer membranes.

186 -GTPase Ypt7 needed for SNARE-mediated lipid bilayer merger.

187 The asymmetric droplet interface bilayer method may be generally applicable for high-thro

188 s research work, we fabricated biodegradable bilayer MN arrays containing nano - microparticles for t

189 The height of bilayer MN arrays was influenced by the weight ratio of

190 tal porcine skin penetration of VD3 NMP from bilayer MN was quantitatively analysed after cryostatic

191 Using vesicles of various sizes as a lipid bilayer model, we show GTP-dependent membrane binding of

192 It also indicates that the lipid bilayer modulates channel gating, although it is not cle

193 found a reversible structural transition in bilayer monodisperse foams by changing the foam liquid f

194 surface energy of two ordered structures for bilayer monodisperse wet foams with arbitrary liquid fra

195 hotoluminescence and Raman spectra of a bare bilayer MoS2 (Molybdenum disulfide).

196 l angles change the electronic structures of bilayer MoS2 and produce two new symmetries in their ban

197 ifferent rotational angles in a freestanding bilayer MoS2 sheet as directly observed using an aberrat

198 w 60 mV dec(-1) at room temperature based on bilayer n-MoS2 and heavily doped p-germanium, etc.

199 , we demonstrate that a combination of lipid bilayer nanodiscs and a multiplexed silicon photonic ana

200 ecule measurements of F0F1 embedded in lipid bilayer nanodiscs, we observed that the ability of the F

201 rified NPC1 that was incorporated into lipid bilayer nanodiscs.

202 Steered simulations along the bilayer normal establish the metastable nature of the in

203 he C-terminal helical domain relative to the bilayer normal, includes the W41 primary gate for proton

204 Unlike monolayers, the Zeeman splitting in bilayers occurs without lifting valley degeneracy.

205 We found that the lipid bilayer of bicelles stabilized the chromophore-free opsi

206 , a hidden equilibrium phase in a hole-doped bilayer of Sn on Si(111).

207 se of the protein precursor within the lipid bilayer of the inner membrane, followed by cleavage by t

208 port of neutral doxorubicin across the lipid bilayer of the liposomes.

209 measurements of phase transitions in single bilayers of 1,2-dimyristoyl-sn-glycero-3-phosphocholine

210 etween pairs of 3 result in the formation of bilayers of 174 A in length.

211 that the Zeeman splitting still persists in bilayers of MoTe2 without lifting the valley degeneracy,

212 stered in the acyl moiety region between the bilayers of phospholipids, which results in ER-LD swelli

213 Self-assembled bilayers offer a promising strategy to directly harness

214 ic transmembrane cavity exposed to the lipid bilayer on the fungal scramblase nhTMEM16 serves as the

215 ylenimine (PEI) and poly(acrylic acid) (PAA) bilayers on a polydopamine-functionalized polysulfone su

216 ong acid and then reassembling fresh PEI-PAA bilayers on the membrane support.

217 ending modulus and fluidity of vesicle lipid bilayers on the micrometer scale, and distinguish betwee

218 ial growth of large-scale WSe2/SnS2 vertical bilayer p-n junctions on SiO2/Si substrates, with the la

219 n particular, the physical properties of the bilayer perovskite Sr3Ru2O7 at the surface are intimatel

220 approaches that include the supported lipid bilayer platform as well as DNA tension sensor technolog

221 PC vesicles to both sides of planar DC18:1PC bilayers preincubated with gA, which reduced channel act

222 We analyze the evolution of bilayer properties along this transition: domains of two

223 tune the 3D cubic phase nanostructure, lipid bilayer properties and the lipid mesophase is limited.

224 f the alcohol-induced changes to a number of bilayer properties and their alteration of the MscL-bila

225 general anesthetics have minimal effects on bilayer properties at clinically relevant concentrations

226 For Na,K-ATPase, bilayer properties can modulate pump activity, and, as o

227 None of the compounds tested altered bilayer properties sufficiently to produce meaningful ch

228 sthetics and related nonanesthetics on lipid bilayer properties using an established fluorescence ass

229 Protein crowding also affects bilayer properties, such as membrane undulations and ben

230 ay that senses drug-induced changes in lipid bilayer properties.

231 osite, yet complementary, influences on many bilayer properties.

232 for membrane binding rather than to trigger bilayer rearrangement.

233 that the peptide was on the surface of lipid bilayer regardless of the charged lipid ratio.

234 amage of the lipids, which then disrupts the bilayer, resulting in cell death.

235 d crystal structure of a two-tailed peptidic bilayer reveals similarities in thickness to a typical p

236 analysis of elastic deformations in a lipid bilayer shows that stiffer lipid domains tend to distrib

237 iotinylated surfaces such as supported lipid bilayers (SLBs) and self-assembled monolayers (SAMs).

238 shing adsorbed vesicles from supported lipid bilayers (SLBs) as well as profiling the extent of defor

239 electrostatic DNA binding to supported lipid bilayers (SLBs) presents an opportunity to build dynamic

240 resented based on the performance of organic bilayer solar cells and careful modeling.

241 t from closed-open transitions in long-lived bilayer-spanning dimers.

242 elix bundle appear to penetrate the membrane bilayer, stabilizing ExoU-membrane association.

