ライフサイエンスコーパス: charge

1 behave as if they carry an electric/magnetic charge.

2 e sequence: fold propensity, and net segment charge.

3 their sources, for example strain or surface charge.

4 sly accomplished using the G-band shift with charge.

5 -liquid interface depending on their surface charge.

6 ection method for transmitters with positive charge.

7 lity to stabilize both negative and positive charges.

8 ibility, that is, its ability to accommodate charges.

9 logues with an increasing number of positive charges.

10 missed intra-abdominal injuries; or hospital charges.

11 ermolecular contacts via their complementary charges.

12 es the unscreened Coulomb interactions among charges.

13 lity due to low extraction of photogenerated charges.

14 erials to investigate light-assisted battery charging.

15 In charge, a portion of Cu metal is oxidized to CuO, which

16 fold increase in ATP:ADP, ATP:AMP and energy charge after portal venous reperfusion, respectively.

17 These results show that interactions between charged amino acid residues are important both to direct

18 etween negatively charged DNA and positively charged amino acid residues, the translocation speed of

19 of ions adsorbed on the graphene as well as charged amino acids associated with the immobilized prot

20 ded at the C terminus (POmega) and contained charged amino acids not more than 3 residues after the a

21 Although positively charged amino acids result in the Tyr-84 swing, amino ac

22 pH strongly affected sorption as negatively charged analytes were attracted by the positively charge

23 Lipopolysaccharide (LPS) surface charge and aggregation were unaltered in the presence of

24 Comparison between the measured surface charge and Gouy-Chapman-Stern model for the silica surfa

25 ntum gate operations, but also for classical charge and information transfer processes.

26 accounts for both the graphene polarization charge and ionic screening of ions adsorbed on the graph

27 enome-wide DNAm profiles in individuals with CHARGE and Kabuki syndromes with CHD7(LOF) or KMT2D(LOF)

28 mogeneous magnetic fields, but interact with charge and spin currents, allowing this moment to be man

29 While some systems exhibit stripes of charge and spin, with a locked periodicity, others host

30 tions were used to determine if the positive charge and susceptibility to posttranslational modificat

31 pectrum analyzer, where both the topological charge and the state of polarization of an input vector

32 eptide pore formation and both lipid-peptide charge and topological interactions.

33 binding domain (LBD) via a mix of positively charged and hydrogen-bonding interactions.

34 he dynamics of relaxation of photo-generated charges and in energetic distribution, is similar to the

35 roteins by neutralizing unfavorable positive charges and thus facilitate their transports.

36 h greater pyrolysis temperature due to lower charging and discharging capacities, although the chargi

37 ing and discharging capacities, although the charging and discharging kinetics remain unchanged.

38 ion mechanisms for inorganic ions by steric, charge, and dielectric exclusion.

39 rged linker DNA because it has a reduced net charge, and in DNA binding and protein-protein interacti

40 important properties such as particle size, charge, and solubility.

41 Nucleic acids are strongly negatively charged, and thus electrostatic interactions-screened by

42 as pore radius, half cone angle, and surface charges are systematically studied in the simulation tha

43 (often with a few counterions to compensate charges) are known now.

44 more modest contribution from the positively charged Arg-1119 in the extracellular pore region in rep

45 on membranes were studied along with surface charge at different electrolyte composition and effectiv

46 Surface charges at the inner leaflet of the plasma membrane may

47 The negatively charged backbone balanced with extra-framework cations a

48 Cationic AMPs bind negatively charged bacteria to exert their antimicrobial activity.

49 allows increased interaction with negatively charged bacterial membranes.

50 of the high-frequency (HF) train of biphasic charge-balanced pulses used by the standard HF deep brai

51 ower footprint area compared to conventional charge-based devices have made spin waves or magnon spin

52 e intercalation is driven by the exchange of charge between the host [Co6Te8(P(n)Pr3)6][C60]3 and the

53 ivery was relatively independent of size and charge but did depend on conformation, with regular, sph

54 and unlikely to be affected by the negative charge by K65 acetylation.

55 verlap distance complements computed partial charges by measuring the size of orbital lobes that best

56 Using pre-steady-state charge (calcium) translocation and steady-state ATPase a

57 at enables both greatly enlarged trapped ion charge capacities and also efficient ion population comp

58 nd, at a charge rate of 30 mA g(-1), exhibit charge capacities of about 120 mA h g(-1).

