ライフサイエンスコーパス: charge density

1 parameter (molar mass, chemical composition, charge density, ...).

2 ectrum with incident illumination by varying charge density.

3 ures in which the resonance is linked to the charge density.

4 ssess them, including the electrode area and charge density.

5 with helical structure, hydrophobicity, and charge density.

6 tions between fluctuations in the electronic charge density.

7 e of merit that is the square of the surface charge density.

8 ed M(2+) cation sites with a higher apparent charge density.

9 resulting in an enhancement of the membrane charge density.

10 modulating interfacial chemistry rather than charge density.

11 impedance which is a function of the surface charge density.

12 n texture, which can be tuned by varying the charge density.

13 asing peak split corresponding to increasing charge density.

14 ntaining acidic lipids depending on negative charge density.

15 crease in lipid packing and membrane surface charge density.

16 rationally design composites based on local charge density.

17 efficiency are dictated by the triboelectric charge density.

18 n BOD-GO composite having different negative charge density.

19 ucture can be modulated under various doping charge densities.

20 due to the heterogeneity in nanotube surface charge densities.

21 ic semiconductors over the relevant range of charge densities.

22 time-dependent density functional transition charge densities.

23 ic stiffening of the polymer chains at large charge densities.

24 epulsive forces due to their higher negative charge densities.

25 ectron-rich RE metal ions and high localized charge density, a property arising from the proximal pos

26 proximately 40 nm cannot be charged at local charge densities above 1 muA cm(-2), and by implication,

27 g of a periodic modulation of the electronic charge density accompanied by a periodic distortion of t

28 ion of this polaron impedes equilibration of charge density across the nanowire and gives rise to dis

29 ty, thickness, lateral pressure profile, and charge density all play distinct roles in the kinetics o

30 ncurred to ionic radius and resultant cation charge density also provide reactivity with significant

31 Bonding and charge density analyses indicate delocalized bonding wit

32 in liposomes of opposite charges and varying charge densities and determined the resultant protein or

33 ction is finally presented, based on surface charge densities and electrode potentials.

34 II) (1), Fe(III) (2)), with almost identical charge densities and morphologies except for their diffe

35 indicate that as low as 26.7% Q(max), 34.0% charge density and 44.0% electromotility in OHCs were su

36 oted by one or more regions of high negative charge density and aromatic/hydrophobic residues that ar

37 membrane solubilization is promoted by a low charge density and by a relatively high fraction of male

38 l and amine can be used to tune the membrane charge density and control ion transport.

39 distribution and the dependence of the local charge density and electric field on the distance betwee

40 e effect of N-tert-butyl substitution on the charge density and electron density localization of the

41 ssure chemistry is rationalized by analyzing charge density and electron localization function distri

42 s the square of the polyelectrolyte's linear charge density and in proportion to the surfactant's hyd

43 ms for its toxicity due to the high positive charge density and non-degradability although the toxici

44 hesis, resulting in a controllable framework charge density and photocatalytic activity toward the se

45 such as all-optical methods to image valance charge density and reconstruct electronic band structure

46 rtificial spin ice arrays where the magnetic charge density and response to external fields can be st

47 generation of siRNA dendrimers due to a high charge density and structural flexibility.

48 -specific by a systematic relationship to PS charge density and substrate structure that is rooted in

49 The effects of alkyl chain length and charge density and the antimicrobial mechanisms for chlo

50 mixtures as a function of the polyion linear charge density and the surfactant hydrophobicity.

51 oncentration in the solution will affect the charge density and thereby may modulate the properties o

52 sed by the cell through resulting changes in charge density and/or mobile cation (and/or anion) conce

53 rum in the presence of thermally fluctuating charge-density and superconducting orders.

