ライフサイエンスコーパス: repulsive

1 net interaction between these two lipids is repulsive.

2 heir interactions are neither attractive nor repulsive.

3 is engineered to be resonantly enhanced and repulsive.

4 the interactions among the atoms are purely repulsive.

5 develop even for cues that have always been repulsive.

6 e interactions between K10 chains are purely repulsive.

7 lit complexes so that signaling is no longer repulsive.

8 t makes one association pleasant and another repulsive?

9 in the central nervous system, exerting its repulsive activity by binding the Neogenin receptor.

10 into the adjacent cortical territories by a repulsive activity mediated by EphB/ephrinB signaling.

11 de exchange factor Trio strongly enhance the repulsive activity of all three intracellular domains, s

12 sensory neurons insensitive to the outgrowth repulsive activity of skin-derived Versican.

13 eins DSH-1 and MIG-5 redundantly mediate the repulsive activity of the Wnt signals to induce anterior

14 Robo1 and Robo2 receptors and mediates Slit repulsive activity, as well as a C-terminal fragment (Sl

15 repulsive actuators, a 19-element two-layer repulsive actuated deformable mirror is operated in pseu

16 allel-plate actuators and these two types of repulsive actuators, a 19-element two-layer repulsive ac

17 the advantages of two-layer and three-layer repulsive actuators, i.e., fabrication requirements and

18 olic numerosity perception, giving rise to a repulsive aftereffect: motion to the left adapts small n

19 l guidance factors with structurally encoded repulsive and adhesive surfaces.

20 7, although AH and BSA respectively undergo repulsive and attractive electrostatic interactions at t

21 ore complex and is likely influenced by both repulsive and attractive electrostatic interactions.

22 ed behavior is a result of interplay between repulsive and attractive forces within positively charge

23 We give evidence for the existence of both repulsive and attractive interactions between pi systems

24 esidues showed that these residues made both repulsive and attractive interactions with protease that

25 amide ligands in positions that satisfy both repulsive and attractive ion-ion interactions.

26 species in solutions, which changes between repulsive and attractive on changing the electrodes' mag

27 ts a layered structure with both significant repulsive and attractive regions, with the magnitude of

28 ributed to a competition between short-range repulsive and long-range attractive vortex-vortex intera

29 f filler network formation using attractive, repulsive and non-interacting potentials were processed

30 e topological properties of these materials, repulsive and quantized Casimir interactions become poss

31 is ligand, the intermolecular interaction is repulsive and supramolecular patterns are not observed.

32 d hydrodynamic as well as nonspecific strong repulsive and weak attractive interactions.

33 e that the integrated actions of attractive, repulsive, and adhesive molecules direct eve-dependent d

34 t low temperatures that become progressively repulsive as temperature is increased.

35 ween the force probe and the surface must be repulsive at very short distances (<5 nm) and attractive

36 substances (CSS), range and magnitude of the repulsive-attractive intersurface forces, and geometry o

37 an in vivo link between semaphorin-mediated repulsive axon guidance and alteration of intracellular

38 A neurons showed that overexpression of this repulsive axon guidance and cell patterning cue models t

39 elopment, netrin-1 is both an attractive and repulsive axon guidance cue and mediates its attractive

40 we have shown that semaphorin3A (Sema3A), a repulsive axon guidance molecule, localizes to the PNNs

41 Myelin-associated molecules, repulsive axon guidance molecules, and extracellular mat

42 -actin disassembly, cellular remodeling, and repulsive axon guidance.

43 trol gene strongly suppress Sema-1a-mediated repulsive axon guidance.

44 e of rapid dissociation, consistent with the repulsive B (1)A' potential along the O-O coordinate com

45 Our data show a weak repulsive barrier before proteins aggregate reversibly,

46 gnalings respectively mediate attractive and repulsive behavior in behavioral plasticity in locusts.

47 in simultaneously recorded neurons predicted repulsive biases that are consistent with the direction

48 In contrast to the paradigm that repulsive bidirectional signaling drives cell segregatio

49 The nanoconfinement of normally repulsive bipyridinium units results in the enforced pi-

50 AMPA stimulation was neither attractive nor repulsive but clearly increased the migration rate of wi

51 ed colloids can be varied from attractive to repulsive by optically introducing dislocation kinks.

