ライフサイエンスコーパス: repulsive

1 lit complexes so that signaling is no longer repulsive.

2 net interaction between these two lipids is repulsive.

3 heir interactions are neither attractive nor repulsive.

4 is engineered to be resonantly enhanced and repulsive.

5 ns and cannot be switched from attractive to repulsive.

6 e interactions between K10 chains are purely repulsive.

7 t makes one association pleasant and another repulsive?

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

9 and Robo family members and show that NELL2 repulsive activity is a function of its Robo3 affinity a

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

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

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

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

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

17 ceptual decisions can be repelled away from (repulsive adaptation) or attracted towards recent visual

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 Here we disentangle repulsive and attractive biases by exploring their respe

21 t is currently unclear whether and how these repulsive and attractive biases interact during visual p

22 The repulsive and attractive CO-pai aromatic interactions we

23 7, although AH and BSA respectively undergo repulsive and attractive electrostatic interactions at t

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

25 effect enabled the selective application of repulsive and attractive forces to send or receive singl

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

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

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

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

30 hydrodynamic interaction from attractive to repulsive and can drive the particle assemblies to under

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

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

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

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

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

36 m recoil as due to molecular excitation to a repulsive anti-bonding state, in which recoil of the dis

37 The consequent shorter lifetime of the repulsive aromatic anion of PhBr is consistent with the

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

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

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

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

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

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

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

45 signals and redirecting axons across potent repulsive barriers to construct novel circuitry.

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 etallic, and inorganic chemistry is not only repulsive but can be attractive because of London disper

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

51 ynaptogenic protein complex is also used for repulsive cell guidance.

52 ation, we show that a computational model of repulsive cell-cell interactions generates a mosaic with

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

54 nwide activity in response to attractive and repulsive chemosensory cues, characterizing multimodal c

55 ts ~2.5 angstrom to avoid a potential steric/repulsive clash.

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

57 Given that one would expect a repulsive Columbic interaction to exist between the elec

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

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

60 Despite the presence of repulsive Coulomb forces, the cation-cation interaction

61 rom the joint effect of Fermi statistics and repulsive Coulomb interactions, which favours ground sta

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

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

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

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

66 and other migrating cell types by acting as repulsive cues within the migratory environment.

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

68 dothelial cells (ECs), while Sema3E mediates repulsive cues.

69 he cortex guided by different attractive and repulsive cues.

70 osensory stimuli can be either attractive or repulsive depending on an animal's hunger state.

71 r more disks, which are either attractive or repulsive depending on the selected pattern of light.

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

73 nsate subjected to a moving spin-independent repulsive dipole potential.

74 ical groundwater velocities by comparing the repulsive DLVO force between particle pairs to the hydro

75 this difference, indicating that VII screens repulsive DNA-DNA interactions.

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

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

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

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

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

81 rise from the balance between attractive and repulsive effects.

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

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

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

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

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

87 Stability was compromised by repulsive electrostatic forces originating from clusteri

88 n is dried, capillary pressure may overwhelm repulsive electrostatic forces, assembling aggregates th

89 ctivity for the cis isomer is also driven by repulsive electrostatic interactions in the case of a sy

90 cromolecular counterion that locally screens repulsive electrostatic interactions with an efficiency

91 uickly ejecting proteins, it is due to their repulsive electrostatic interactions with the exit tunne

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

93 There was no repulsive energy barrier between particles and collector

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

95 esoscopic model for the cumulative effect of repulsive excluded volume protein-protein interaction an

96 ge in dominant length scales, switching from repulsive excluded-volume interactions to intrachain att

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

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

99 Upon inhibition of trophic signaling, these repulsive factors may promote axonal pruning.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

114 0 due to the greater amount of electrostatic repulsive forces between droplets present at pH 7.0.

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

116 rane binding of syb-2 may compensate for the repulsive forces between the two membranes and/or the SN

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

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

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

120 f syb-2 regulate SNARE assembly and minimize repulsive forces during membrane fusion.

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

122 ross the midline in the floor plate requires repulsive forces from local Slit repellents.

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

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

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

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 Remarkably little attention has been paid to repulsive forces.

133 usly increasing intermolecular electrostatic repulsive forces.

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

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

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

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

138 Cdk5 activity is induced by the repulsive guidance cue Semaphorin3a (Sema3a), leading to

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

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

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

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

143 The repulsive guidance effect was significantly reduced when

144 ndritic morphogenesis but is dispensable for repulsive guidance events.