54 organic solvent drying speed, (ii) membrane charge density, and (iii) polyethylene glycol-conjugated

55 , total elementary charge movement (Q(max)), charge density, and electromotility intermediate between

56 Variation of the lanthanide ion modulates charge density, and ligand modification allows alteratio

57 nanoparticles, such as size, shape, surface charge, density, and porosity play a central role in bio

58 o Fe, with negative spin density and minimal charge density anisotropy.

59 In addition, the charge density applied in this study is of the order of

60 nsport behavior at the Dirac point where the charge density approaches zero.

61 These differences in local surface charge density are challenging to visualize, but recent

62 local electrical field built up by the high charge density around the aggregate-nanofiber interface,

63 embrane protein is modulated by the negative charge density around the protein.

64 opore can induce reversible negative surface charge densities as high as 1 C m(-2), and that the effe

65 eted to be driven by the decrease of surface charge density as well as potential mineral dissolution

66 nsight into the creation and manipulation of charge density at an oxide heterostructure interface and

67 gates to systematically modify local surface charge density at the interface between the nanochannel

68 model on the basis of the molecular size and charge density at the ionized nitrogen is used here as a

69 ranes, decreased lateral chain pressure, low charge density at the membrane surface, and increased sa

70 tal-olefin interactions induced by increased charge density at the metal site.

71 that the spatial distribution of the surface charge density at the nanopore wall and the resulting io

72 hts that materials can have widely different charge densities but also large variation in performance

73 oscale assemblies in terms of dimensions and charge densities but toward which DNA and heparin exhibi

74 composite having the same moderate negative charge density, but the highest kS of (79.4+/-4.6)s(-1)

75 rt a method for increasing the triboelectric charge density by coupling surface polarization from tri

76 nanochannel walls reduced the native surface charge density by up to approximately 4-5 times compared

77 The elevation of negative charge density caused by the presence of the risk factor

78 mine) and a small inorganic ligand with high charge density (ChaMs).

79 the C-terminal cluster reducing the positive-charge density completely abolished binding of R-LPS.

80 ainted with different quantities of the high charge-density contaminant is measured at a fixed total

81 ial response due to the presence of the high charge-density contaminant.

82 sed for detection and quantification of high charge-density contaminants in heparin.

83 Strong evidence for charge-density correlation in the underdoped phase of th

84 a in polarized (0001) plane and high surface charge density could promote higher Anti-C(ab) loading a

85 From topological analyses of experimental charge-density data, we show for the first time that the

86 lar to LAO/STO 2DEGs, we predict that the 1D charge density decays laterally within a few unit cells

87 singularities must decrease with increasing charge density demonstrating the ability to modify the e

88 The charge density dependence of the mobility of semiconduct

89 ation of biomolecules by probing the surface charge density dependence on the applied gate field.

90 pretation can be aided via an examination of charge density depletion across the molecular system.

91 ed parameters; association energies, partial charges, density descriptors as encompassed by the QTAIM

92 f membrane proteins and show how the surface charge density dictates the stability of folded states.

93 Density of states and charge density difference calculations reveal that stron

94 evenly charged polyelectrolytes by CGE, and charge density distribution of variously charged polyele

95 hod offers a possibility of directly probing charge-density distributions at interfaces between highl

96 PTFE acquire significantly different surface charge densities during contact with water, such a diffe

97 frameworks, which provide large net positive charge densities, excellent structural stability, and en

98 Charge density fluctuations can be measured with orders

99 donor sensitive to the Stark effect and thus charge density fluctuations in the CT state.

100 ned by accounting for the wavelike nature of charge density fluctuations.

101 plicate the hydrophobic surface and cationic charge density found among HDPs; the charge and hydropho

102 Measurement of charge density from an electroactive area may result in

103 al barrier by providing an increased surface charge density from the increased membrane surface and a

104 a technique for measuring the layer-resolved charge density, from which we directly determine the val

105 The nanoscale morphology and high charge densities give a high rate of electron-hole encou

106 on temperature, in particular at an induced charge density >5 x 10(12) cm(-2), and can reliably be d

107 mations predict that the variation in linear charge density has a minor effect on the extent of catio

108 ation capacity; however, their high cationic charge density has been shown to be cytotoxic.

