ライフサイエンスコーパス: coulomb

1 e long-standing macroscopic laws of Amontons-Coulomb.

2 uces an altered, more unfavorable balance of Coulomb and polar desolvation energies.

3 mplex interplay between local, multi-orbital Coulomb and spin-orbit interaction in elemental bismuth.

4 on of CoHex(3+) ions is mainly determined by Coulomb and steric interactions, while ion-correlation f

5 y and the energy scales of both the screened Coulomb and the electron overlap repulsions.

6 100% coulombic efficiency at both low (0.15 coulomb) and high (4.5 coulombs) discharge and charge ra

7 the applied transmembrane field, long-range Coulomb, and salt-concentration-independent, short-range

8 sfer of qstep2 (= nETqe/(1 + ARECRE/AOECOE)) coulombs (ARE,AOE andCRE,COEare the areas (cm(2)) and di

9 At this separation, the residual Coulomb attraction between charges is at or below therma

10 econfiguration of the local environment, the Coulomb attraction between electric charges is decreased

11 rvation on Qst, confirming the electrostatic Coulomb attraction between the H2 and the open metals be

12 in low dielectric constant media, where the Coulomb attraction of the ions may be significant and th

13 f the RPs are not significantly distorted by Coulomb attraction over these long distances.

14 ic photoconversion systems must overcome the Coulomb attraction to achieve long-range charge separati

15 The generation of gaseous polyanions with a Coulomb barrier has attracted attention as exemplified b

16 s, i.e., the Pt NP-metal surface dipole, the Coulomb blockade and quantum confinement effect in deter

17 gle-electron transistors based on electronic Coulomb blockade and quantum logic gates in Rydberg atom

18 ly 30-micrometer-wide channel shows a robust coulomb blockade effect at room temperature with a thres

19 experimentally imaging the transition from a Coulomb blockade localized in a zero-dimensional system

20 ade: the ionic counterpart of the electronic Coulomb blockade observed for quantum dots.

21 Coulomb blockade oscillations exhibit periodicity consis

22 Tracking noise levels around the Coulomb blockade peak as a function of gate voltage yiel

23 le-electron transistors, exhibiting periodic Coulomb blockade peaks.

24 the molecule exponentially increases in the Coulomb blockade regime and decreases at the charge dege

25 By immersing a Coulomb blockade thermometer in the (3)He/(4)He refriger

26 t the cooling of electrons in nanoelectronic Coulomb blockade thermometers below 4 mK.

27 electron-transport activation energy and the Coulomb blockade threshold for the GQD network were 35 m

28 detailed characterization of the collective Coulomb blockade transition, which is the finite-size an

29 es, strong coupling effects occur, including Coulomb blockade, negative differential resistance, dyna

30 fined quantum transport phenomena, including Coulomb blockade, the Kondo effect, clear excited states

31 pore junction, and the observation of ionic Coulomb blockade: the ionic counterpart of the electroni

32 from a continuum, yielding uniformly spaced Coulomb-blockade conductance peaks, consistent with tele

33 Here, we use Coulomb-blockade spectroscopy in an InAs nanowire segmen

34 How photoexcitations evolve into Coulomb-bound electron and hole pairs, called excitons,

35 Excitons, Coulomb-bound electron-hole pairs, are elementary photo-

36 nto superfluids, whereas spatially separated Coulomb-bound electrons and holes possess strong dipole

37 own to perform better than standard screened Coulomb canned routines, or to predict ion-binding sites

38 nteraction between electron spins in coupled Coulomb-confined systems.

39 t stable aggregates containing three or more Coulomb-correlated electron-hole pairs remain mostly une

40 Here it is extended to include Coulomb correlations and percolative band narrowing, as

41 n solid state, as they benefit from enormous Coulomb correlations between electrons and holes.

42 Coulomb correlations can manifest in exotic properties i

43 me develops as t/U decreases and the role of Coulomb correlations increases.

44 these fermions are critically influenced by Coulomb correlations.

45 phate) yielded a red colored solution with a Coulomb count corresponding to a net four-electron oxida

46 The very low coulomb count required (ca. 0.1 F per olefin) for the co

47 We develop a theory of interlayer Coulomb coupling containing no free parameters that acco

48 anofriction interface between a laser-cooled Coulomb crystal of individually addressable ions as the

49 Here, we report on the Coulomb crystallization of HCIs (specifically (40)Ar(13+

50 on and manipulation of a wide variety of ion Coulomb crystals formed from small numbers of ions.

