ライフサイエンスコーパス: charge density

1 ique chemical recognition of anions with low charge density.

2 with helical structure, hydrophobicity, and charge density.

3 tions between fluctuations in the electronic charge density.

4 asing peak split corresponding to increasing charge density.

5 crease in lipid packing and membrane surface charge density.

6 rationally design composites based on local charge density.

7 efficiency are dictated by the triboelectric charge density.

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

9 TENG are established to enhance and evaluate charge density.

10 ectrum with incident illumination by varying charge density.

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

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

13 molecules can be used to reveal the surface charge density.

14 um-mechanical fluctuations in the electronic charge density.

15 ize eluting peptides based on their size and charge density.

16 the eluting peptides based on their mass and charge density.

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

18 epulsive forces due to their higher negative charge densities.

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

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

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

22 nd density of dipolar, ionic activation (ie, charge density) across the myocardium to guide ablation

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

24 tion on grain surfaces modulates the surface charge density among neighboring quantum wells.

25 For this purpose, electron charge density analysis, impedance spectroscopy, density

26 From the matrix of their triboelectric charge densities and band structures, it is found that t

27 d sulphated polymers with different negative charge densities and resultant structure-property-activi

28 charge densities, variations in the spatial charge densities and the atom- and orbital-projected den

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

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

31 The charge density and divergence of the beam at the sample

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

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

34 leading to analytical formulas for the space charge density and impedance of the system for two paral

35 Charge density and molecular coverage on the surface of

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

37 correlations fall off exponentially, whereas charge density and spin density modulations are dominant

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

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

40 xtent of neutralization of a reflectin's net charge density and the size of resulting multimeric prot

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

42 )imide (BmimNTf(2)) as a function of surface charge density and thickness were investigated using two

43 s to highly luminescent films by controlling charge density and transfer in novel device structures.

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

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

46 el that considers nanopore geometry, surface charge density, and electrolyte concentration calculates

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

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

49 e hierarchical structures at pH values where charge densities are high.

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

51 hnical challenge, since anions with a higher charge density are often preferentially sorbed by tradit

52 re in these insulators is instead fractional charge density arising from filled bulk bands, but measu

53 We tested charge density as a translocase determinant and confirme

54 In this study, we have evaluated length and charge density as translocase determinants using model p

55 These models showed that negative charge density associated with tetrahedral sites results

56 Sn}-S bonding interactions and increases the charge density associated with the S(2-) ions.

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

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

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

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

61 Proteins that have the highest positive charge density at their C-terminus are overwhelmingly ri

62 leading to a situation where the protein net-charge density balances the attractive dispersion force

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

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

65 ate, an anionic polysaccharide with the same charge density but no specific transmembrane receptors.

66 electrostatic fields that reflect the local charge density, but imaging this with single atom sensit

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

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

69 s presented to enhance its effective surface charge density by increasing the efficiency of contact e

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

71 This negative fixed charge density can also be used for enhancing intra-NP r

72 change in cytoplasmic ion concentrations and charge density can alter location and enzymatic function

73 Meanwhile, its effective charge density can be further improved as the device siz

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

75 roporous and gellular structure, showed that charge density (CD) was the most important characteristi

76 taneous measurements of the surface mass and charge density changes in real time.

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

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

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

80 rovides a real-space image of the multipoint charge-density correlation functions, which reveal snaps

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

82 anes over fourfold, suggesting that interior charge density could be an important tool to enhance the

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

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

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

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

87 ted by means of experimental and theoretical charge density determination to elucidate the nature of

88 Further, the calculated charge density distribution and density of states provid

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

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

91 NP has a high negative fixed charge density due to the presence of negatively charged

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

93 ing the mass uptake and evolution of surface charge density during polyelectrolyte multilayer formati

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

95 ctions with the tissue's high negative fixed charge density (FCD) for delivering small molecule drugs

96 ge proteoglycans, the source of tissue fixed charge density (FCD).

97 Charge density fluctuations can be measured with orders

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

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

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

101 is extreme rigidity in combination with high charge density gives insight into the self-assembly of m

102 or harvesting mechanical energy, low surface charge density greatly hinders the practical application

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

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

105 emapped to guide each subsequent ablation of charge density-identified targets.

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

107 Our charge-density imaging method advances electron microsco

108 The distribution of charge density in materials dictates their chemical bond

109 h the four-point correlation function of the charge density in momentum space.

110 It remains a challenge to resolve charge density in nanostructures and functional material

111 ntally measure boundary-localized fractional charge density in rotationally symmetric two-dimensional

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

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

114 ionized water and PTFE can produce a surface charges density in the scale of 1 nC cm(-2) , which is t

115 is found to decrease with increasing surface charge density, indicative of a negative differential ca

116 tching current on the operating temperature, charge density, input power and frequency shows a noise-

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

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

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

120 The normalized triboelectric charge density is derived to reveal the intrinsic charac

121 As the charge density is increased, the IL dynamics become slow

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

123 The charge density is nearly two orders of magnitude higher

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

125 Surface charge density is the key factor for developing high per

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

127 Built from an unusual high-charge-density ligand 2,5-dioxido-1,4-benzenedicarboxyla

128 As a result of the high surface-charge density, ligand binding to this protein is allost

129 eptor affinity, metal nanoparticles with the charge density lower than receptor biomolecules can redu

130 onclusions This novel ultrasound imaging and charge density mapping system safely guided ablation of

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

132 The charge density mismatch concept was applied to the synth

133 ft due to O bonds), because valence electron charge density moves toward electronegative O atoms in t

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

135 r Fe(iii) removal and it was summarized that charge densities of functional groups, produced zeta-pot

136 hod, this study quantifies the triboelectric charge densities of nearly 30 inorganic nonmetallic mate

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

138 electron doping mechanism in SWCNTs up to a charge density of -18 me/C, far beyond that achievable b

139 sed on the mechanism, an ultrahigh projected charge density of 1.85 mC m(-2) is obtained in ambient c

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

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

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

143 wing to the abundance of Al sources and high charge density of Al(3+).