59 approximately 4.2 V vs Na/Na(+) ) with high charge capacity (190 mAh g(-1) ).

60 Charge carrier dynamics in amorphous semiconductors has

61 The charge carrier lifetime increased upon reversing the app

62 Using this method, the charge carrier mobility of C8 -benzothieno[3,2-b]benzoth

63 and/or providing type- and energy-dependent charge carrier scattering.

64 cal Hall effect, permits here measurement of charge carrier type, density, and mobility in epitaxial

65 The charge-carrier mobility of organic semiconducting polyme

66 toresponse due to the different photoexcited-charge-carrier trapping times in sp(2) and sp(3) nanodom

67 Understanding the nature of charge carriers in nanoscale titanium dioxide is importa

68 2) domains, and the trapping of photoexcited charge carriers in the localized states in sp(3) domains

69 tielectron system, utilizing molecular based charge carriers, made from inexpensive, abundant, and su

70 the preferential localization of more highly charged cations to the inner shell of the ion atmosphere

71 This is especially concerning for positively charged CDR mutations that are linked to antibody polysp

72 he former being stronger due to the positive charge centralized on the pyridyl nitrogen, N-H(+).

73 gained high MK2i-loading efficiency through charge-charge interaction, and 2) this depot platform en

74 ts several hydrophobic contacts and a strong charge clamp at the interface between these partners.

75 an alpha clamp, a phenylalanine clamp, and a charge clamp.

76 Positively charged coatings using direct attachment and formation o

77 We fabricate charge collection narrowing photodetectors based on four

78 photocurrent methods that require efficient charge collection.

79 des a novel, alternative approach to trapped-charge dating based on direct, non-destructive probing o

80 peed of DNA can be manipulated by deliberate charge decorations inside the nanopore.

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

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

83 Charge density fluctuations can be measured with orders

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

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

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

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

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

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

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

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

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

93 the three lowest-order multipoles-the total charge, dipole, and quadrupole moment-we show that the v

94 ce in terms of discharged energy density and charge-discharge efficiency is achieved in the PEI sandw

95 ode has a 90.0% capacity retention after 400 charge/discharge cycles and a capacity of 1.2 mAh/cm(2)

96 ifold advantages of high power density, fast charging-discharging, and long cyclic stability.

97 ipation flow of electronic spins with no net charge displacement.

98 ta function may be due to differences in CTD charge distribution and differential alignment of the CT

99 radii for cations with spherically symmetric charge distribution is obtained by charge-weighted avera

100 The electronic structure and charge distribution of this molecule resemble those of M

101 nuclein (betaS) aggregation via altering its charge distribution, thus opening new possible roles for

102 ntage of the interactions between negatively charged DNA and positively charged amino acid residues,

103 The charged droplet consists of approximately 2400 water mol

104 eam of gas-enriched spray with small, highly charged droplets and ions and directing it toward the MS

105 ), polarizable models (e.g., the fluctuating charge, Drude oscillator, and the induced dipole models)

106 in the Kondo regime, we uncover directly the charge dynamics of this peculiar mechanism of electron t

107 ng the reversibility of the photoresponse to charging effects.

108 distributions in the electric fields of the charged electrode.

109 Our approach combines charged excitations carried by strings, with topological

110 nt on size exclusion and the contribution of charge exclusion is weak.

111 act CRY2 homo-oligomerization, with positive charges facilitating oligomerization and negative charge

112 binding energy from delocalized, collective charge fluctuations-in contrast to complexes with other

113 genuine effects of molecular orientation on charge generation and recombination.

114 independently sustain appreciable long-lived charge generation.

115 hese flakes by SPS promoted the formation of charged grain boundaries, which led to the enhanced TE p

116 physiological ligand, because the negatively charged hyaluronan shows enhanced affinity for YKL-40 ov

117 membranes was found to increase the surface charge, hydrophilicity (by 20%), porosity (by 77%) and p

118 Moreover, two C-terminal charges impact CRY2 homo-oligomerization, with positive

119 ng single-walled carbon nanotube nested in a charged, impermeable covalent functional shell, Tube(wed

120 This transfer causes charge in-neutrality in the GONR which is compensated by

121 quantitatively control the total ionization charges in mass spectrometry.