51 s is determined by the interplay between the Coulomb (de)stabilization originating from the "boron co

52 ncy at both low (0.15 coulomb) and high (4.5 coulombs) discharge and charge rates.

53 Coulomb, dispersion and hydration effects appeared to be

54 ode, first-order electrostatic interactions (Coulomb) dominate the overall binding energy as evidence

55 The Coulomb drag in a system of two parallel layers is the r

56 Coulomb drag is a process whereby the repulsive interact

57 electrical engineering perspective, perfect Coulomb drag is analogous to an electrical transformer t

58 tive to many-body effects, and find that the Coulomb drag resistivity significantly increases for tem

59 We focus on the Coulomb drag transport measurements, which are sensitive

60 , such as the metal-insulator transition and Coulomb drag, and to the realization of functional devic

61 predominantly due to a reduction in adverse Coulomb effects as a result of ions being selectively in

62 gy of approximately 0.95-3.68 eV, due to the Coulomb electric interaction, and easily overcome the ac

63 bonding, despite the powerful opposition of Coulomb electrostatic forces.

64 After incorporating a Coulomb electrostatic potential and optimizing the solva

65 The integrated area of the current signal (coulombs) elicited by this electrolyte injection is depe

66 g the program ZENO and find that the average Coulomb energy <E C> is directly proportional to <m>.

67 These results indicate that the increase in Coulomb energy as a result of bringing the two positive

68 The Coulomb energy E C is defined by the energy required to

69 ly that a uniformly charged disc has a lower Coulomb energy than a sphere of the same volume.

70 e band alignment and transient excited-state Coulomb environment, rather than solely on quantum confi

71 D crystals experience a spatially nonuniform Coulomb environment, whose effect on the charge transpor

72 ge, it is often dominated by the much larger Coulomb exchange counterpart.

73 Coulomb excitation experiments were performed using acce

74 We Coulomb-explode the molecule with a second precisely del

75 ate geometric isomers by means of coincident Coulomb explosion imaging is presented, allowing isomer-

76 The results were obtained by Coulomb explosion imaging using a free electron laser an

77 y elusive Efimov state of (4)He3 by means of Coulomb explosion imaging.

78 n under maintenance of the 2-fold charge and Coulomb explosion into two singly charged fragments.

79 energies are matched closely by a classical Coulomb explosion model.

80 dataset from a pump-probe experiment on the Coulomb explosion of nitrogen molecules, our analysis re

81 2'-dipyridyl as a ligand exclusively undergo Coulomb explosion to produce two monocationic fragments.

82 ry atomization by the usual sequence of many Coulomb explosions).

83 ately 0.2 bar (0.02 MPa) farther from static Coulomb failure and the rift segments approximately 0.2

84 ion of the seismic source and to compute the Coulomb Failure Function (CFF) variation on the aftersho

85 rusion and find that both would increase the Coulomb failure stress on possible SSE slip surfaces by

86 s before the earthquake, but changes in Mohr-Coulomb failure stress were probably too small to trigge

87 es a certain threshold, the resulting strong Coulomb field causes an unusual atomic collapse state; t

88 nsfer (CT) states that are stabilized by the Coulomb field of ions.

89 ugh the slits is determined by measuring the Coulomb field that it produces at large distances; under

90 al character of the proton in water and that Coulomb fields exerted by other cations, in particular d

91 variations of bonding lengths due to excess Coulomb force from bare ions at the dislocation core.

92 t the photon dispersion relation governs the Coulomb force, we obtain a fivefold-improved limit on an

93 uction force, and could be comparable to the Coulomb force.

94 Strong Coulomb forces are predicted to induce nucleation into a

95 These compete with long-range Coulomb forces associated with cationic and anionic side

96 e negatively charged DNA, reducing repulsive Coulomb forces between nucleotides and allowing the DNA

97 raction is van der Waals interactions and/or Coulomb forces in water, the van't Hoff enthalpy of the

98 nanomaterials are assumed to be governed by Coulomb forces, London dispersion, hydrogen-bond acidity

99 l) radical pair, being subject to attractive Coulomb forces, resides on the protein surface in the HE

100 gy and display exotic behaviour dominated by Coulomb forces.