52 cumbrance in -BTzOR-Ar- dyads by eliminating repulsive C-H...H-C interactions with neighboring arene

53 ever, results from theory and simulation for repulsive cavities appear to be inconsistent with recent

54 s (E(b)) and enhance reaction rates, whereas repulsive Cbeta(delta(-))...X(delta(-)) interactions inc

55 Based on this, repulsive charge interactions are engineered into the bu

56 nd above 200 mM NaCl where the electrostatic repulsive charge was at a minimum.

57 spersion, some migratory cells are guided by repulsive collisions with their neighbors.

58 ex vivo, SlitC binding to PlexinA1 elicits a repulsive commissural response.

59 n barrier and contrast this to the case of a repulsive condensate, in both cases finding excellent ag

60 nt to Al2O3 under globally electrostatically repulsive conditions.

61 own appears to be stabilization--relative to repulsive confinement--of the unfolded state through bin

62 ontribution of a pathogenic mutation and the repulsive contribution of the EC domain.

63 bind to the negatively charged DNA, reducing repulsive Coulomb forces between nucleotides and allowin

64 BPQT(4+) host-guest interactions to overcome repulsive Coulombic interactions between the cationic M1

65 that the polo-like kinase PLK-1 mediates the repulsive coupling between MEX-5 and POS-1 by increasing

66 Normally, Sema3d provides a repulsive cue to endothelial cells in this area, establi

67 on of multiple, and in some cases redundant, repulsive cues from various tissues is critical to patte

68 ymerization in neuronal growth cones whereas repulsive cues induce actin disassembly.

69 e midline, and then are thought to switch to repulsive cues to grow away on the opposite side.

70 tion of long- and short-range attractive and repulsive cues.

71 tens of minutes, and which are attractive or repulsive, depending on the surface chemistry of the sus

72 ction disassembly, which suggests an overall repulsive effect between cells.

73 regated morphologies due to the increasingly repulsive effective interactions between the blend compo

74 tractive soluble growth factor gradients and repulsive effects arising from cell-cell contact, termed

75 y of two parallel H-bonds avoiding secondary repulsive effects contributes to the high-affinity bindi

76 withdrawing ammonium group and charge-charge repulsive effects in the transition state.

77 athway amplifies the F-actin disassembly and repulsive effects of a growth-preventing pathway.

78 Furthermore, the repulsive effects of prenol were maintained when co-pres

79 The strong, on-site, repulsive electron-electron interactions that are the pr

80 r when Cooper pair formation is dominated by repulsive electron-electron interactions, so that the sy

81 ligand-imposed Pt-Pt distance accompanied by repulsive electronic congestion.

82 is the result of its ability to diminish the repulsive electronic interactions originating from the a

83 Here we evaluate the interplay between repulsive electrostatic (Fel) and attractive van der Waa

84 e capsid, neighboring DNA strands experience repulsive electrostatic and hydration forces as well as

85 en the change in brine composition induces a repulsive electrostatic force between the oil-brine and

86 f the CTA(+) covered Au NPs and decrease the repulsive electrostatic forces among NPs, leading to ass

87 Ps, which are governed by the competition of repulsive electrostatic forces and attractive poor solve

88 on the nanotube surfaces, thereby increasing repulsive electrostatic forces and steric effects.

89 presence of attractive depletion forces and repulsive electrostatic forces assemble into equilibrium

90 roles of attractive base stacking forces and repulsive electrostatic forces creating this stiffness.

91 Stability was compromised by repulsive electrostatic forces originating from clusteri

92 sand compared to clean sand is likely due to repulsive electrosteric forces between the PVP coatings

93 or repulsive Netrin-1 signals together with repulsive ephrin signals.

94 ed in which a balance between attractive and repulsive exosite interactions in the native state is sh

95 We suggest that calibration of the repulsive exponent in the LJ potential widens the range

96 ided by a concerted action of attractive and repulsive factors to reach their target.

97 istically, radial migration is controlled by repulsive FLRT2-Unc5D interactions, while spatial organi

98 ent, likely due to the reduced electrostatic repulsive force and presence of the additional methyl gr

99 reover, we show that tuning the range of the repulsive force below the particle roughness suppresses

100 ere we introduce the natural phenomenon of a repulsive force between cells of different types.