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 Repulsive guidance molecule A (RGMa) is a potent neurite

148 The Repulsive Guidance Molecule a (Rgma)/Neogenin 1 (Neo1) s

149 examine the role of a novel innate molecule, repulsive guidance molecule b (RGMb), in murine models o

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

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

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

153 Repulsive guidance molecules (RGMs) are cell surface pro

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

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

156 Concurrent attractive and repulsive history biases in perceptual decisions may thu

157 In contrast, the repulsive hydration and undulation interactions differed

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

159 anthopterin included, however, a problematic repulsive interaction between C=O and N of two adjacent

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

161 In contrast with the repulsive interaction energy between the particles and t

162 bonding can stabilize Boat, whereas electron repulsive interaction from opposing ester substituents f

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

164 For softer repulsive interaction potentials, these two transitions

165 vidence that magnons in a condensate exhibit repulsive interaction resulting in the condensate stabil

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

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

168 Both attractive and repulsive interactions are qualitatively explained by a

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

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

171 l growth process dominated by competitive or repulsive interactions between astrocytes.

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

173 Both repulsive interactions between cell and EPSs and the ove

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

175 Repulsive interactions between methane and water dominat

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

177 that, by altering the ratio of attractive to repulsive interactions between peptides, the behavior ca

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

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

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

181 natures of correlated motion suggest unusual repulsive interactions between the water molecules.

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

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

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

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

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

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

188 on occurs as a result of adsorbate-adsorbate repulsive interactions on the catalyst surface which adj

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

190 gand and the alkene substrate and that Pauli repulsive interactions tended to decrease enantioselecti

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

192 interactions with the OX1R while introducing repulsive interactions with the OX2R.

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

194 Carbonyl oxygens were observed to form repulsive interactions with unsubstituted arenes and att

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

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

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

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

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

200 stable rafts exhibiting chiral structure and repulsive interactions.

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

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

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

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

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

206 Colloidal particles with a repulsive interparticle potential spontaneously form cry

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

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

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

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

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

212 Here, we ask, what repulsive mechanism prevents the vortices from merging,

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

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

215 inement of orbitally shaken and magnetically repulsive millimeter-scale particles.

216 Ki-67 forms repulsive molecular brushes during the early stages of m

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

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

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

220 rtho aryl substituents and, conversely, with repulsive NCIs when the phenol has no aryl ortho substit

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

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

223 lyst imparts a combination of attractive and repulsive non-covalent interactions to direct the enanti

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

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

226 y controls cellular interactions by inducing repulsive or adhesive properties, depending on forward o

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

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

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

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

231 ds with one attractive patch on an otherwise repulsive particle surface serve as model systems to exp

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

233 Dilute suspensions of repulsive particles exhibit a Newtonian response to flow

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

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

236 ic data by the model enables quantifying the repulsive potential at the surface, as well as retrievin

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

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

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

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

241 Execution of their signature repulsive program then generates pulling forces, enablin

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

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

244 ile Pd(II) catalysts modulated by a mutually repulsive pyridine-type ligand have been shown to favor

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

246 signaling in turn induces expression of the repulsive receptor Plexin-A4, via induction of the trans

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

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

256 ence weakens the gap junctions and induces a repulsive sensory response to the training odorants, whi

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

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

259 yses suggest that Fili sends a transsynaptic repulsive signal to neurites of nonpartner classes that

260 tion places it in a prime position to send a repulsive signal to the trailing edge of the cell ahead

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

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 regulated by the balance between trophic and repulsive signaling.

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

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

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

268 " and 7A' through a crossing with the purely repulsive states 7A", 8A' and 8A" leading to a major R +

269 e initially populated Rydberg states and the repulsive states leading to dissociation induced by othe

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

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

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

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

274 at the selectivity is dominated by classical repulsive steric effects.

275 e transformation of the minor isomer through repulsive steric forces.

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

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

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

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

280 Although water is predicted to de-wet purely repulsive surfaces and evacuate crevices, the extent of

281 y calculation augmented by a Born-Mayer-type repulsive term between Li ions and the anions of the mat

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

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

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

285 orces between active spinning particles from repulsive to attractive.

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

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

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

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

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

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

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

293 lagen fibrils in their adhesive and in their repulsive, viscoelastic mechanical response as well as a

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

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

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

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

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

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

300 The repulsive zeta potential for the rock and the oil in low