ライフサイエンスコーパス: repulsion

1 on by the LCD is controlled by electrostatic repulsion.

2 electrons interact by the long range Coulomb repulsion.

3 e of both steric hindrance and electrostatic repulsion.

4 e is energetically favorable even for strong repulsion.

5 s essential for netrin-1/UNC5C-promoted axon repulsion.

6 ron density on O-3 increased 1,3-syn-diaxial repulsion.

7 d formation, which outcompeted electrostatic repulsion.

8 tive cellular effects as F-actin disassembly/repulsion.

9 helix of one protomer breaks to relieve the repulsion.

10 NC5C is involved in netrin-1-mediated axonal repulsion.

11 ork distortions are required to avoid steric repulsion.

12 respectively drive pheromone attraction and repulsion.

13 uito heat seeking relied on cooling-mediated repulsion.

14 dominating increase of short-range entropic repulsion.

15 liver bud formation and laterality via cell repulsion.

16 further inward and receiving stronger water repulsion.

17 tors bind Slit guidance cues to mediate axon repulsion.

18 y the authors' brief discussion of reference repulsion.

19 ectrons minimize their strong mutual Coulomb repulsion.

20 tether between cells, thereby enabling cell repulsion.

21 way is required for EphB2-stimulated contact repulsion.

22 eractions between neurons through homophilic repulsion.

23 attraction, although some ORN types produced repulsion.

24 1 reverse signaling and causes neuronal axon repulsion.

25 spreading is due to long-ranged internuclear repulsion.

26 tor of up to 1.4 was observed due to Coulomb repulsion.

27 rans substantiating effect through lone pair repulsion.

28 the C38 tail opposes aggregation via steric repulsion.

29 exin receptors are known to induce cell-cell repulsion.

30 e close to each other, causing electrostatic repulsion.

31 le of superconductivity from on-site Coulomb repulsion.

32 territories, possibly mediated by cell-cell repulsion.

33 prompted by the intramolecular electrostatic repulsion.

34 NMs significantly possibly by electrosteric repulsion.

35 sfer in competition with destabilizing Pauli repulsions.

36 one entropy and salt-dependent electrostatic repulsions.

37 pitope, highlighting roles for charge-charge repulsions.

38 n and for those held apart due to long-range repulsions.

39 Cu catalyst and the ligand-initiator steric repulsions.

40 cessive chlorination, due to nonbonded Cl-Cl repulsions.

41 gap in colloid attachment between favorable (repulsion absent) and unfavorable (repulsion present) co

42 rotein regions, application of attraction or repulsion, accounting for pairwise distance restraints,

43 lly biased to varying degree of net-negative repulsion across organisms.

44 n a layer and across the stromal gap, steric repulsion across the lumenal gap, and regulation of prot

45 tastasis formation by altering melanoma cell repulsion/adhesion to bone endothelial cells, and repres

46 e forcefully, granular stresses overcome the repulsion allowing particles to interact frictionally an

47 ed counterions from solution to avoid charge-repulsion along its backbone and with other PAH molecule

48 e dissociation products occurred due to C.Br repulsion along the prior C-Br bond direction.

49 ither Mott physics that captures the Coulomb repulsion among charges, or Hund physics that aligns the

50 Despite the repulsion among the anions, the lowest energy states hav

51 gered ABAB stacking that reduces the Coulomb repulsion among the stripes.

52 test the idea that event overlap triggers a "repulsion" among hippocampal representations that develo

53 st LPS contents studied due to electrostatic repulsion and abolishes membrane damage to S. oneidensis

54 al diversity is facilitated by electrostatic repulsion and an underpacked core between domains.

55 eural crest invasion is based on short-range repulsion and asymmetric attraction between neighboring

56 fluctuation spectrum, and oscillates between repulsion and attraction as a function of wall separatio

57 ut mice in hair growth, wound healing, water repulsion and body temperature regulation.

58 rons can be used to exactly balance both the repulsion and diffraction-broadening.

59 drance mechanism, coupled with electrostatic repulsion and entrance effects.

60 ic pair interactions consisting of hard-core repulsion and extra short-range soft-core repulsion beyo

61 nriched gene, PCDH15, mediates daughter cell repulsion and facilitates proliferation.