101 orce field single-point partial charges with Coulomb formula.

102 face where forces are described by isotropic Coulomb friction.

103 nduced carrier correlations that lead to the Coulomb gap at EF, which we resolve experimentally in a

104 to previous reports of Luttinger liquids and Coulomb gap behaviour at low temperatures suggests that

105 omenon where wavefunction delocalization and Coulomb gap collapse are disrupted by doping-induced dis

106 ons, as observed in the analogous electrical Coulomb gas, like monopole dimerization, critical phase

107 We realize a model for 2D Coulomb glass as a cylindrical type II superconductor co

108 ng the salient features of the time-resolved Coulomb imaging experiment.

109 th the influence of scattering from screened Coulomb impurities.

110 narios for candidate quantum spin-liquids in Coulomb impurity lattices of various geometries.

111 We show that Coulomb impurity lattices on the surface of gapped honey

112 t positive carrier densities is dominated by Coulomb impurity scattering.

113 and valley degeneracies in the vicinity of a Coulomb impurity.

114 d, high-field terahertz pulses to reduce the Coulomb-induced potential barrier for carrier transport.

115 pores are driven to their maximum volume by Coulomb inflation.

116 e, complicating a priori identification of a Coulomb interacting surface.

117 tion originates from charge-transfer-induced Coulomb interaction among the gold, reactant, and reduci

118 rtant even at room temperature due to strong Coulomb interaction and a large exciton density of state

119 various novel properties, such as long-range Coulomb interaction and flat Landau levels.

120 rscore the importance of multi-band physics, Coulomb interaction and Hund's coupling that together ge

121 xtended Su-Schrieffer-Heeger model including Coulomb interaction and spin-flip effect.

122 s is determined by the interplay between the Coulomb interaction and the symmetries of the system.

123 ged particle systems is the screening of the Coulomb interaction between charge carriers.

124 wo-dimensional (2D) logarithmic character of Coulomb interaction between charges and the resulting lo

125 r the eigenvalues of the TM tau in which the Coulomb interaction between charges mimics the repulsion

126 e in a pK(a) was observed when the favorable Coulomb interaction between His121 and Glu75 was elimina

127 tionally explained in terms of the classical Coulomb interaction between spatially separated charged

128 motion, the two systems being coupled by the Coulomb interaction between the charges of the rotors (l

129 e at resonant illumination arises due to the Coulomb interaction between the electrons and holes in t

130 and demonstrate deterministic tuning of the Coulomb interaction between two ions, independently cont

131 onductors, these result principally from the Coulomb interaction between Wannier-Mott excitons.

132 rovement in performance is due to the strong Coulomb interaction between WS2 and MoS2 layers.

133 We show that in strong-coupling theory a Coulomb interaction can produce an order parameter in th

134 el, with resultant strong enhancement of the Coulomb interaction energy.

135 ting and may stimulate the use of long-range Coulomb interaction for coherent quantum control in othe

136 results highlight the key role played by the Coulomb interaction in the control and manipulation of o

137 The Coulomb interaction in the lowest-energy docking configu

138 states based on the unusual strength of the Coulomb interaction in these materials and its environme

139 e protein significantly because the apparent Coulomb interaction is sufficient to offset the dehydrat

140 (TMDs), reduced dielectric screening of the Coulomb interaction leads to strongly correlated many-bo

141 ndent mobility explains most results but the Coulomb interaction may play a role in shaping the fine

142 e implement such coupling through the mutual Coulomb interaction of two ions held in trapping potenti

143 eadily entangled with each other through the Coulomb interaction or remote photonic interconnects.

144 xcited from the valence band is bound by the Coulomb interaction to the hole it left behind.

145 The GGA plus on-site Coulomb interaction U (GGA + U) enhances the exchange sp

146 approximation formalism, taking into account Coulomb interaction U (LDA + U).

147 derstood regarding the role of their reduced Coulomb interaction U relative to their strongly correla

148 eans of sympathetic motional cooling through Coulomb interaction with a directly laser-cooled ensembl

149 s with enhanced masses, despite their strong Coulomb interaction with each other and the positive bac

150 cluding the collective plasmon modes via the Coulomb interaction, which opens up new pathways to mani

151 nduction is achieved from a charge frozen by Coulomb interaction.

