ライフサイエンスコーパス: coulombic

1 igh fluorophilicity of [2]+ arises from both Coulombic and cooperative effects which lead to formatio

2 values, obtained from a novel separation of coulombic and Hofmeister effects.

3 er structures in the gas phase due to strong Coulombic and hydrogen-bonding interactions.

4 icult to isolate effects such as the role of Coulombic and hydrogen-bonding interactions.

5 Moreover, we find that Coulombic and intrinsic contributions to membrane bindin

6 eld in conjunction with ReaxFF and including Coulombic and Lennard-Jones interactions is employed to

7 In order to elucidate to what extent Coulombic and other interactions contribute to the origi

8 alyzes Michael addition reactions using only Coulombic and other weak interactions to activate variou

9 ts (epsilon(eff) and epsilon(p)) required in Coulombic and Poisson-Boltzmann models.

10 nergy of the binding and its two components, Coulombic and reaction field energy.

11 ic separations realize negligible long-range Coulombic and short-range charge-transfer-mediated coupl

12 reveal strong intermolecular van der Waals, Coulombic, and H-bond interactions in striking agreement

13 ely; however, large losses in van der Waals, Coulombic, and H-bond interactions strongly suggest that

14 holes, which can more easily overcome their coulombic attraction and form free charges.

15 s, and an enthalpic component, stemming from Coulombic attraction between opposite charges.

16 o nanoelectrospray ionization as a result of Coulombic attraction between positively charged protein

17 Second, Coulombic attraction between the separated charges favor

18 recombination-poor diffusion and significant Coulombic attraction can cause electrons and holes to en

19 ognition process, which relies on an initial Coulombic attraction of anionic SAMs to the cationic HBS

20 inhibited by supramolecular factors such as Coulombic attraction or repulsion between a charged gues

21 fs (tryptophan zipper, disulfide, d-Pro-Gly, Coulombic attraction, l-Pro-Gly) enhance formation rates

22 han would be expected on the basis of simple Coulombic attraction.

23 cular, strong correlations are found between Coulombic attractions and the electrostatic desolvation

24 can provide conformational stabilization via Coulombic attractions that do not require entropically c

25 e LUMO, and hence lowers Ueff, the effective Coulombic barrier to charge transfer.

26 s (I37K, Q40K, and V38E) lead to significant Coulombic changes that weaken favorable van der Waals in

27 on potentials (alpha-values) quantifying non-Coulombic chemical interactions of KGlu with unit area o

28 At the same time, the Coulombic component of the binding energy was found to f

29 The binding is dominated by the coulombic contributions, which account for why the toxin

30 e reaction rate accelerations possible under Coulombic control and highlight important design criteri

31 Interatomic or intermolecular Coulombic decay (ICD) is a nonlocal electronic decay mec

32 This intermolecular Coulombic decay (ICD) process has since been shown to be

33 and charge transfer, such as intermolecular Coulombic decay and electron-transfer mediated decay (ET

34 the long-lived ones decay by an interatomic Coulombic decay between two iodine atoms, during the mol

35 standing of Auger-stimulated ion desorption, Coulombic decay, photodynamic cancer therapies, and may

36 A well-known example is interatomic Coulombic decay, where an excited atom relaxes by transf

37 FRET is mediated by weak Coulombic dipole-dipole coupling of donor and acceptor f

38 -) largely compensates for the destabilizing Coulombic effect of any salt on the binding of this asse

39 FrdA E49Q and SdhA Q50E mutants suggest that coulombic effects and the electronic state of the FAD ar

40 ind guests in solution; cavity enclosure and coulombic effects appear to be crucial drivers of host-g

41 peration conditions which would minimize the Coulombic effects are discussed.

42 cts between hemes bL and bH and intermonomer Coulombic effects between bL hemes.