62 , but it rotates because of an electrostatic repulsion and forms a hydrophobic interface with ACE2.

63 The interplay of steric repulsion and hyperconjugative interactions in aza-glyci

64 imple flow geometries suggests intergranular repulsion and its influence on the frictional nature of

65 ield and a competition between vortex-vortex repulsion and Lorentz force.

66 ge density (r(2) = 0.94) while electrostatic repulsion and loss of positive charge due to destruction

67 disruption of RCP or EphA2 opposes cell:cell repulsion and metastasis in an autochthonous mouse model

68 d endocytic pathway which controls cell:cell repulsion and metastasis in vivo.

69 bility alteration, including rock/oil charge repulsion and microdispersion formation.

70 Attributing to the electrostatic repulsion and physical prevention of the ladder-shaped D

71 ically or genetically disrupts Slit-mediated repulsion and produces severe axon guidance defects in v

72 :Dsg and Dsc:Dsc interactions by same-charge repulsion and promote heterophilic Dsg:Dsc interactions

73 es outgrowth of the common cardinal vein via repulsion and signals through PlexinD1.

74 Strong Coulomb repulsion and spin-orbit coupling are known to give rise

75 We also characterize the repulsion and steering effect with various excitation vo

76 We demonstrate that cholesterol limits this repulsion and tendency to curve.

77 lecular systems are defined by electrostatic repulsion and the ability of the dominant attractive for

78 sebaceous lipids resulted in impaired water repulsion and thermoregulation, increased rates of UVB-i

79 group as opposed to factors lowering steric repulsion and/or dipole minimization.

80 lding overcomes intramolecular electrostatic repulsions and forces local dipoles in each layer of the

81 sites decreases the propensity for Coulombic repulsions and unfolding/restructuring, helping to prese

82 al than the proximal region of the GC during repulsion, and knockdown of either UNC5C or TUBB3 abolis

83 tin, phosphorylation increases electrostatic repulsion, and likely protein alignment and interfilamen

84 t lead to long-range attraction, short-range repulsion, and mutual alignment between adjacent swimmer

85 egativity, DeltaVNN is the change in nuclear repulsions, and Deltaomega is the change in multielectro

86 itively charged ions to reduce electrostatic repulsions, and induce attractions that can facilitate D

87 y, we demonstrate that electrostatic dye-dye repulsions are negligible for the interdye distance regi

88 NaCl electrolyte concentrations, interfacial repulsions are soft and longer in range, this transition

89 to the next, at odds with any simple Coulomb repulsion argument.

90 the axon guidance field is the importance of repulsion as a guidance mechanism for steering axons to

91 the axon guidance field is the importance of repulsion as a major guidance mechanism.

92 ompensating for intermolecular electrostatic repulsion, as a mechanism to control the length of a sup

93 mponent of these barriers, mediating contact repulsion at the cell surface in chick half-somites.

94 Many mutations reduce electrostatic repulsion at the Env apex and increase PG16 recognition

95 reactivity stems from differences in steric repulsions at the Ru alkylidene after CPE ring opening.

96 The resulting confounding electrostatic repulsion/attraction is strongly influenced by eluent sa

97 at we find is required for subsequent axonal repulsion away from Slit.

98 o-dimensional (2D) Hubbard model with strong repulsion below half-filling.

99 oscopy, most likely due to the electrostatic repulsion between 4-ABA-grafted graphene layers.

100 s packed under very high pressure due to the repulsion between adjacent layers of DNA, the circular d

101 ctive hopping behavior facilitated by strong repulsion between Ag ions.

102 ular macromolecules results from the overall repulsion between all components of the system and leads

103 are proposed to be due to the electrostatic repulsion between amino-functionalities and DA.

104 glomeruli, likely owing to contact-mediated repulsion between axons expressing identical combination

105 lectrostatically mimics DNA and can overcome repulsion between basic DNA binding regions of three bZI

106 nanoparticle bonding, whereas electrostatic repulsion between colloidal bonds governs CM symmetry.

107 lated substrate interaction and a long-range repulsion between dots.

108 Repulsion between E100 and the negatively charged surfac

109 n fail spectacularly, when the electrostatic repulsion between electrons causes strong correlations.