152 ron-hole pairs into free charges against the Coulomb interaction.

153 y--via the Pauli exclusion principle and the Coulomb interaction.

154 current owing to the heavy screening of the Coulomb interaction.

155 ted charges that is based on their classical Coulomb interaction.

156 ults suggest that any qubit scheme employing Coulomb interactions (for example, encoded spin qubits o

157 ional lattice sum (Ewald-like) treatments of Coulomb interactions add significant overhead to compute

158 The long coherence times and strong Coulomb interactions afforded by trapped ion qubits have

159 a oxygen planes that enhances the unscreened Coulomb interactions among charges.

160 This is true despite the Coulomb interactions an electron experiences from the ho

161 complex that is stabilized predominantly by Coulomb interactions and depends on neither the sequence

162 s determined by a balance between attractive Coulomb interactions and loss of hydration but also modu

163 us factors such as dimensionality, topology, Coulomb interactions and symmetry.

164 charge-transfer states are strongly bound by Coulomb interactions and yet efficiently converted into

165 n the conduction band of graphene enabled by Coulomb interactions at the interface.

166 nt of organic semiconductors leads to strong Coulomb interactions between electron-hole pairs that sh

167 We demonstrate here, however, that Coulomb interactions between electrons in different laye

168 y, can be produced as the result of enhanced Coulomb interactions between electrons.

169 ong-range interactions in the form of either Coulomb interactions between ions or dipolar interaction

170 olar liquids decreases on heating, enhancing Coulomb interactions between ions.

171 s and subject to strong magnetic fields, the Coulomb interactions between them can become very strong

172 bital and/or spin orders arising from strong Coulomb interactions between transition metal and oxygen

173 Coulomb interactions break the degeneracy of the Landau

174 Strong, long-range Coulomb interactions can lead to correlated motions of m

175 However, the long range of the Coulomb interactions impedes the development of a simple

176 Strong Coulomb interactions in organic photovoltaic cells dicta

177 Spherical truncations of Coulomb interactions in standard models for water permit

178 t with the magnitude of medium to long-range Coulomb interactions in this protein.

179 sulators, and demonstrate that 2D long-range Coulomb interactions lead to peculiar size effects.

180 ion of single-particle effects and many-body Coulomb interactions lift the six-fold Landau level (LL)

181 superfluorescence (SF), which is enhanced by Coulomb interactions near the Fermi edge.

182 g the properties of a nonuniform system with Coulomb interactions onto those of a simpler system with

183 ed electrons and holes are strongly bound by Coulomb interactions or excitons, the photophysics of th

184 rged and polar systems, to which long-ranged Coulomb interactions typically make a large contribution

185 The Stoner approach perturbatively treats Coulomb interactions when the latter need to be large, w

186 able contributions from dehydration and from Coulomb interactions with surface carboxylic groups.

187 Coulomb interactions within the network report an effect

188 site spin exchange field, intra-atomic 4f-4f Coulomb interactions, and spin-orbit coupling.

189 he complex interplay between local polarity, Coulomb interactions, and structural reorganization as d

190 l charge and statistics, as well as modified Coulomb interactions, exist in a two-dimensional electro

191 lecules, held together by hydrogen bonds and Coulomb interactions, have attracted great interest beca

192 erate states at the Fermi energy, and strong Coulomb interactions, non-Fermi liquid behaviour is pred

193 transition in electronic liquids, driven by Coulomb interactions, represents a new class of strongly

194 itio anisotropic Eliashberg theory including Coulomb interactions, we investigate the electron-phonon

195 ntrol can be achieved by enhancing the local Coulomb interactions, which drive domain reorientation.

196 topological defects, and magnetic long-range Coulomb interactions.

197 tion of spin-orbit-driven band splitting and Coulomb interactions.

198 le on the electron acceptor side of PSII via Coulomb interactions.

199 ed mass renormalization driven by the strong Coulomb interactions.

200 y be highly correlated by strong, long-range Coulomb interactions.

201 values are governed by short-range polar and Coulomb interactions.

202 -ranged and slowly varying components of the Coulomb interactions.

203 l osmolytes may have on surface charging and Coulomb interactions.