101 nteraction, by controlling the van der Waals repulsive force between Cesium Rydberg atoms located ins

102 Repulsive force between the O-H bonding electrons and th

103 s outside of the connector channel, a strong repulsive force from the viral protein would be generate

104 ines are held apart at the intersection by a repulsive force generated by the Frank elasticity.Discli

105 If the repulsive force is sufficiently high, shift becomes a st

106 PE-DOTAP-AuNP (DDA) whereas they enhance the repulsive force on the Cyst and AUT monolayers.

107 ordering on the water, resulting in a strong repulsive force over some tens of nanometers with superp

108 an atomic force microscope (AFM), whereas a repulsive force was detected for the interaction between

109 bly because of the tension generated by this repulsive force.

110 l metastable and make swelling possible when repulsive forces among the capsid proteins become large

111 ult of the competition between electrostatic repulsive forces and attractive molecular interactions.

112 Under high compression, stronger repulsive forces appear due to the strong compression of

113 0 due to the greater amount of electrostatic repulsive forces between droplets present at pH 7.0.

114 ion above an onset stress needed to overcome repulsive forces between particles.

115 ymer coatings are frequently used to provide repulsive forces between surfaces in solution.

116 d how the balance between the attractive and repulsive forces defines the equilibrium docked state we

117 lative proportion of attractive, neutral and repulsive forces defines types of potentials, that induc

118 rparts, likely because of an increase in the repulsive forces due to their higher negative charge den

119 n which rotation is powered by Van der Waals repulsive forces during the final 85 degrees of rotation

120 en the two systems allows us to decouple the repulsive forces from the attractive hybridization inter

121 ysicochemical balance between attractive and repulsive forces fully explains grana stacking.

122 ilayer interactions are usually prevented by repulsive forces generated by the glycocalyx, a dense an

123 the importance of long-ranged electrostatic repulsive forces on thin-film stability.

124 s provide strong support for the notion that repulsive forces play a major role in the formation of l

125 Then repulsive forces provided by the actin system are necess

126 each solute particle is engineered to impose repulsive forces strong enough to overpower van der Waal

127 inning of the confined fluid and the osmotic repulsive forces that dominate the overall (dynamic and

128 he subtle balance between the attractive and repulsive forces that drives the stimuli-induced self-as

129 that serves as a decoy for C, and secondly, repulsive forces with a key active site residue prevent

130 wide spacing results from a balance between repulsive forces, due to Tau's projection domain (PD), a

131 of the components interact mechanically via repulsive forces, occurring as the bacterial cells grow

132 ds and demonstrate a validated model for the repulsive forces, proposing that this universal behavior

133 usly increasing intermolecular electrostatic repulsive forces.

134 Remarkably little attention has been paid to repulsive forces.

135 tional bias influenced by the attractive (or repulsive) forces resulting from congestion, accessibili

136 ate the reflection of a solitary wave from a repulsive Gaussian barrier and contrast this to the case

137 growth cone movements in both attractive and repulsive gradients in a microfluidic device.

138 We propose that Wnt5 acts as a repulsive guidance cue for the PN dendrites, whereas Drl

139 larization in part through the liberation of repulsive guidance cue semaphorin 3A (Sema3A).

140 Contrary to this model, we find that the repulsive guidance cue Slit stimulates the formation and

141 axon, we discovered that the beam acts as a repulsive guidance cue.

142 es to semaphorin 3F and Eph receptor B2, two repulsive guidance cues crucial for AC development, was

143 tion and growth cone collapse in response to repulsive guidance cues.