243 top surface is carbonized to create a unique bilayer structure.

244 headgroups with minimal perturbation to the bilayer structure.

245 nanosheets (NS) of manganese oxide to form a bilayer structure.

246 usion measurements of VSG in supported lipid bilayers substantiate this possibility, as two freely di

247 es of lipid membranes, we could modulate the bilayer-substrate interaction and corresponding separati

248 catalytic effect on tOmpA folding in thicker bilayers, suggesting that BAM catalysis involves lowerin

249 ], incorporated into a phospholipid membrane bilayer supported on 3 mum silica microspheres.

250 In the orientation perpendicular to the bilayer surface, HZ induces a local thinning of the bila

251 arges of extramembrane domains and the lipid bilayer surface.

252 Nanodiscs that hold a lipid bilayer surrounded by a boundary of scaffold proteins ha

253 Given a well-controlled donor/acceptor bilayer system, we uncover the genuine effects of molecu

254 Sensing bilayer tension, MscL channels are sensitive to changes

255 s 25 +/- 5x higher in planar supported lipid bilayers than within nanoscale membrane curvature.

256 rformed in a solid-supported cushioned lipid bilayer that closely matched the chemical composition of

257 o nanovesicles or incorporation into a lipid bilayer that encapsulates mesoporous silica nanoparticle

258 ve bacterial outer membrane (OM) is a unique bilayer that forms an efficient permeation barrier to pr

259 we show that lipopolysaccharides (LPS) form bilayers that interact with PhiX174 at an icosahedral fi

260 Owing to the inversion symmetry in bilayers, the photoluminescence helicity should no longe

261 between each droplet and the hydrogel; each bilayer then incorporated bR.

262 tion (50 +/- 4% dC18:1) in the dC18:1+dC22:1 bilayer; these simulated values are within the 95% confi

263 proteins to move across hydrophobic membrane bilayers, they must be unfolded and translocated by a me

264 d, segregation of Pb to the surface of three bilayer thick PbSe-SnSe alloy layers was discovered with

265 el membranes, and computationally, to affect bilayer thickness and lipid phase separation, and subseq

266 ng the outward chain lateral pressure in the bilayer, through addition of lamellar phosphatidylethano

267 Overcoming the lipid bilayer to deliver RNA into cells has remained the major

268 cing various phase-separated lipid mono- and bilayers to the MACs.

269 Our Zn10 L15 prism thus inserts into lipid bilayers to turn on anion transport, which can then be t

270 y negatively charged S vacancy in monolayer, bilayer, trilayer and bulk MoS2.

271 ed by first dissembling the existing PEI-PAA bilayers using strong acid and then reassembling fresh P

272 olecular machines can drill through cellular bilayers using their molecular-scale actuation, specific

273 the possibility of peptide exchange between bilayers using three different types of experiments.

274 ositol bisphosphate (PIP2) -containing lipid bilayer, using coarse-grained molecular dynamics.

275 structural H2 O on Zn(2+) intercalation into bilayer V2 O5 .nH2 O is demonstrated.

276 ches the polar/apolar interface of the lipid bilayer very well.

277 Here we show that lipid bilayer vesicles (liposomes) can be triggered to release

278 LC linear mesh morphology is also present on bilayer vesicles in solution.

279 fically targeting phospholipids in the lipid bilayer via the production of singlet oxygen ((1)O2).

280 n in the amphiphilic headgroup region of the bilayer was supported by (15)N-NMR of uniformly labeled

281 While no segregation for single bilayers was observed, segregation of Pb to the surface

282 g vibration in hydrated phosphocholine lipid bilayers, we are able to measure a correlation function

283 erstand how it interacted with charged lipid bilayers, we employed Small Angle Neutron Scattering to

284 Two orientations of HZ molecule in the bilayer were found and characterized.

285 acting with a dimyristoylphosphatidylcholine bilayer were performed at the condition of low peptide-t

286 nd turret region, coupled to the surrounding bilayer, were actively involved in channel gating.

287 e lipid molecules within the otherwise fluid bilayer when the latter is supported.

288 ains two different stacking sequences in the bilayer, where the atomic structure of the stacking boun

289 abrupt change in the bending modulus of the bilayer which could be associated with the dissolution o

290 th large sidechains is immersed in the lipid bilayer, while the inner barrel surface is highly charge

291 embrane domain (TMD) forms a trimer in lipid bilayer whose structure has several peculiar features th

292 ical and cylindrical micelles, and stacks of bilayers, whose structures responded to atmospherically

293 outer membrane is a unique asymmetric lipid bilayer with lipopolysaccharide in the outer leaflet.

294 onstrate the control of degree of freedom in bilayer with magnetic field, which makes bilayer a promi

295 lane charge current simply by use of a FM/NM bilayer with magnetization collinear to the charge curre

296 rate constant for transport across the lipid bilayer with values in the range from 1 to 3x10(-12)cms(

297 allel beta-sheets that assemble into stacked bilayers with alternating hydrophobic and polar interfac

298 nological synapses formed on supported lipid bilayers with laterally mobile ICAM-1 and anti-CD3 mAb.

299 We simulate model lipid bilayers with the MARTINI coarse-grained force field on

300 des that spontaneously cross synthetic lipid bilayers without bilayer disruption.