204 semiconductors with strong light-matter and Coulomb interactions.

205 small intervalley scattering, and long-range Coulomb interactions.

206 ch forms a proximity-induced superconducting Coulomb island (a 'Majorana island') that is isolated fr

207 in EuS/Al/EuS heterostructures with metallic coulomb islands confined within a magnetic insulator bar

208 espond physically to infinite-range (a = 0), Coulomb-like (a = 1), monopole-dipole (a = 2) and dipole

209 of small metal nanoparticles is governed by Coulomb-like charging and equally spaced charge-transfer

210 ed larger amounts of H(ads) until reaching a coulomb limiting coverage close to 1 UPD monolayer of H(

211 brane metamaterials in which electromagnetic Coulomb, Lorentz and Ampere forces, as well as thermal s

212 to spin and charge instabilities, driven by Coulomb, magnetic, and lattice interactions.

213 be 0.052(2) Debye (1 Debye = 3.336 x 10(-30) coulomb-meters) for the triplet rovibrational ground sta

214 The classic Coulomb-Mohr failure criterion predicts the development

215 ructural information from the widely applied Coulomb momentum imaging method.The timescale of isomeri

216 chanisms developed recently one can name the Coulomb (near-field, dipolar) mechanism for nanostructur

217 resulting current is integrated to yield the coulomb number and hence the amount of analyte originall

218 ame charge, demonstrating that the resulting coulomb number may indeed be reduced for systems of limi

219 nstrate clear Coulomb staircase/blockade and Coulomb oscillations at room temperature and also at low

220 We argue that disorder-enhanced Coulomb pair-breaking (which usually destroys supercondu

221 The method is free of adjustable Coulomb parameters, and has no double counting issues in

222 ties such as pressure in systems of screened Coulomb particles to experimental measurements.

223 zoelectric coefficients (e(31,f) = -27 +/- 3 coulombs per square meter) and figures of merit for piez

224 hey form a highly unusual magnetic state--a "Coulomb phase"--whose excitations are point-like defects

225 may be cast as a prototypical theory of the Coulomb phase.

226 e and the spin liquid have been described as Coulomb phases, governed by an emergent gauge principle.

227 te Carlo method to investigate the effect of Coulomb potential and the nonadiabatic subcycle ionizati

228 harged and massless fermion in an attractive Coulomb potential as realized in graphene.When the conti

229 the electron wave packet is affected by the Coulomb potential as well as by the laser field.

230 tive that charges are free from their mutual Coulomb potential because we would expect rich vibration

231 ides a high dielectric environment where the Coulomb potential between charges is mitigated.

232 onadiabatic ionization is accounted for, and Coulomb potential can be neglected only in the tunnel io

233 uced tensile strain perturbations mimics the Coulomb potential in a mesoscopic atom.

234 concentration in each layer, changes in the Coulomb potential led to control of the gap between vale

235 molecular bonding originate from the central Coulomb potential of the atomic core.

236 a quantum phase transition in the attractive Coulomb potential of vacancies in graphene, and further

237 oseconds, mainly by electron escape from the Coulomb potential over a barrier that is lowered by the

238 der Waals interfaces is the poorly screened Coulomb potential that can give rise to bound electron-h

239 ically much softer radical with a low onsite Coulomb potential U.

240 arges exist in this material, interact via a Coulomb potential, and have measurable currents.

241 as testing the rotational invariance of the Coulomb potential.

242 massless Dirac fermion in an attractive 1/r Coulomb potential.

243 lan formula and using a value of 0.1 for the Coulomb pseudopotential, mu*.

244 o-step process is required to transfer nETqe coulombs (qe is the absolute value of the elemental elec

245 m a staggered ABAB stacking that reduces the Coulomb repulsion among the stripes.

246 Strong Coulomb repulsion and spin-orbit coupling are known to g

247 ionic repulsion to the Thomas-Fermi screened Coulomb repulsion and to the Born-Mayer valence electron

248 e layer to the next, at odds with any simple Coulomb repulsion argument.

249 Coulomb repulsion between adjacent ions is found to be t

250 aves can also be induced in solids by strong coulomb repulsion between carriers, and at the extreme l

251 parameter to account for the strong on-site Coulomb repulsion between Np 5f electrons.

252 , leads to a long range of the electrostatic Coulomb repulsion between platelets.