109 nal groups on the nanopore wall, the surface charge density highly depends upon the proton concentrat

110 oteins reveal a common dependence on (i) net charge density, (ii) surface hydrophobicity, and (iii) t

111 The nanoscale morphology and high charge densities in organic photovoltaics (OPVs) lead to

112 c inhomogeneities in initial water and fixed charge densities in the cartilage using magnetic resonan

113 n by RO/NF membranes and (ii) measurement of charge density in active layers provides a valuable char

114 ule system: analyses based on intermolecular charge density in the absence of the tip fail to capture

115 acid sodium salt, AQ), through tuning of the charge density in the ligand shell of the QD, within an

116 The mobile charge density in the pili, as well as the temperature a

117 on due to imperfections, and measurements of charge density in the polyamide active layers of reverse

118 Our results reveal that the charge density in the region very close to the edges is

119 For the maximization of the surface charge density in triboelectric nanogenerators, a new me

120 er than that of 1, suggesting that the spin (charge) density in GEAn(+*) is more dispersed in GQ-1.

121 We propose that fixed charge-densities in the brain are involved in regulating

122 NPs with zero-to-low surface charge densities interact via a long-range attraction th

123 nced by efficient delocalization of cationic charge density into the five-membered imidazoline ring.

124 nfirmed by both experimental and theoretical charge density investigations.

125 The trapped charge density is correlated to the cell performance, an

126 ring these electrode properties and show the charge density is dependent on electrode geometry.

127 d basic residues are present and the overall charge density is low.

128 and an effective gate voltage from a surface charge density is proposed to describe biasing of V(g) a

129 ets greatly enhanced and its maximum surface charge density is systematically studied, which shows a

130 f surface plasmon resonance (SPR) on surface charge density is used to detect small molecules (60-120

131 counterparts of 2D materials, including high charge density, large surface area, remarkable electron

132 ction can provide a time-dependent record of charge-density maps with sub-cycle and atomic-scale reso

133 work supports growing evidence that surface charge density may be the driving force of virus capsid

134 Small changes in structure and charge density near a transition can tip the balance bet

135 The polarization charge densities of 73.7 and 119.0 microC cm(-2) are suc

136 into three regimes depending on the surface charge densities of the NPs.

137 constraint of air breakdown, a triboelectric charge density of 1003 microC m(-2), which is close to t

138 ability, water-resistance and a high surface charge density of 250 muC m(-2).

139 structural instability produced by the high charge density of a calcium binding site.

140 ami, which correlates with the variations in charge density of both origamis.

141 In order to identify an optimal charge density of GO for BOD-ErGO composite preparation,

142 on for others to consider the influence of a charge density of GO on direct bioelectrochemistry/bioel

143 sponse to the change of solvent polarity and charge density of individual macroions.

144 The high charge density of nucleic acids and resulting ion atmosp

145 extent of the aggregation is reliant on the charge density of polymer, which is equivalent to dCO2 c

146 gree of AuNP aggregation is dependent on the charge density of polymer, which is related to dCO2 conc

147 EGFC promoted HA synthesis and increased the charge density of synthesized GAGs.

148 The higher charge density of the assembly, a result of the folding

149 n the ARMs of the excess CP and the negative charge density of the capsid exterior.

150 or insertion of excess PtdSer increases the charge density of the inner leaflet, generating foci of

151 ese differences were attributed to the lower charge density of the KC (US) as a result of sonochemica

152 However, the varying charge density of the linking blocks greatly affects the

153 , which leads to an increase in the negative charge density of the membrane due to the formation of c

154 c in nature and are dependent on the anionic charge density of the membrane surface.

155 ic manner that is dependent upon the anionic charge density of the membrane.