110 manipulate multi-electron beams, because the repulsion between electrons rapidly alters the beam shap

111 o be complemented by taking into account the repulsion between hydrogen atoms.

112 E46K misfolding pathway avoids electrostatic repulsion between K46 and K80, a residue pair which form

113 ns along the c-axis, driven by electrostatic repulsion between localized electron clouds on Tl and Te

114 of isomeric metallacycles governed by steric repulsion between methyl groups of the hydrocarbon chain

115 an be assigned to shielding of electrostatic repulsion between monomers on the fibril surface or betw

116 ries that minimize the unfavorable lone-pair repulsion between neighboring nitrogen atoms and maximiz

117 recognition that leads to either adhesion or repulsion between neurites.

118 caused by the large change in electrostatic repulsion between NPs when the dimers move from intersti

119 s to regulate contact-mediated attraction or repulsion between opposing cells, thereby influencing ti

120 expression; this relieves a native synaptic repulsion between PV cells and pyramidal neurons, thereb

121 Electrostatic repulsion between subcomponents can be overcome by the a

122 mers in the equilibrium revealed the highest repulsion between the 3-allyloxy group and the isopropox

123 els of force-extension behavior to show that repulsion between the aggrecans induces an internal tens

124 ges (zeta-potential) and hence electrostatic repulsion between the AgNPs.

125 primarily from intramolecular electrostatic repulsion between the allosteric and orthosteric ligands

126 The origin of this difference is Pauli repulsion between the electrons forming the bond and cor

127 he gas phase because of strong electrostatic repulsion between the extra electrons.

128 nation of capillary action and electrostatic repulsion between the graphene and its container to ensu

129 st-guest complex formation leading to charge repulsion between the host units, as well as an osmotic

130 reveal that in the anti-Markovnikov pathway, repulsion between the ligand and the alkyl group is mini

131 f the longer chains due to the electrostatic repulsion between the low-pI ACE2 and the heparin segmen

132 Added electrostatic repulsion between the membrane surfaces is used to ident

133 mobile H2 layers is to decrease the Coulomb repulsion between the negatively charged hydrogen atoms

134 fully expands the cages due to electrostatic repulsion between the positively charged sites.

135 organic semiconductor devices due to Coulomb repulsion between the two charges.

136 the collector surfaces through electrosteric repulsion between the two interpenetrating charged polym

137 rin skeleton, which alleviates electrostatic repulsion between the two NH protons, and two polarizati

138 Based on Coulomb's Law alone, electrostatic repulsion between two anions is expected to prevent thei

139 s a crucial role in overcoming the hydration repulsion between two membranes and thus rather lowers t

140 Our work revealed repulsion between virus and host CUBs when they are over

141 ng, alpha-helix formation, and electrostatic repulsions between acidic side chains, which collectivel

142 ic charge around the anion arise because the repulsions between weakly positively charged H atoms are

143 teractions at longer range--interparticulate repulsion--between particles that are complexing Eu(III)

144 re repulsion and extra short-range soft-core repulsion beyond the hard core, whose length scale is ro

145 e pH is lowered and electrostatic and steric repulsion builds up as the network histidine residues be

146 phenomenon is not specific to EphB2/ephrinB1 repulsion but is also present during the formation of bo

147 ptor) is safely large to avoid electrostatic repulsion but, at the same time, amenable to a closer ap

148 nal entropy and an increase in electrostatic repulsion by anionic lipids.

149 First, an attenuation of the interionic repulsion by the solvent facilitated close approach of t

150 three intracellular domains, suggesting that repulsion by Unc5, Robo, and Drl, and perhaps repulsion

151 ges in the membrane tension induced by ionic repulsion can explain the magnitude, time course, and sp

152 ttern of short-term attraction and long-term repulsion cannot be captured by an ideal Bayesian observ

153 sphere system (alphaBc) and screened Coulomb repulsion combined with short-range attraction (HEWL).

154 sically challenging because inter-electronic repulsion, crystal field, and spin-orbit coupling effect

155 By contrast, for weak repulsion, crystallites slowly grow and fuse through rea

156 cts the migration of neurons using a contact repulsion-dependent mechanism.