144 The repulsive guidance effect was significantly reduced when

145 We show that osteoclasts express the repulsive guidance factor Semaphorin 4D and induce conta

146 The repulsive guidance ligand ephrin-A3 is expressed only on

147 We propose that while repulsive guidance mechanisms contribute to lumen format

148 molog neogenin functions in both netrin- and repulsive guidance molecule (RGM)-mediated axon guidance

149 Repulsive guidance molecule A (RGMa) is a potent neurite

150 minimally deleted region including only the repulsive guidance molecule B (RGMB) and chromodomain he

151 D-L2), a known ligand of PD-1, also binds to repulsive guidance molecule b (RGMb), which was original

152 Repulsive guidance molecule family members (RGMs) contro

153 Repulsive guidance molecule member a (RGMa) is a membran

154 We previously showed that repulsive guidance molecule member a (RGMa) is upregulat

155 Lrig2 binds Neogenin, a receptor for repulsive guidance molecules (RGMs), and prevents premat

156 BD) and (2) a kinase-dependent inhibition of repulsive guidance pathways that does not require the Ab

157 urons, PKC activation has been implicated in repulsive guidance responses and inhibition of axon rege

158 mical switch that controls Semaphorin/Plexin repulsive guidance.

159 rotein that was initially characterized as a repulsive-guidance cue.

160 In contrast, the repulsive hydration and undulation interactions differed

161 hich is attributed to the presence of strong repulsive hydration forces due to the highly hydrophilic

162 s, with the latter commonly considered to be repulsive in nature.

163 irect result of such charge-transfer-induced repulsive interaction between cationic gold and positive

164 the charged particle surface resulting in a repulsive interaction between the particles.

165 rmation giving rise to a weak and long-range repulsive interaction force between the surfaces.

166 NT clusters by suppressing the electrostatic repulsive interaction from the oxidized surfaces.

167 The attenuation of the 1,3-syn-diaxial repulsive interaction indicates that TBDPS has stereoele

168 Even though a strong repulsive interaction is expected for both MAbs due to t

169 Conversely, MAb2 displays a repulsive interaction potential throughout the concentra

170 For softer repulsive interaction potentials, these two transitions

171 setups, we derive a strong photon long-range repulsive interaction, by controlling the van der Waals

172 tum phases induced by this photon long-range repulsive interaction.

173 peroxide solutions show that attractive and repulsive interactions arise from the catalytically gene

174 lt indicates that bulkier counterions screen repulsive interactions at the ligand/solvent interface m

175 Here, we show that repulsive interactions between an exchangeable mimic of

176 on a delicate balance between attractive and repulsive interactions between biomolecular building blo

177 Both repulsive interactions between cell and EPSs and the ove

178 ity, supporting models that account for both repulsive interactions between DNA strands and local var

179 Coulomb drag is a process whereby the repulsive interactions between electrons in spatially se

180 ty of the map is determined by attractive or repulsive interactions between molecular tags that are d

181 ) insertion, a novel divalent metal relieves repulsive interactions between the adducted guanine base

182 nd dimethylformamide) are crucial to provide repulsive interactions between the charged outlying ioni

183 te binding site(s) on the kinase but also by repulsive interactions between the kinase and nonpermiss

184 ely packaged DNA strands, as a result of the repulsive interactions between the negative charges on t

185 ; that is, emulsion drops with attractive or repulsive interactions can be generated by changing the

186 in the dispersion interaction are masked by repulsive interactions even at displacements significant

187 tural features within the glycoligand reduce repulsive interactions for the Cu(I) state.

188 ssume positions in which they face the least repulsive interactions from other cells and the embryo's

189 ntified almost a decade ago, yet the role of repulsive interactions in guiding structure formation is

190 ion and describe how combined attractive and repulsive interactions influence the shape and size of t

191 We present evidence that fiber type-specific repulsive interactions inhibit innervation of slow myofi

192 st, the contributions from electrostatic and repulsive interactions nearly cancel out due to solvent

193 ollapse into a sharp peak is at odd with the repulsive interactions of polaritons and their positive

194 The effects of repulsive interactions on DNA interaxial distance were p

195 ); such differences appear to reflect weaker repulsive interactions on the curved surfaces prevalent

196 ley locking in hole-doped TMDs together with repulsive interactions selectively favours two topologic

197 accounts for a combination of attractive and repulsive interactions simultaneously, and results in an

198 n be rationalized in terms of attractive and repulsive interactions with the d-band, such that inert

199 rophobically modified silica, which exhibits repulsive interactions with the PEI, freeing up binding

200 In the achiral regime, the cusp defects have repulsive interactions, but away from this limit we meas

201 mulations using pairwise additive long-range repulsive interactions, demonstrating the ability to con

202 , which are believed to be formed locally by repulsive interactions, may prevail.