156 y confounded because the ligands perturb the charge density of the metallic core, inducing Lewis acid

157 the Gouy-Chapman model, the initial surface charge density of the mica surface was determined to be

158 is proportional to the concentration and the charge density of the polyanions.

159 sponse of polyions increases with increasing charge density of the polyions.

160 layer adsorption is a direct function of the charge density of the second layer.

161 tection, where molecular binding changes the charge density of the sensor and leads to sensing signal

162 mediates result from the net increase in the charge density of the substrate-cofactor pi-bonding netw

163 Here, we measure the fixed charge density of the TM and show that this density of f

164 A simple way to express surface charge density of these particular GO nanosheets was dev

165 Ps are in their oxidized state, but the high charge density of this state is detrimental for the prev

166 Local variations in charge density on an electrode surface are manifest in a

167 ptamer to the protein results in a change in charge density on the bead surface, the isoelectric poin

168 influence on activation mediated by electric charge density on the extracellular and intracellular me

169 Instead, they result from the surface charge density on the glass surface and the resulting el

170 new approach to visualize and quantify fixed charge-densities on brain slices using a focused proton-

171 The use of surface plasmons, charge density oscillations of conduction electrons of m

172 face-bound solvent ions produces long-ranged charge-density oscillations in the molten salt around so

173 rication of electrode coatings with improved charge densities over a typical (Ru,Ir)O2 catalyst.

174 The charge densities over the surface with mixed oxidized an

175 Upon intercalation, a charge density per graphene layer of 5 10(13) +/- 5 10(1

176 In these devices, a charge-density plasma wave is excited by an ultra-relati

177 High charge-density polyanion contaminants and impurities in

178 ed chondroitin sulfate (OSCS) and other high charge-density polyanions that could potentially be used

179 Owing to their high negative charge density, PP-InsP(y) will not cross the cell membr

180 g product ion yield by nearly 4-fold for low charge density precursors.

181 in relation to the overall structure and the charge density profile of the two biopolymers.

182 The oxide charge density (q(ox)) is determined for both the format

183 nonlinearly related to the biochar's surface charge density (r(2) = 0.94) while electrostatic repulsi

184 for studying bonding, based on the electron-charge density, rather than a conventional atomic pair-c

185 6% and 3% (99% overall) of the total induced charge density reside within the four innermost layers,

186 isible enhancement in the nonlocality of the charge density response in the range of 10 to 20 nanomet

187 ly protected surface state creates a surface charge density similar to a plasmon in a metallic nanopa

188 r relationship between mobility and electron charge density, similar to field-effect induced changes

189 reaction correlate with the nitronyl carbon charge density, suggesting a nucleophilic nature of O2(*

190 phosphomimetic M2-1 variant revealed altered charge density surrounding this flexible region although

191 that release up to three times more electric charge density than that produced by PbZr0.52Ti0.48O3 (P

192 the design of spin textures with topological charge densities that can be tailored at ambient tempera

193 hange was limited by the maximum interfacial charge density that could be attained before dielectric

194 ng that ascribes to the polymer an effective charge density that is independent of force and salt.

195 Together with the decreased charge density, the AMPs exhibited inhibited toxicity ag

196 c doping is in terms of modifications of the charge density to screen the electric field generated at

197 en metal sites and proximal highly localized charge density toward materials with enhanced CO2 sorpti

198 le highest occupied molecular orbital (HOMO) charge density toward the cation with a subsequent elect

199 asmonic and photonic applications due to its charge-density tunability, high electron mobility, optic

200 CV profiles are integrated to determine the charge density values for oxide reduction (q(ox,red,CV))

201 scattering, which reports on correlations in charge density variations, must be measured.

202 xp are determined by analyzing the slopes of charge density versus Deltaf plots for the Ag electrodep

203 ids with significantly increased dissociated charge densities via judiciously balancing ion pair inte

204 In plasma wakefield acceleration, a charge-density wake with high accelerating fields is dri

205 The charge density was varied at the interface by changing t

206 ty, emulsifying properties and electrostatic charge density, water holding and fat absorption capacit

207 compound, Pb3-xSb1+xS4Te2-delta, that has a charge density wave (CDW) at room temperature.