43 it was necessary to incorporate intramonomer Coulombic effects between hemes bL and bH and intermonom

44 However, large ion populations may manifest Coulombic effects contributing to the spatial dispersion

45 In this study, we present an analysis of Coulombic effects on IMS resolution.

46 ntermediate comes from studies of steric and Coulombic effects on the quenching rate constants and fr

47 Owing to favorable Coulombic effects, the para-derivative [1]+ has a very h

48 tion rates (0.39 vs. 0.37 m(3)-H(2)/m(3)/d), coulombic efficiencies (90% vs. 77%), and overall hydrog

49 cycles indicates excellent reversibility and coulombic efficiencies above 99%.

50 The Coulombic efficiencies and cycle lives of LMBs with ethy

51 nimized specific surface area delivered high Coulombic efficiencies and long cycling stability at 60

52 with low round-trip overpotentials and high coulombic efficiencies as opposed to traditional K-O(2)

53 e lithium plating on copper with outstanding coulombic efficiencies at room and elevated (50 degrees

54 volumetric energy and power density values, coulombic efficiencies in excess of 95%, and stability o

55 with capacities of nearly 900 mA h g(-1) and Coulombic efficiencies in excess of 99%.

56 s with remarkable cycling stability and high coulombic efficiencies in excess of 99.5%.

57 Li-SPAN cells cycle trouble free and at high Coulombic efficiencies in simple carbonate electrolytes.

58 Coulombic efficiencies near 100 % for every cycle, sugge

59 se nanoparticles to achieve high first-cycle Coulombic efficiencies of 94% to >100%.

60 occupy the solvation sheath and improve the Coulombic efficiencies of both the anode and cathode.

61 O(2) , NCM 811) cathodes exhibit 99.6-99.9% Coulombic efficiencies, high discharge voltages up to 4.

62 yte have an impressive performance with high Coulombic efficiencies, small overpotentials, and good c

63 bits stable cycling over 50 cycles with high Coulombic efficiencies.

64 capacity decay, low rate capacities and low Coulombic efficiencies.

65 ll specific energy of >300 W h kg(-1) with a Coulombic efficiency >95% for 80 cycles.

66 mA g(-1), with only 11% capacity fade and a Coulombic efficiency >99%.

67 hours of continuous cycling are achieved at Coulombic efficiency >99.5 % without dendrite formation

68 g(-1) at 100 mA g(-1) after 50 cycles), high coulombic efficiency (>95%), excellent cycling stability

69 y-z)Al(z)O(2) (NCA) show reduced first cycle Coulombic efficiency (90-87% under standard cycling cond

70 lithium deposition and significantly improve Coulombic efficiency (99% over 400 cycles at a current d

71 fter 200 cycles at 0.2C), and a high average Coulombic efficiency (99.7% from the second cycle to the

72 -electrolyte contact area, resulting in high Coulombic efficiency (99.87%) and volumetric capacity (1

73 Zn@Nafion-Zn-X composite anode delivers high coulombic efficiency (ca. 97 %), deep Zn plating/strippi

74 as the positive electrode) demonstrates high Coulombic efficiency (ca. 99.8 %) and a negligible capac

75 rnately catalyzing anodic acetate oxidation (Coulombic efficiency (CE) 85.3%) and cathodic denitrific

76 consumes electrolyte and Li, leading to low coulombic efficiency (CE) and short cycle life for Li me

77 t 9.35 +/- 0.28 g Fe3O4-Fe/L, resulting in a Coulombic efficiency (CE) for iron oxidation of 93.5 +/-

78 Consequently, the Coulombic efficiency (CE) increased: 57% for 0.02 g of F

79 nding to minimize cycling capacity decay and Coulombic efficiency (CE) loss.

80 anode materials to achieve high first cycle Coulombic efficiency (CE) of >100% or serve as an excell

81 over a period of 12 weeks and had an average Coulombic efficiency (CE) of 84.1 +/- 1.1% at practicall

82 Mg electrodeposition was achieved with high Coulombic efficiency (CE) of 90% and high current densit

83 only 10 mM bicarbonate buffer and an average Coulombic Efficiency (CE) of 93%.