122 exotic excitations, for example the magnetic charges in spin ices, also called monopoles.

123 The role of space charges in stabilizing polarization gradients is also di

124 yr-84 swing, amino acids that are negatively charged induce a not previously described Lys-146 lift.

125 es facilitating oligomerization and negative charges inhibiting it.

126 on to energetics, controlled electrochemical charge injection experiments in the nonsolvent electroly

127 e system to the logic high level due to self-charge injection into the redox active polymeric system.

128 of intercalating ion determines whether the charge injection is fully reversible (for Li(+)) or lead

129 he nanoscale and direct interaction with the charged interfaces produce anomalous sub-diffusion, due

130 tions with dicarboxylate anions are shown to charge-invert the positively charged phospholipids to th

131 collisional cross-section of single multiply charged ions can be obtained from these CDMS measurement

132 rface shows that the modification of surface charge is 4 times too large to be explained by the chang

133 a spin order is destroyed, while the role of charge is less known.

134 At higher NOM-to-DNP ratios, DNP charge is reversed, and DNP aggregates remain stable in

135 Mobility of charges is a quintessential property in this aspect; how

136 ngle-electron (SE) pump with a semiconductor charge island is promising for a future quantum current

137 n Cd2Os2O7 and that it exhibits complex spin-charge-lattice coupling.

138 is less effective in neutralizing negatively charged linker DNA because it has a reduced net charge,

139 EIEIO involves irradiating singly charged lipid ions with electrons having kinetic energie

140 e surface of lipid bilayer regardless of the charged lipid ratio.

141 compensation field (DF and CF), and mass-to-charge (m/z).

142 gh luminescence loses its PL when positively charged macromolecules are wrapped around its surface.

143 se sensing for simultaneous size and surface charge measurements on a particle-by-particle basis, ena

144 Encouragingly, the charge mobility has been improved recently by driving na

145 Here we use charge modulation spectroscopy to reveal a bipolaron she

146 oderate DC electric fields are used to drive charged molecules out of the tip.

147 line supramolecular frameworks consisting of charged molecules, held together by hydrogen bonds and C

148 ng Poisson-Nernst-Planck (PNP) equations for charged multispecies diffusion coupled with the fluctuat

149 units are made as precursors with positively charged N-terminal anchors, whose cleavage via the prepi

150 the transition from a hydrated environment (charged nanodroplet generated by electrospray ionization

151 The assembly of charged nanoparticles (NPs) and proteins in aqueous solu

152 Multiply charged negative ions are ubiquitous in nature.

153 ated on twenty types of polymers (positively charged, negatively charged, or neutral) and ten combina

154 o, the detection results of other negatively-charged neurotransmitters like acetylcholine demonstrate

155 mine release from PC12 cells, revealing that charge neutralization of 5RK promotes spontaneous and in

156 hape-dependent uptake behavior of negatively charged, non-spherical polyethylene glycol (PEG) hydroge

157 clude that a concentrated region of negative charge, not steric properties, resulting from multiple i

158 a circular configuration with zero skyrmion charge number.

159 into account the effects of the density and charge of analytes.

160 etal is positioned to stabilise the negative charge of the 5'-phosphate, and thus three metals could

161 Critically, the positive charge of the lysine residues was necessary for fusion r

162 ively, which is significant dominated by the charge of the redox probe.

163 ss-HSDNA/rGOae electrode in three different charges of the redox mediators (i.e., neutral FcCH2OH, c

164 There is a correlation between the amount of charge on the atoms and their catalytic activity.

165 ts the spatial distribution of the deposited charge on the dielectric surface between the adjacent el

166 ncreased stabilization of a partial positive charge on the nitro-substituted carbon in both transitio

167 forces originating from clustering of point charges on the NTD surface required for function.

168 , 1.11-1.70) following OAR as well as higher charges (OR, 1.28; 95% CI, 1.01-1.62) and increased 30-d

169 ge side-chain size, flexibility, hydropathy, charge, or polarizability.

170 of polymers (positively charged, negatively charged, or neutral) and ten combination forms via hemol

171 "site-selective" Mott scenario without real charge order on Ni sites.