157 itored by ThT fluorescence shows that charge repulsion dictates phosphorylation-mediated fibril disso

158 ocess that is required for subsequent axonal repulsion downstream of the Robo receptor.

159 barrierless cage opening followed by Coulomb repulsion-driven fragmentation.

160 support parallel ionpair-pi interactions and repulsion-driven ion pairing with self-assembled fluorop

161 Early on, we have argued that repulsion-driven ion-pairing interactions with anionic l

162 in response to self-assembly, i.e., generate repulsion-driven ion-pairing interactions.

163 ange attraction and long-range electrostatic repulsion drives the formation of a colloidlike cluster

164 at considers the increased particle-particle repulsion due to branched chains and ligand polydispersi

165 dimerization might involve alleviating this repulsion due to its high density of negative charges.

166 s the open conformation as the electrostatic repulsion due to the reaped electrons pushes the DH and

167 n the transition-elements periods, and Pauli repulsion emerges as the factor that unifies CSB over th

168 The fitted repulsion energies fall within the theoretical range of

169 ion, and visualized dynamic contact-mediated repulsion events in primary mouse hippocampal neurons ov

170 afficking of EphA2 which generates cell:cell repulsion events that drive tumour cells apart.

171 We find that the repulsion exponent p approximately 6.5 provides an excel

172 We propose the inference of the repulsion exponent through Hierarchical Bayesian uncerta

173 rticle surface according to the conventional repulsion figures.

174 high salinity marine waters by electrosteric repulsion for long time periods.

175 the balance of the long-range attraction and repulsion forces which stabilizes the cluster patterns a

176 the interior of the NPC, setting up entropic repulsion forces.

177 al studies identify the cause as interligand repulsion forcing a wider C-Pd-C angle and tilting of th

178 iated activation of EphB4 induces tumor cell repulsion from bone endothelium, translating in reduced

179 not very effective because of electrostatic repulsion from clay surfaces with a net negative charge.

180 oes not bind Slits, but instead signals axon repulsion from its own ligand, NELL2.

181 hat the initial clustering is due to nuclear repulsion from the cell poles, while the third, most rob

182 centrosomes' attraction to kinetochores and repulsion from the chromosome arms have to be proportion

183 face carboxyl content, despite electrostatic repulsion from the growing negative charge.

184 raction between the charged species, and the repulsion from the surfaces with lower dielectric consta

185 atial scales, from long-range attraction and repulsion from the troop's sleeping site, to relatively

186 valence 6s orbital, and the respective Pauli repulsion generates M-M bonds with CSB character.

187 on of the AgNPs as a result of electrostatic repulsion, giving rise to a detectable color change.

188 Electrostatic repulsion has been found to govern colloidal stability o

189 vigate across the CNS midline, ROBO-mediated repulsion has traditionally been thought to be repressed

190 illary column operating in the electrostatic repulsion-hydrophilic interaction mode (ERLIC) and coupl

191 and RhoA signaling necessary for growth cone repulsion in GABAergic interneurons in vitro, which may

192 epulsion by Unc5, Robo, and Drl, and perhaps repulsion in general, involves Trio activity.

193 a more important role than A36-driven super-repulsion in promoting the cell-to-cell spread of vaccin

194 nsive approach is taken to study the role of repulsion in the assembly behavior of DNA-NPs, enabling

195 UBB3 or UNC5C blocked netrin-1-promoted axon repulsion in vitro and caused defects in axon projection

196 Dopamine promotes CO(2) repulsion in well-fed animals, whereas octopamine promot

197 related to differences in electron-electron repulsions in the conjugated and nonconjugated systems,

198 rhenium centers, reducing electron-electron repulsions in the rhenium-Cp moieties and thereby streng

199 ng the phenomenon of negative dependence, or repulsion, in data.

200 yn isomer fraction increases, intermolecular repulsion increases, resulting in a decrease in the unit

201 model incorporating line tension and dipole repulsion indicated that even small changes in line tens

202 Bi-directional contact repulsion induced by Eph/ephrin signaling involves trans

203 ke clay particles that is driven by particle repulsions instead.

204 averted due to a screened long-range Coulomb repulsion intrinsic to disordered q1D materials.