203 For strong repulsive interactions, we observed two-dimensional Mott

204 clusions in membranes can acquire long-range repulsive interactions, which might more generally have

205 s, for dynamic arrest in systems with purely repulsive interactions.

206 rane osmometry under conditions dominated by repulsive interactions.

207 s, and Stoner's itinerant ferromagnetism for repulsive interactions.

208 stable rafts exhibiting chiral structure and repulsive interactions.

209 uggests that the observed trend is driven by repulsive interactions.

210 n the molecules is dominated by the onset of repulsive interactions.

211 mbly by tuning the balance of attractive and repulsive intermolecular forces.

212 els demonstrate that balanced attractive and repulsive interparticle interactions dictated by the lig

213 Furthermore, coalescence is promoted by repulsive latex and silica particles but inhibited by at

214 ucts of accumulated pleasure memories-even a repulsive learned cue for unpleasantness can become sudd

215 cine-rich transmembrane protein 2 (FLRT2), a repulsive ligand of the UNC5 receptor family for neurons

216 Semaphorin 3F, a repulsive ligand to Nrp2, regulates both migration of Nr

217 xon guidance molecules, including Slits, the repulsive ligands for roundabout (Robo) receptors, and N

218 cell adhesion molecules and as heterophilic repulsive ligands of Unc5/Netrin receptors.

219 Thus, our study uncovers a local repulsive mechanism required for self-avoidance and demo

220 the ability to switch between attractive and repulsive migration in response to extracellular guidanc

221 thin tissues and elicits both attractive and repulsive migratory responses.

222 Dscams and Pcdhgs, in self-recognition, but repulsive molecular mechanisms remain obscure.

223 masses of the antihydrogen do not rule out a repulsive nature for the antimatter gravity.

224 over perversions during their formation, the repulsive nature of the perversion-perversion interactio

225 itons in trains are created with effectively repulsive nearest-neighbor interactions or rather evolve

226 synergistically integrate both attractive or repulsive Netrin-1 signals together with repulsive ephri

227 C. elegans responds to a repulsive odorant by first backing up and then either co

228 ional imaging disclosed a LH region tuned to repulsive odors comprised exclusively of third-order neu

229 actions causes intrachain interactions to be repulsive, on average.

230 fer whether protein-protein interactions are repulsive or attractive, resulting in solutions that are

231 The weak interactions can be repulsive or attractive, thus enhancing or diminishing t

232 A pseudo-three-layer electrostatic repulsive out-of-plane actuator is proposed.

233 ieved by an approximation of the short-range repulsive part of the interaction, combined with nonaffi

234 that fragility reflects the strength of the repulsive part of the interatomic potential, which can b

235 In contrast to repulsive particles at zero temperature, we argue that t

236 structure, each receptor couples to a common repulsive pathway.

237 s; and (iii) competition between short-range repulsive (pi...pi) interactions and long-range attracti

238 k(on) could be attributed to the presence of repulsive polymers that mimic the glycocalyx, which poin

239 it is shown that the phase diagram of a soft repulsive potential leads to the morphological diversity

240 tructure calculations typically use a simple repulsive potential that neglects the effects of solvati

241 , we show that stronger liquids have steeper repulsive potentials.

242 g of the vesicle lysis tension and hydration repulsive pressure that combine to enhance fusion.

243 These potentials usually are highly repulsive, producing cavity-bound hydrated electrons tha

244 te binding of proteins to the ligands due to repulsive protein-protein and protein-ligand steric inte

245 "anchor" and create attractive "pulling" or repulsive "pushing" interactions.

246 from the rods' chirality lead to long-range repulsive raft-raft interactions.

247 ncoupling of polymerized TUBB3 with netrin-1-repulsive receptor UNC5C is involved in netrin-1-mediate

248 Given the number and variety of different repulsive receptors, it is generally thought that there

249 Given the number and variety of different repulsive receptors, it is generally thought that there

250 erms of the signaling pathway(s) used by the repulsive receptors, mutations in the guanine nucleotide

251 llular domains of three different Drosophila repulsive receptors, Unc5, Roundabout (Robo), and Derail

252 to compare directly the outputs of different repulsive receptors.