172 The charge ordered structure of ions and vacancies character

173 Conversely, release of charged osmolytes (d-aspartate) was strongly reduced by

174 This model was extended to charged particle exposures by integrating Monte Carlo ca

175 emitted in the opposite direction of moving charged particles in a left-handed material.

176 Charged particles such as protons and carbon ions are an

177 e electromagnetic field fluctuations and the charged particles that comprise an undamped kinetic Alfv

178 The effect of adding salt to the charged phase changes the structure from the primitive c

179 ns are shown to charge-invert the positively charged phospholipids to the negative mode.

180 esembles UBA5 His336 and enters a negatively charged pocked on the other UFM1 molecule.

181 e associative phase separation of oppositely charged polyelectrolytes into polyelectrolyte dense (coa

182 rials such as complexes and multilayers from charged polymers depends on (inter)diffusion of these po

183 c repulsion between the two interpenetrating charged polymers.

184 oxidation reaction at significantly reduced charge potentials mainly takes place at Li2 O2 /electrol

185 xcessive depletion of electrolyte during the charge process.

186 nce of thermal activation of carriers out of charge puddles.

187 ge rates (270 mA g(-1), 80 cycles) and, at a charge rate of 30 mA g(-1), exhibit charge capacities of

188 ls); They perform outstandingly at very high charge rates (270 mA g(-1), 80 cycles) and, at a charge

189 of the most discriminating couples [mass-to-charge ratio (m/z); retention time (tR)] and on the most

190 Attenuation of the charge recombination for RSQ2 was revealed by electroche

191 We propose that the charged region and chain directionality assist product d

192 duced charge trapping and optically-mediated charge release.

193 Mutation of a charged residue at the interface (Arg-103) weakens the i

194 luster (by nitrosylation) permits positively charged residues in the C-terminal helix to engage in DN

195 bc9 residues interacting with the negatively charged residues of the NDSM.

196 Charged residues on the LBD surface form pathways that f

197 nserved, the linear patterning of oppositely charged residues shows minimal variation.

198 Charged residues were poorly tolerated, conferring extre

199 e site contains several conserved positively charged residues, and a portion of the active site shows

200 iour, including emergent magnetic monopoles, charge screening and transport, as well as magnonic resp

201 buted to the intricate interplay between the charge screening at the PZT/SNNO interface and the charg

202 Even low charge screening lifts the phonon Kohn anomaly near the

203 Increasing charge segregation from WT RAM sharply decreases transcr

204 ray spectroscopy when coupled to a low-noise charge-sensitive preamplifier.

205 he amplitude of the resulting P700(+*)A1(-*) charge-separated state indicates that the yield is direc

206 solid state and the origin of the long-lived charge-separated state were studied by steady-state and

207 transports it to the reaction center, where charge separation occurs.

208 tenna complexes to the reaction center where charge separation occurs.

209 organisms perform this energy transport and charge separation with near unity quantum efficiency.

210 d A(-*)-R(*) radical pair, where the initial charge separation yields a 3:1 statistical mixture of D(

211 imately 150 ps decay assigned to trapping by charge separation, and the amplitude of the resulting P7

212 energy losses in the reductive, short-range charge shift from C60 to C70.

213 s ranging across nonpolar, polar, ionic, and charge-shift bonds.

214 Analogues with five positive charges show the lowest activity.

215 formation supporting the importance of these charged side chains in fibril formation of betaS.

216 The negatively charged silicon-vacancy centre combines the advantages o

217 Ion exchange at charged solid-liquid interfaces is central to a broad ra

218 ved upon metalation, effectively turning the charge state and cationization mode into extra separatio

219 od for stabilizing the photoluminescence and charge state of color centers based on epitaxial growth

220 residues and the preference for a dianionic charge state of FHA-bound pThr.

221 Therefore, potential contributions from charge state should be considered when using experimenta

222 ated trapping and isolation of an individual charge state was also demonstrated to saturate the ion g

223 The d/l-pairs coeluting in one charge state were resolved in another, and epimers merge

224 d on all covalent biotin additions, for each charge state, for both the lysine- and cysteine-biotin c

225 nstrated to saturate the ion guide with that charge state.

226 with an energy above 1.3 eV can excite this charged state and recover the bright neutral state.