205 and-substrate steric interactions and steric repulsions involving the pseudoaxial substituent in the

206 As a result, ROBO-mediated axonal repulsion is activated early in development to prevent p

207 We found that heterochromatin repulsion is locally encoded by Set1/COMPASS on certain

208 most unconventional superconductors, Coulomb repulsion is minimized through the formation of higher a

209 This suggests that neural and perceptual repulsion is not a mechanism to enhance perceptual perfo

210 Repulsion is reduced both in vivo and in vitro by a rang

211 r than in graphene while the on-site Coulomb repulsion is reduced to a lesser extent.

212 that cannot be cleaved revealed that midline repulsion is still present but longitudinal axon guidanc

213 raction between diamondoids overcomes steric repulsion leading to a cis configuration at the active g

214 Electrostatic repulsion leads either to autodetachment of electrons or

215 nformation at low force, where electrostatic repulsion leads to a strong excluded volume effect, and

216 at this previously insurmountable electronic repulsion may be overcome through the use of sufficientl

217 Herein, cation-cation repulsion may play a significant role for the high valen

218 Based on ion specificity, an adsorption-repulsion mechanism, we suggest that the exocytotic Hofm

219 from quadrupole-energy-minimizing to steric-repulsion-minimizing.

220 for relatively thin substrates a short-range repulsion occurs, which prevents the two drops from comi

221 ivity over ascorbic acid (AA) because of the repulsion of AA by the negative electric field at the ho

222 oid membranes due to increased electrostatic repulsion of adjacent membranes; 2) p-PSBS accumulation

223 ity/alkalinity often break the electrostatic repulsion of AuNPs suspension, or/and the surface functi

224 a tok mutants lacking Slit cleavage, midline repulsion of axons occurs normally, confirming that Slit

225 l molecules and helps overcome the Coulombic repulsion of bringing two cationic species into contact.

226 er and solute channel is responsible for the repulsion of cations.

227 ture due to the adsorption and electrostatic repulsion of chaotropes on the hydrophobic portion of th

228 fine balance between surface charges, steric repulsion of coating molecules, and hydration forces aga

229 from neutral H(2)O(2) and that electrostatic repulsion of contaminants from the electrode is not prob

230 that polycations can turn electrostatic self-repulsion of DNA into attraction, yet the physical mecha

231 ransition from E* to E through electrostatic repulsion of E217.

232 on strategies as gene knockdown leads to the repulsion of economically important plant parasites and

233 ckdown of each transporter gene triggers the repulsion of economically relevant Meloidogyne and Globo

234 Contact repulsion of growing axons is an essential mechanism for

235 dings indicate that event overlap triggers a repulsion of hippocampal representations-a finding that

236 synchronized discharges could facilitate the repulsion of large predators or immobilize large prey.

237 extended conformation, possibly due to local repulsion of like-charges along the chain.

238 idization between them interact via a strong repulsion of range and strength larger than the repulsio

239 usion of key DNA-binding residues and charge repulsion of the DNA backbone.

240 Electrostatic repulsion of the highly negatively charged MS2, fr, and

241 Lateral repulsion of the ions on both sides of the membrane affe

242 Especially at high coverage, a hard-sphere repulsion of the molecules and the confinement at the ca

243 he lipids, possibly due to the higher steric repulsion of the protein coated nanoparticles.

244 Due to the repulsion of the two aryl substituents within the same b

245 ional destabilization of 3-Pheq conformer by repulsion of unidirectional dipoles of the endocyclic ox

246 Bacterial motility, and in particular repulsion or attraction toward specific chemicals, has b

247 nt can be achieved through either increasing repulsion or reducing attraction by modifying the fluid

248 del accounting for an enhanced electrostatic repulsion originating from the surface immobilization of

249 onal theory calculations including a Coulomb repulsion parameter U, we explore the topological proper

250 lation have much less linkage information in repulsion phase than in coupling phase.

251 nation fractions between dominant markers in repulsion phases.

252 emoving the steric hindrance and same-charge repulsion phenomena via multilayer adsorption.