208 Charge density wave (CDW) correlations have been shown t

209 Charge density wave (CDW) formation, a key physics issue

210 e we report an X-ray study of the high-field charge density wave (CDW) in YBCO.

211 Charge density wave (CDW) order appears throughout the u

212 e authors identify the emergence of a unique charge density wave (CDW) order in monolayer TiTe2 that

213 ncy to short-range-correlated incommensurate charge density wave (CDW) order is "intertwined" with th

214 etition occurs between superconductivity and charge density wave (CDW) order.

215 Recently, it has become clear that a charge density wave (CDW) phase exists within the pseudo

216 viously and with the interpretation that the charge density wave (CDW) reduces Hc2 in underdoped YBa2

217 The electronic structure of a charge density wave (CDW) system PrTe3 and its modulated

218 etal-"insulator" crossover is not due to the charge density wave (CDW) that was thought, and the natu

219 We show that single-layer TiSe2 exhibits a charge density wave (CDW) transition at critical tempera

220 Recently, charge density wave (CDW) was found below the supercondu

221 Charge density wave (CDW), the periodic modulation of th

222 ting properties of superconductivity and the charge density wave (CDW).

223 perature, which is attributed to an apparent charge density wave (CDW).

224 = 4.1196(1) A; c = 8.0951(2) A], exhibits a charge density wave (CDW)/spin density wave (SDW) transi

225 endency towards transient stabilization of a charge density wave after near-infrared excitation, coun

226 Both the charge density wave and the superconducting phase have b

227 reduction of electron correlation due to the charge density wave decoherence.

228 This alternative proposal for charge density wave formation may be of general relevanc

229 prevailing thinking about the mechanisms of charge density wave formation.Due to reduced dimensional

230 superconductors, magnetic domain walls, and charge density wave materials.

231 es, molecular structures, organic salts, and charge density wave materials.

232 ory has long predicted an interaction-driven charge density wave or Wigner crystal state.

233 copy, we observed the emergence of a (2 x 2) charge density wave order in single-layer TiTe2 with a t

234 ith irregularly textured domain walls in the charge density wave order inherent to this Mott state.

235 The charge density wave order is manifested by periodic dist

236 a superconducting dome in the proximity of a charge density wave phase.

237 e the role of disorder on the pseudo-gap and charge density wave phases of underdoped cuprates.

238 The unique charge density wave phenomenon in the single layer raise

239 election of the ordering vector in the model charge density wave system ErTe(3).

240 The one-dimensional nature is evident from a charge density wave transition, whose periodicity is giv

241 Surprisingly, no charge density wave transitions were observed in two-lay

242 he smectic order is treated as an electronic charge density wave with an associated Peierls distortio

243 onsistent with Ginzburg-Landau theory when a charge density wave with d-symmetry form factor and wave

244 ng of these results indicates that a biaxial charge density wave within each CuO2 plane is responsibl

245 tructure distortion is not associated with a charge density wave, but is rather associated with Te p-

246 However, we detect a subtle charge density wave-like Fermi surface instability in me

247 relaxation dynamics of an initially prepared charge density wave.

248 transition metal dichaclogenide which has a charge- density wave transition that has been well studi

249 e of interest for studying phenomena such as charge-density wave (CDW) and superconductivity.

250 a previously unknown unidirectional (stripe) charge-density wave (CDW) smoothly interfacing with the

251 A charge-density wave (CDW) state has a broken symmetry de

252 ayered compound exhibiting an incommensurate charge-density wave (CDW).