84 ility of 5 mA cm(-2) , and a remarkably high Coulombic efficiency (CE) of ~99.57% without dendrite fo

85 ersible cycling of Li metal anodes with high Coulombic efficiency (CE) on both conventional planar su

86 Coulombic efficiency (CE) varied by electron donor, with

87 Furthermore, the measured Coulombic efficiency (CE) was at least 79%, which is 2.5

88 eversible Li anodes, e.g. as measured by the coulombic efficiency (CE), raise prospects for as signif

89 use short circuits, thermal runaway, and low coulombic efficiency (CE).

90 h anodes suffer from dendrite growth and low Coulombic efficiency (the ratio of charge output to char

91 ate cycling of a lithium metal anode at high Coulombic efficiency (up to 99.1%) without dendrite grow

92 The Coulombic efficiency also reaches a record 99% in 150 cy

93 950 h) at 0.5 mA cm(-2) , with 98.9% cycling Coulombic efficiency and 0.085 V overpotential.

94 ctrochemical performance, specifically, 95 % Coulombic efficiency and 197 mV overpotential, enabling

95 cled at 450 degrees Celsius with 98 per cent Coulombic efficiency and 73 per cent round-trip energy e

96 ghest capacitance of 1,287 F/g, with 100% of Coulombic efficiency and 79% of capacitance retention.

97 gh energy and power performance, nearly 100% coulombic efficiency and 85% energy efficiency after 25,

98 /- 4.35%, while the average percent error of Coulombic efficiency and COD removal rate predictions we

99 /Li2 O interface are critical to enhance the coulombic efficiency and cyclic performance of SnO2 -bas

100 nt species of VFA by using two methods i.e., coulombic efficiency and cyclic voltammetry was investig

101 apacity of 891 mAh g(-1) at 0.5 C with 99.5% coulombic efficiency and cycling stability up to 1000 cy

102 High coulombic efficiency and dendrite suppression in carbona

103 60 mA h g(-1)) and lowest potential, but low Coulombic efficiency and formation of lithium dendrites

104 f lithium metal anodes suffers from the poor Coulombic efficiency and growth of lithium dendrites.

105 ransport towards the Li-metal, also has high Coulombic efficiency and kept 93 % of its capacity after

106 exhibit a dendrite-free morphology with high Coulombic efficiency and long cycle life during plating/

107 to achieve high sulfur utilization with high Coulombic efficiency and long cycle life of Li-S batteri

108 hiation-induced strain and thus exhibit high Coulombic efficiency and long cycle life.

109 polymer/LLZT-2LiF/LiFePO4 battery has a high Coulombic efficiency and long cycle life; a Li-S cell wi

110 modified electrode achieved greatly enhanced Coulombic efficiency and longer cycle life.

111 ing lithium plating/stripping results in low Coulombic efficiency and severe safety hazards.

112 h the supramolecular capsules retains a high Coulombic efficiency and shows a large increase in capac

113 capacity of approximately 110 mAh g(-1) with Coulombic efficiency approximately 98%, at a current den

114 60 mAh g(-1) at 6 C, over 6,000 cycles with Coulombic efficiency approximately 99%.

115 A low operational voltage and high coulombic efficiency are achieved by using a novel compo

116 However, low first-cycle Coulombic efficiency as a result of the formation of a s

117 over the MCMB reference but present a lower Coulombic efficiency as well as a higher capacity loss p

118 to cycle up to 1000 times, with nearly 100% coulombic efficiency at both low (0.15 coulomb) and high

119 unmodified samples, which usually show rapid Coulombic efficiency decay in fewer than 100 cycles.

120 but suffer from rapid capacity fade and low Coulombic efficiency due to the high permeability of red

121 , leading to serious safety concerns and low Coulombic efficiency during charge/discharge cycles.