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

145 Indirectly measuring the charge density of bulk materials is possible through X-r

146 from the root, has a fairly uniform negative charge density of ca. -15 mC/cm(-2) (in pH 6.8 aqueous s

147 ng technique that can directly map the local charge density of crystalline materials with sub-angstro

148 t all ionic strengths because of the greater charge density of dsDNA.

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

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

151 is able to detect differences in the surface charge density of hair at different distances from the r

152 e effect of systemically varying the anionic charge density of nanoparticles on their occlusion effic

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

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

155 By increasing the surface charge density of pore surfaces, current-rectification r

156 C gels is achieved by genetically tuning the charge density of protein backbones.

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

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

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

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

161 e of the FG-TENG is due to the high positive charge density of the regenerated cellulose.

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

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

164 The charge density of the surface (number of positively char

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

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

167 technology, the enhancement of triboelectric charge density of triboelectric nanogenerator (TENG) is

168 Thus, the MDC-TENG achieves a record high charge density of ~5.4 mC m(-2), which is over 2-fold th

169 ramework, the relationships between reaction charge density (OH(-) /H(3) PO(4) ), alkali and organoam

170 dge of the corresponding surface (and space) charge densities on the electrodes.

171 he IL films can be achieved by adjusting the charge density on substrates through multilayer network

172 cy buffer against the accumulation of excess charge density on the metals by partially redistributing

173 anogenerators is limited by low and unstable charge density on tribo-layers.

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

175 ding its size, height, geometry, and surface charge density or distribution, are removed while allowi

176 )PMo(12)O(40) (PMo), i.e. changing the POM's charge density or polarizability in order to get deeper

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

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

179 logical-Hall resistivity and the topological-charge density, our quantitative analysis shows much lar

180 This work also reveals the actual charge density (over 4.0 mC m(-2)) in a TENG electrode b

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

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

183 High charge-density polyanion contaminants and impurities in

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

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

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

187 lecular configurations in thin crystals from charge density projections, and uncovers the structures

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

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

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

191 6% and 3% (99% overall) of the total induced charge density reside within the four innermost layers,

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

193 irectly measures the total amount of surface charge density resulted from molecules near the surface

194 f 1-butene selectivity is traced to the high charge density retained by the M(2+) metal centers expos

195 ometric interfaces, while the DFT-calculated charge density reveals no charge transfer/accumulation a

196 electrostatic interactions between the high charge-density saccharide residues flanking the "canonic

197 concept was applied to the synthesis of high-charge-density silicoaluminophosphate SAPO-69 (OFF) and

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

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

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

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

202 The higher charge density (the increasing ionic strength) that acco

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

204 mers, the absence of a chromophore, the high charge density, the low abundance, and the instability o

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

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

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

208 A high average charge density up to 2.38 mC m(-2) is achieved using the

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

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

211 i- and C-dominated energy bands, the spatial charge densities, variations in the spatial charge densi

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

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

214 ed materials with phase transitions, such as charge density wave (CDW) and magnetic and dipole orderi

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

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

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

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

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

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

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

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

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

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

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

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

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

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

229 Although routinely labeled a charge density wave (CDW), this DW state could actually

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

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

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

233 Monolayer VSe(2) , featuring both charge density wave and magnetism phenomena, represents

234 cate interplay between superconductivity and charge density wave and spin density wave orders tunable

235 ry liquid with power-law superconducting and charge density wave correlations associated with half-fi

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

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

238 The charge density wave in the high-temperature superconduct

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

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

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

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

243 The charge density wave order is manifested by periodic dist

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

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

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

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

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

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

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

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

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

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

254 However, this axionic charge-density wave has not yet been experimentally dete

255 s predicted to arise from the formation of a charge-density wave in a Weyl semimetal(1,2)-that is, a

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

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

260 t with the anomalous transport of an axionic charge-density wave. Our results show that it is possibl

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

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

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

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

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

268 around the temperature at which short-range charge-density-wave formation occurs.

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

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

271 ed RIXS measurement at the Ti L(3)-edge on a charge-density-wave material TiSe(2).

272 Vestigial states due to primary spin and charge-density-wave order have been discussed in iron-ba

273 ng relationship between diagonal nematic and charge-density-wave order in HgBa(2)CuO(4+delta).

274 of order, such as antiferromagnetism(5-7) or charge-density-wave order(8), that might themselves be r

275 The accompanying sliding mode in the charge-density-wave phase-the phason-is an axion(3,4) an

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

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

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

279 agnetoconductance in the sliding mode of the charge-density-wave Weyl semimetal (TaSe(4))(2)I for col

280 Charge density waves (CDWs) in the cuprate high-temperat

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

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

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

284 ysical and chemical properties, ranging from charge density waves to superconductivity and electroche

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

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

287 range from generalized Wigner crystals(7) to charge density waves.

288 With the discovery of charge-density waves (CDWs) in most members of the cupra

289 formed pairs and to competing orders such as charge-density waves(1-4).

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

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

292 rospective technical approach to improve the charge density, which could push the output performance

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

294 such as batteries, as the electrode surface charge density will influence properties like diffusion

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

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

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

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

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

300 s of such nanoparticles with tunable anionic charge density within the stabilizer chains, which are p