253 proper contrast due to tool operation in the repulsive regime on both materials.

254 The attractive/repulsive relationship between superconductivity and mag

255 Moreover, this is correlated with gain of repulsive response to Sema3A.

256 negative inhibition of Gnaz dampen the axon-repulsive response to Shh, and Gnaz mutant intestines co

257 Consistent with a repulsive role in arbor lamination, we observed compleme

258 etically for isotropic particles with a soft repulsive shoulder but have not been experimentally real

259 na around the microspheres and induce a soft repulsive shoulder that governs the self-assembly in thi

260 functional relevance of the cluster size for repulsive signaling is not understood.

261 own that the Slit/Roundabout and Netrin/Unc5 repulsive signaling pathways facilitate site-specific lo

262 Robo1/2 mutant embryos showed that Slit-Robo repulsive signaling was not required for post-crossing t

263 -DCC attractive signaling, but not Slit-Robo repulsive signaling, remains active in hindbrain post-cr

264 GRPs were still responsive to the remaining repulsive signals of CSPG.

265 Neural crest cells and repulsive slit1/robo2 signals then guide axons from late

266 n chain dimensions in the presence of purely repulsive spherical crowders.

267 quantum interference between attractive and repulsive states throughout the full depth of the Fermi

268 ndau-Verwey-Overbeek theory with an additive repulsive steric (entropic) ion-surface binding force.

269 ive noncovalent interactions juxtaposed with repulsive steric and electrostatic interactions explains

270 mechanism pointed to the importance of both repulsive steric and stabilizing intermolecular non-cova

271 n of interlayer coupling originates from the repulsive steric effects that leads to different interla

272 gen-bonding interactions, as well as typical repulsive steric interactions, in the transition state.

273 sidering attractive interactions, as well as repulsive steric interactions, when seeking to rationali

274 ed helices into close proximity, including a repulsive stretch of positively charged residues.

275 forming internal hydrogen bonds or avoiding repulsive substitution patterns.

276 which may be an indication of the effect of repulsive surface forces combined with selective pore si

277 ractions are represented by a single, purely repulsive term with no contributions from van der Waals

278 sight into the balance of the attractive and repulsive terms in the potential, and the resonance Rama

279 Biological weapons were regarded as "morally repulsive." This complacency stemmed from a 1972 Biologi

280 ows that intermolecular contrast arises from repulsive tip-sample interactions whose interpretation c

281 orces between active spinning particles from repulsive to attractive.

282 Both compounds were repulsive to IJs of Steinernema glaseri and S. riobrave

283 we transform the interaction energy from net repulsive to net attractive.

284 ent field, which can be tuned from isotropic repulsive to weakly or highly anisotropic attractive by

285 n into cis-signaling endosomes to outbalance repulsive trans-signaling.

286 By demonstrating both attractive and repulsive transistor modes, a single transistor architec

287 old occurs via spin-orbit coupling to nearby repulsive triplet states.

288 t C1q blocked both the growth inhibitory and repulsive turning effects of MAG in vitro.

289 g calpain cleavage of talin and FAK inhibits repulsive turning from focal uncaging of Ca(2+) within f

290 s growth cone filopodial protrusion and that repulsive UNC-40-UNC-5 heterodimers inhibit filopodial p

291 lypican functions in both the attractive and repulsive UNC-6/netrin pathways.

292 sensitive interplay in which attractive and repulsive van der Waals interactions between the differe

293 shed deep into the type 2 regime with purely repulsive vortex interactions.

294 ate hydration and induces strongly polarized repulsive water structures beyond at least three hydrati

295 ximating the substrate:GroEL interactions as repulsive, we obtain a strong acceleration in rate of be

296 er; however, the net F-A interaction remains repulsive while T-A pairing is attractive.

297 erse forces are attractive with left-CPL and repulsive with right-CPL.

298 nd particles) and its confinement are purely repulsive, with only a short-range attraction between th

299 Eliminating the function of a repulsive Wnt receptor, Ryk, in mice and rats by either

300 Furthermore, we show that blocking repulsive Wnt signalling increases axon plasticity and s