122 However, dendrite growth and limited Coulombic efficiency during cycling have prevented its p

123 is amide electrolyte achieves a high average Coulombic efficiency during cycling, resulting in an out

124 86% incommensurate sample achieves above 99% coulombic efficiency exhibiting 930 mAh g(-1) specific c

125 of approximately 1400 mA h g(-1) with a low Coulombic efficiency for the first cycle (approximately

126 The Coulombic efficiency improves to approximately 99% for m

127 for over 250 cycles, and outstanding average Coulombic efficiency in excess of 99.9%.

128 ted here will be generally useful to enhance Coulombic efficiency in many electrochemical systems (e.

129 es and determine the underlying cause of low Coulombic efficiency in plating and stripping (the charg

130 Reduced coulombic efficiency is observed at low rates (<25 mVs(-

131 resulted in similar organic removal, but the Coulombic efficiency obtained from the MPPC was 21 times

132 ppress Li dendrite growth and achieve a high Coulombic efficiency of >99 % for both the Li anode and

133 ile showing excellent long-term performance (coulombic efficiency of 100 % and energy efficiency of 7

134 chieve over 260 mAh/g after 700 cycles and a Coulombic efficiency of 101.1%, without the use of harmf

135 Besides, a maximum coulombic efficiency of 26.87% with 91% COD removal was

136 er squared (mA cm(-2)) of applied current at coulombic efficiency of 35% (35% of the applied current

137 pacity as high as 301 mAh g(-1) with initial Coulombic efficiency of 93.2%.

138 cling performance (over 1,000 cycles) with a Coulombic efficiency of 94.1%.

139 The use of fluoromethane shows a high coulombic efficiency of 97% for cycling lithium metal an

140 capacity of 3 mAh cm(-2) and a high average Coulombic efficiency of 97.3% are achieved.

141 fic capacity of 1,030 mAh g(-1) at 0.5 C and Coulombic efficiency of 98.4% over 1,000 cycles are achi

142 ) for more than 1,000 cycles with an average Coulombic efficiency of 98.4%.

143 ay as low as 0.046% per cycle and an average coulombic efficiency of 98.5% was achieved.

144 close to 600 mAh g(-1) at a high rate with a Coulombic efficiency of 99 over 160 cycles, an extremely

145 bles a Zn||Ti cell to achieve a high average Coulombic efficiency of 99.1 % for 350 cycles.

146 raphene and stability over 100 cycles with a Coulombic efficiency of 99.3% at a current rate of 0.2 C

147 as anode and LiCoO(2) as cathode) with high Coulombic efficiency of 99.4% over 300 cycles.

148 n Zn||Ti half-cell to achieve a high average Coulombic efficiency of 99.5% for 400 cycles (400 h), an

149 anode to achieve a high Li plating/stripping Coulombic efficiency of 99.55 % (1 mA cm(-2) , 1.0 mAh c

150 e charge/discharge process with an excellent Coulombic efficiency of 99.6%.

151 state Li/LiFePO4 cells showed a notably high Coulombic efficiency of 99.8-100% over 640 cycles.

152 te to the electrode leading to not only high coulombic efficiency of 99.9% but also maintaining high

153 ity of 802 mAh g(-1) after 659 cycles with a Coulombic efficiency of 99.9%, which outperforms convent

154 le capacity of 3.0 mAh cm(-2) and an average Coulombic efficiency of 99.9%.

155 performance is enabled by a stable half-cell coulombic efficiency of 99.97%, averaged over the first

156 ecific capacity of about 70 mA h g(-1) and a Coulombic efficiency of approximately 98 per cent.

157 apacity of approximately 100 mAh g(-1) and a Coulombic efficiency of approximately 99% over hundreds

158 gh-order polysulfide in electrolytes and low Coulombic efficiency of Li anode require excess electrol

159 ndrites, leading to long cycle life and high Coulombic efficiency of lithium metal anodes.

160 duction rate of 49.9 mmol/day . m(2), with a Coulombic efficiency of over 90%.