253 , dephosphorylated taus are separated due to Coulomb repulsion between similarly charged isoforms.

254 e of the mobile H2 layers is to decrease the Coulomb repulsion between the negatively charged hydroge

255 ible in organic semiconductor devices due to Coulomb repulsion between the two charges.

256 insulators are prevented from conducting by Coulomb repulsion between them.

257 decreasing pH and salt concentration, due to Coulomb repulsion by charged residues.

258 ng hard-sphere system (alphaBc) and screened Coulomb repulsion combined with short-range attraction (

259 riguing because both the lattice and on-site Coulomb repulsion contribute to the insulator-to-metal t

260 The strong intramolecular Coulomb repulsion in multiply charged anions (MCAs) crea

261 may be averted due to a screened long-range Coulomb repulsion intrinsic to disordered q1D materials.

262 In most unconventional superconductors, Coulomb repulsion is minimized through the formation of

263 band Hubbard model, in which the short-range Coulomb repulsion leads to a k-space differentiation bet

264 uggesting that the tremendous intramolecular Coulomb repulsion makes the [Py(SO(3))(4)](4-) anion ext

265 n spin-orbit coupling, bandwidth and on-site Coulomb repulsion stabilizes a J(eff) = 1/2 spin-orbital

266 s, where the insulating gap is driven by the Coulomb repulsion U on the transition-metal cation, and

267 s, a finding which heralds a reduced on-site Coulomb repulsion U.

268 surface-layer Mn, which is reduced by direct Coulomb repulsion when the As vacancy is moved nearby.

269 operties are comparatively unaffected by the Coulomb repulsion.

270 he point charges interact through a screened Coulomb repulsion.

271 the metallic bandwidth and U is the on-site Coulomb repulsion.

272 aired electrons minimize their strong mutual Coulomb repulsion.

273 ion charges to reduce the contributions from Coulomb repulsions, as well as from the cooling effect o

274 Comparisons with DFT calculations show that Coulomb's law overestimates the large unfavorable intera

275 While Coulomb's law predicts the size-dependent trend, it over

276 Coulomb's law reproduces the measured CSPs optimally wit

277 Contrary to the simple expectations from Coulomb's law, Weinhold proposed that anions can stabili

278 change in free energy (DeltaDeltaG(E)) using Coulomb's law.

279 Over 200 years after Coulomb's studies, a general connection between the mech

280 itions to the effects of charge-trapping and Coulomb scalability in memory nanodevices.

281 component of the polariton provides a finite Coulomb scattering cross section, such that the differen

282 Due to multiple Coulomb scattering inside the measured object it has sho

283 719 dye into TiO2 is dominated by long-range Coulomb screening of the final states of the excitonic t

284 , and instead induces a strongly fluctuating Coulomb spin liquid with defect-induced frozen magnetic

285 roscopy measurements on the particles show a Coulomb staircase that is correlated with the measured p

286 entials of the catalyst are evenly spaced (a Coulomb staircase), more consistent with bulk-like prope

287 We demonstrate clear Coulomb staircase/blockade and Coulomb oscillations at r

288 ree M >/= 3 foreshocks all produced positive Coulomb stress at the mainshock hypocenter.

289 red branching direction predicted by dynamic Coulomb stress calculations.

290 because they must fall in zones of positive Coulomb stress change.

291 c stress wavefield and find the peak dynamic Coulomb stress is similar on the rifts and transforms.

292 , moment deficit calculations and cumulative Coulomb stress transfer.

293 Static shear- and Coulomb-stress increases of 6 to 14 kilopascals from the

294 round state of a two-dimensional (2D) random Coulomb system with logarithmic interactions.

295 e ionic and molecular-dipolar state in dense Coulomb systems at near ambient conditions.

296 ysical, and spectroscopic properties of semi-Coulomb systems such as ionic liquids.

297 sfer of qstep1 (= nETqe/(1 + AOECOE/ARECRE)) coulombs; the second step is associated with the diffusi

298 m by which electrons and holes overcome this Coulomb trapping is still unsolved, but increasing evide

299 We found that Coulomb, van der Waals, charge-dipole, dipole-dipole, an

300 PEt3 ligands are shown to create an internal coulomb well that lifts the quantum states of the Ni9Te6