253 ulsion of range and strength larger than the repulsion predicted by models that neglect ionic correla

254 avorable (repulsion absent) and unfavorable (repulsion present) conditions through a combination of h

255 ect-for mixtures at rest or shearing slowly, repulsion prevents frictional contacts from forming betw

256 ment increased via reduced colloid-collector repulsion (reduced radius of curvature) and increased at

257 Cell repulsion requires bidirectional trans-endocytosis of cl

258 LRT1-3), thereby promoting cell adhesion and repulsion, respectively.

259 hrin-A-EphA2 signaling, which induces a cell repulsion response in RasV12 cells.

260 roles for CHL1 in both axonal extension and repulsion, selectively of DA neurons, suggestive of a ro

261 mulations driven by nearest-neighbor vacancy repulsions show checkerboard vacancy order to emerge for

262 sential role in netrin-1/UNC5C-mediated axon repulsion.SIGNIFICANCE STATEMENT Proper regulation of mi

263 oints by introducing directionality in their repulsion structure, and the principal directions corres

264 qualitative differences in receptor-mediated repulsion, suggesting that, despite their highly diverge

265 siology and behaviour, the Robo-Slit midline repulsion system, and the neurotrophin signalling system

266 , we were able to demonstrate that the Pauli repulsion term increases more significantly when going f

267 rmation of finite-sized rafts and mediates a repulsion that distributes them evenly throughout the me

268 charge acquired during ESI reduces Coulombic repulsion that leads to dissociation, and charge reducti

269 explicitly show how CIL yields an effective repulsion that promotes cell dispersal, thereby hinderin

270 s of anionic lipids experience electrostatic repulsion that, being exerted asymmetrically, is predict

271 Due to electronic repulsion, the antiferromagnetic correlations of the imp

272 Under conditions of strong interparticle repulsion, the colloidal crystal rapidly grows from the

273 rgistic effects of size exclusion and charge repulsion, the novel UF hollow fibers can effectively re

274 ascular deformity was related to endothelial repulsion through binding to the UNC5B receptor.

275 f alpha-lapachone is a result of lower Pauli repulsion throughout the reaction path, when compared to

276 hiking) and are necessary for switching from repulsion to CO2 (a carrier animal cue) in nondauers to

277 ple key roles in neurodevelopment, from axon repulsion to dendrite elaboration.

278 ng charge neutralization overcomes coulombic repulsion to progressively allow condensation, folding,

279 s usually show uni-directional attraction or repulsion toward their specific cue molecules.

280 the insulating gap is driven by the Coulomb repulsion U on the transition-metal cation, and charge-t

281 ) when the on-site electron-electron Coulomb repulsion (U) is much larger than the nearest-neighbor i

282 sequences, each intracellular domain elicits repulsion via a common pathway.

283 the very general Valence Shell Electron Pair Repulsion (VSEPR) model to the most esoteric reaction me

284 The strength of 1,3-syn-diaxial repulsion was evaluated for main types of protecting gro

285 The repulsion was mediated by two mechanisms-activation of a

286 lizing force and then varying this colloidal repulsion, we can trigger self-assembly of these nanopar

287 Focusing on Semaphorin/Plexin repulsion, we identified an interaction between the F-ac

288 to clarify the conditions of attraction and repulsion, which are determined by balance between activ

289 rminal branch numbers without causing axonal repulsion, which is a role that distinguishes Sema5B fro

290 s) must overcome electrostatic strand-strand repulsion, which is moderated by the surrounding atmosph

291 nth depends on coordinated inter-endothelial repulsion, which prevents uncontrolled layering of the e

292 remarkably strong long-range attractions or repulsions, which can be split into three regimes depend

293 fts with the same chirality have long-ranged repulsions, while those with opposite chirality acquire

294 LJ potential models atomistic attraction and repulsion with century old prescribed parameters (q = 6,

295 d restriction via contact-dependent cellular repulsion with macrophages.

296 ng about stabilization due to greater steric repulsion with the box frame.

297 e covalent bond-pairing is weakened by Pauli-repulsion with the semicore electrons, and CSB takes ove

298 sions was mainly attributed to electrostatic repulsion, with droplet aggregation occurring at low pH

299 ional analysis, we reveal that electron pair repulsion within the deprotonated anion is not the reaso

300 e electric field that decays within the core repulsion zone of the surface and hence vanishes in regi