161 The hybrid cathode also shows a high Coulombic efficiency of over 99 % after 250 cycles.

162 t inserting sulfur into pores of carbon, the coulombic efficiency of SC/Li cell in the new DOL/D2 ele

163 The transformation occurs at high yield and coulombic efficiency of the 4-electron CO(2) reduction i

164 lexes, plays a significant role in enhancing coulombic efficiency of the corresponding solvated Mg co

165 to improvements in the voltage stability and coulombic efficiency of the electrolyte.

166 High coulombic efficiency of up to 94 % was achieved in dimet

167 lity, and excellent cycling stability with a Coulombic efficiency of ~100%.

168 an example, the protected Li anodes achieve Coulombic efficiency of ~99% and ultralong-term reversib

169 pansion, delivering a significantly improved Coulombic efficiency of ~99.2% over 150 cycles at 4 mA c

170 ectrolyte showed good cyclability and a high coulombic efficiency over 40 charge/discharge cycles.

171 ng up to 99% of their capacity and 99 +/- 1% Coulombic efficiency over 50 cycles by bulk electrolysis

172 ire arrays reaches 969.72 mAh . g(-1) with a coulombic efficiency over 99% at 500 mA . g(-1) after 50

173 ty by dissolution suppression, and 3) higher Coulombic efficiency owing to the lack of oxygen evoluti

174 mony nanocrystals have a consistently higher Coulombic efficiency than larger nanoparticles.

175 batteries reached voltages up to ~ 4 V, high Coulombic efficiency up to 99.9%, and high energy and po

176 The anode Coulombic efficiency was 44-69%, which is comparable to

177 Thus, the Coulombic efficiency was approximately 16% higher in the

178 A bioanode with high current density and coulombic efficiency was developed by co-immobilization

179 cm(-2) ) with excellent cycle stability and Coulombic efficiency were both demonstrated in Li metal

180 d Mg metal allows reversible operation (100% Coulombic efficiency) with no dendrite formation.

181 5 g L(-1) acetate) at 379 g m(-2) d(-1) (36% Coulombic efficiency).

182 cific capacity of 1,540 mAh g(-1) with a 75% coulombic efficiency, and an 86% incommensurate sample a

183 res of the solid electrolyte interphase, low Coulombic efficiency, and dendritic growth of Li.

184 tal dendrite growth for liquid systems, poor Coulombic efficiency, and gas evolution.

185 lls exhibit better cycling stability, higher Coulombic efficiency, and less self-discharge compared t

186 ock to achieve high sulfur utilization, high Coulombic efficiency, and long cycle life.

187 age hysteresis, a flat voltage plateau, high Coulombic efficiency, and no performance decay for at le

188 by issues related to dendrite growth and low Coulombic efficiency, CE.

189 ic charge/discharge capacities and excellent Coulombic efficiency, demonstrating the effectiveness of

190 near the surface, which leads to a decreased coulombic efficiency, likely because of trapped Li withi

191 new electrolyte demonstrates a close to 100% coulombic efficiency, no dendrite formation, and stable

192 rode-electrolyte interfaces that impacts the Coulombic efficiency, operational rate capability, and l

193 ic and "dead" Na formation that leads to low Coulombic efficiency, short lifespan and even safety con

194 be the optimized parameter toward capacity, Coulombic efficiency, stability, and rate capability enh

195 Organic loading in a fed-batch MFC affected Coulombic efficiency, which decreased from 40% at 0.66 g

196 methane microbial fuel cell operates at high Coulombic efficiency.

197 exhibits a good cycle life and an excellent coulombic efficiency.

198 from the growth of lithium dendrites and low Coulombic efficiency.

199 Ah g(-1) reversible capacity and nearly 100% Coulombic efficiency.

200 ng with excellent cycling stability and high coulombic efficiency.

201 in terms of capacity, cycling stability, and Coulombic efficiency.

202 rbide particles cycle lithium-ions with high Coulombic efficiency.

203 based batteries, cause safety issues and low Coulombic efficiency.

204 r approximately 30 h with approximately 100% Coulombic efficiency.

205 uel cells with increased current density and coulombic efficiency.

206 l composite electrode and about 100 per cent Coulombic efficiency.