253 Here we show that a model of competing charge-density wave and superconducting orders provides

254 perature far exceeds the critical value, the charge-density wave is preserved until the lattice is su

255 In the case of the charge-density wave material 1T-TiSe2, our data indicate

256 cs in the Brillouin zone, X-ray detection of charge-density wave order at intermediate temperatures a

257 and superconductivity emerges in a textured charge-density wave state induced by ionic gating.

258 ds, with superconductivity developing from a charge-density wave state.

259 We find that the charge-density wave states in 1T-TaS2 collapse in the tw

260 matically change with nanoarchitecture and a charge-density wave-like transition is observed.

261 the spatial distribution of both short-range charge-density-wave 'puddles' (domains with only a few w

262 Recently, 3D charge-density-wave (CDW) formation with long-range orde

263 2H-NbSe(2) is a canonical Charge-Density-Wave (CDW) layered material the structura

264 Recent theories of charge-density-wave (CDW) order in high-temperature supe

265 ground states, such as antiferromagnetism or charge-density-wave (CDW) order.

266 Mott-insulating ground state with a peculiar charge-density-wave (CDW) order.

267 The charge-density-wave (CDW) phase is a macroscopic quantum

268 for YBa2Cu3O(6+delta), which indicates that charge-density-wave correlations are universally respons

269 Here we report the observation of charge-density-wave correlations in the model cuprate su

270 s accompanied by the disruption of competing charge-density-wave correlations, which explained some b

271 omains are spatially anticorrelated with the charge-density-wave domains, because higher doping does

272 t al. report that the domain wall state in a charge-density-wave insulator 1T-TaS2 decomposes into tw

273 c states localized on domain walls in a Mott-charge-density-wave insulator 1T-TaS2 using scanning tun

274 e interactions between electrons and ions in charge-density-wave materials, and should be germane acr

275 erconducting state coexists with short-range charge-density-wave order and quenched disorder arising

276 t with a Fermi-surface reconstruction by the charge-density-wave order observed in YBa2Cu3Oy, provide

277 ciated with Fermi-surface reconstruction and charge-density-wave order-is a key limiting factor in th

278 use higher doping does not favour the stripy charge-density-wave puddles, leading to a complex emerge

279 We found that the charge-density-wave puddles, like the steam bubbles in b

280 erconducting and commensurate/incommensurate charge-density-wave states in the phase diagram.

281 the layer thickness, but the newly observed charge-density-wave transition temperature increases fro

282 or cooperation between superconductivity and charge density waves (CDWs) in the transition metal dich

283 spin, with a locked periodicity, others host charge density waves (CDWs) without any obviously relate

284 y of holes scattered by the short-wavelength charge density waves decreases.

285 Such highly unusual enhancement of charge density waves in atomically thin samples can be u

286 ivity and electronic orders, such as spin or charge density waves, have been a central issue in high

287 o-dimensional quantum matter phases, such as charge density waves, spin density waves and superconduc

288 ample correlated materials with rich phases (charge density waves, superconductivity, hard ferromagne

289 we identified the Peierls origin of multiple charge-density waves in a three-dimensional system for t

290 metal, possible Mott insulators with tunable charge-density waves, and topological semimetals with ed

291 wettability, surface potential, and surface charge density were compared before and after plasma tre

292 as the temperature and pH dependence of the charge density, were similar to those of carbon nanotube

293 into a toroidal pore with an overall reduced charge density, which could explain the mechanism of syn

294 ution and net amount of pericellularly fixed charge-densities, which, determined at 0.4-0.5 M, is muc

295 erage for cross-linked m/z species with high charge density, while HCD was optimal for all others.

296 ), the periodic modulation of the electronic charge density, will open a gap on the Fermi surface tha

297 tive detection of molecules with low surface charge density with 97.6% detection accuracy compared to

298 d at least 5 million pulses at 0.45 mC/cm(2) charge density with less than 7.5% impedance change, whi

299 dy the correlation of the particles' surface charge density with their translocation time and verify

300 graphene can be used to optically determine charge density, with decreasing peak split corresponding