207 ass) for >1,000 cycles at approximately 100% coulombic efficiency.

208 leads to ionization of a neighboring one via Coulombic electron interactions.

209 ds the leading end toward the anode, because Coulombic (electrophoretic) forces are dominant on negat

210 Coulombic electrostatic interactions have been shown to

211 )obs) by way of an analytic treatment of the Coulombic end effect (CEE).

212 ucleus-independent chemical shift (NICS) and Coulombic energy of 15 j,k-fulvalenes (j, k = 3, 5, 7, 9

213 eceptor uses surface area, total energy, and Coulombic energy to achieve affinity.

214 e in the 2-4 mum size range and then undergo Coulombic fission.

215 ttraction overlaid with a normally repulsive Coulombic force.

216 Coulombic forces are evidently primary, but despite deve

217 If the anion is mobile, Coulombic forces hold this species in close proximity to

218 polar molecules can be driven by fluctuating Coulombic forces induced by flowing polar liquids at nan

219 Thus, Coulombic forces mediate extracellular and intracellular

220 osing influence exerted by van der Waals and Coulombic forces on the reactivity of the carbohydrate/a

221 d guests, and we confirm the primary role of Coulombic forces with a simple mathematical model approx

222 lding blocks that attract each other through Coulombic forces(1-4).

223 ed conformation in dimethyl sulfoxide due to Coulombic forces.

224 nd rigid surface, and unilateral contact and Coulombic friction with an uneven surface.

225 K(obs) and on Delta H degrees (obs) dissects coulombic, Hofmeister, and osmotic contributions to thes

226 the tested solutes on ProP appear to be non-coulombic in nature.

227 cling conditions, as well as the first-cycle coulombic inefficiency.

228 substitution, designed to create a favorable Coulombic interaction between ONC and a phosphoryl group

229 inally, evidence is presented that shows the Coulombic interaction between the charged analyte and cl

230 ntropy of the confined polyelectrolytes, the Coulombic interaction between the charged species, and t

231 In the case of HP7, the Coulombic interaction between the terminal NH3(+) and CO

232 hange at the chain termini implies that this Coulombic interaction contributes before or at the trans

233 ent of this catalysis boosting effect to the Coulombic interaction of these positive charges with the

234 pole-dipole coupling, referred to as a super-Coulombic interaction, is a result of an effective inter

235 with two chain ends in close contact through Coulombic interaction.

236 fts in our studies indicates that additional Coulombic interactions across the nonspecific-binding in

237 ent that aligns the patches that would favor Coulombic interactions along the chain.

238 minates between guanine and adenine by using Coulombic interactions and a network of hydrogen bonds.

239 n, with no limitations due to intermolecular Coulombic interactions and nonspecific binding.

240 gh an initial Rayleigh instability driven by Coulombic interactions and show how the intermediate sta

241 ew tool has been used to explore the role of Coulombic interactions between a core position on one he

242 Still, nonspecific Coulombic interactions between cationic molecules and an

243 he electrostatic energy as a sum of pairwise Coulombic interactions between effective fixed atomic ch

244 esigned and synthesised peptides to show how Coulombic interactions between ionizable 2,3-diaminoprop

245 nts and RO, and that TS exhibits most of the Coulombic interactions between R and O.

246 ost-guest interactions to overcome repulsive Coulombic interactions between the cationic M12L24 cages

247 smectic-ordered ionic liquid crystal through Coulombic interactions between the ion species.

248 tionally active catalysts owing to favorable Coulombic interactions involving the ammonium group and

249 t in major grooves of O pre-TS, forming most Coulombic interactions of RO and burying aromatic carbon

250 Stabilizing Coulombic interactions of this sort are found with many

251 It was found that the Z-scores of Coulombic interactions peak at a considerably negative v

252 ntum wells and are attributed to the intense Coulombic interactions present in 2D TMDs.

253 sole nucleating event; it also suggests that Coulombic interactions should be considered in the desig

254 As one would anticipate, Coulombic interactions under the periodic boundary condi

255 g, though small, are viewed as signatures of Coulombic interactions which support theories of polyele

256 shoe-shaped structure to engender long-range Coulombic interactions with RNase 1, which is cationic.

257 nsfer process that is strongly influenced by Coulombic interactions with the proximal cubane cluster

258 olecule are ideally suited to forming strong Coulombic interactions with two contiguous phosphate gro

259 All these findings indicate that the Coulombic interactions within WT protein-protein complex

260 These factors include Coulombic interactions, hydrogen bonding, and solvation,

261 fferences are largely determined by internal Coulombic interactions.

262 ly damp the possible periodic distortions in Coulombic interactions.

263 ectrostatic potentials results in disfavored Coulombic interactions.

264 ed that this counteranion effect arises from Coulombic ion-pairing interactions between the counteran

265 Here, we examine non-Coulombic ionic effects on the oligomerization propertie

266 fer rates, are conventionally limited to the Coulombic near-field.

267 es is driven thermodynamically by attractive Coulombic occlusion of the fourth vacant coordination si

268 s not a good discriminator of the WT; while, Coulombic or reaction field energies perform better depe

269 This non-Coulombic ordering is further enhanced in the presence o

270 We show that Coulombic ordering reduces when the pores can accommodat

271 al neutrality occurs in these liquids due to Coulombic ordering, in which ion shells of alternating c

272 regulation by SOD1 would prevent long range coulombic perturbations to residue pK(a) 's upon ET at c

273 r reaction enables electrons to escape their Coulombic potentials on ultrafast time scales.

274 s and monovalent microions that interact via Coulombic potentials to simulations of macroions interac

275 Coulombic recovery decreased as a function of nitrate do

276 ls (MEC and MPPC) achieved approximately 30% Coulombic recovery.

277 first one, dominated by long-range screened Coulombic repulsion (Wigner glass) and a second one, sta

278 d across the octahedral faces, and the Ir-Ir Coulombic repulsion across shared faces that destabilize

279 r the pairs on the outside--a consequence of Coulombic repulsion between the inner bipyridinium subun

280 Upon oxidation, Coulombic repulsion between the positively charged and m

281 Coulombic repulsion in the two-dimensional electron syst

282 ns of small molecules and helps overcome the Coulombic repulsion of bringing two cationic species int

283 charge per group becomes less likely due to Coulombic repulsion of like charges.

284 ar proton redistribution according to simple Coulombic repulsion prior to backbone cleavage into C: a

285 type-II conduction band alignment driven by coulombic repulsion that eliminates non-radiative multi-

286 ering the charge acquired during ESI reduces Coulombic repulsion that leads to dissociation, and char

287 he resulting charge neutralization overcomes coulombic repulsion to progressively allow condensation,

288 d dumbbell components gives rise to enhanced Coulombic repulsion, destabilizing the ground-state co-c

289 Despite the unfavorable Coulombic repulsion, the singlet diradical dianion dimer

290 r shape with limited mixing by diffusion and Coulombic repulsion.

291 the spatial evolution of ion packets due to Coulombic repulsion.

292 f charged sites decreases the propensity for Coulombic repulsions and unfolding/restructuring, helpin

293 nium radical cation, despite the presence of Coulombic repulsions.

294 nding information(12-18), polymer-attenuated Coulombic self-assembly enables conventional colloids to

295 roach that we refer to as polymer-attenuated Coulombic self-assembly.

296 A(*-)/D(*+) encounter pair, which outweighs Coulombic stabilization in acetonitrile.

297 to the free A(*-) + D(*+), which opposes the Coulombic stabilization of A(*-)/D(*+).

298 That prediction incorporated only a Coulombic stabilization of the A(*-)/D(*+) encounter pai

299 s strategy of catalysis boosting by means of Coulombic stabilization of the initial Fe(0)-CO2 adduct

300 ic charge analysis provided estimates of the Coulombic work terms associated with ion pairing, DeltaG