227 Charge-state distributions are not obtained for proteins

228 usters are structurally identical in the two charge states, with nearly perfect Ih point symmetry, an

229 metal oxides have been shown to provide high charge storage capacity but with poor cyclic stability d

230 ed analytes were attracted by the positively charged surface at pH 3.

231 eptides upon interaction with the negatively charged surface functional groups.

232 at this activity is mediated by a positively charged surface that is partially masked by its intramol

233 leading to dissimilar disease states such as CHARGE syndrome or autism spectrum disorders.

234 The charge-tagged carbene was generated in situ in a tandem

235 tecting group, thus eliminating the negative charges that have been shown to have a negative effect o

236 During charging, the oxidation reaction at significantly reduce

237 Excimer states having variable charge transfer (CT) character are frequently implicated

238 How tightly bound charge transfer (CT) excitons dissociate at organic dono

239 phore pi-backbone the highest intramolecular charge transfer (ICT) is observed.

240 pe semiconductive g-C3 N4 induces a vigorous charge transfer across the MoB/g-C3 N4 Schottky junction

241 screening at the PZT/SNNO interface and the charge transfer at the SNNO/LSMO interface.

242 the sensitivity of the yield of photoinduced charge transfer between a QD and a molecular probe to ev

243 Controlling the charge transfer between a semiconducting catalyst carrie

244 r electrochemical window and 70% higher CTC (charge transfer capacity) than Pt microelectrodes of sim

245 method to organize two-dimensional molecular charge transfer crystals into arbitrarily and vertically

246 upled acceptors has been proposed to enhance charge transfer efficiency in functional organic electro

247 such as graphene are uniquely responsive to charge transfer from adjacent materials, making them ide

248 /cm(2) was necessary to induce a significant charge transfer from SiC to WSe2, where a reduction of v

249 g augmented by dispersion, polarization, and charge transfer in competition with destabilizing Pauli

250 Metal-to-ligand charge transfer is involved in both the formation of Pu3

251 We then analyse the charge transfer mechanism through the protection layers

252 oss the c-Si/a-B interface systems where the charge transfer occurs mainly from the interface Si atom

253 is characterized by a significant degree of charge transfer permitted by the pi-stacking that occurs

254 The charge transfer resistance in the impedimetric measureme

255 Increasing rotating speed reduces the charge transfer resistance resulting in the lower detect

256 tacene-C60 DA interface, we confirm that the charge transfer transition is strongly aligned orthogona

257 The results highlight a charge transfer transition that leads to changes in the

258 serve as an efficient medium for long-range charge transfer.

259 rs from a long-lived doublet ligand-to-metal charge-transfer ((2)LMCT) state that is rarely seen for

260 present a comprehensive investigation of the charge-transfer (CT) effect in weakly interacting organi

261 c transitions of mixed ligand-to-metal-metal-charge-transfer (IPr --> AuM2) and interligand (IPr -->

262 orm-to-naphthyridine, metal/ligand-to-ligand charge-transfer (ML-LCT) excited states were observed in

263 ms these materials undergo an intramolecular charge-transfer event upon photoexcitation.

264 t transition-metal complexes with long-lived charge-transfer excited states.

265 R molecules that host LiCl salt exhibit fast charge-transfer kinetics and as much as five-times highe

266 ll as purely quantum mechanical effects like charge-transfer or exciton-coupling, are included.

267 Overall, the charge-transfer resistance decreased after antibody bind

268 ed to characterize Na(+) and H(+) transport, charge translocation, and thermal stability of the diffe

269 relationship between heating or cooling and charge transmission characteristics.

270 nd the molecular characteristics that permit charge transport can render the materials stiff and brit

271 rovide many active edge sites, enhanced mass/charge transport capability, easy release oxygen gas bub

272 This work is a direct evidence of charge transport control in a protein backbone through e

273 tes the potential role played by polarons in charge transport in CH3NH3PbI3.

274 coupling between QDs and allow for efficient charge transport in QD films.

275 Charge transport is investigated for solution-sheared fi

276 rk points out the importance of matching the charge transport layers in perovskite solar cells when t

277 Although the mass and charge transport occurs by advection by thermal velocity

278 g fluid momentum equation result in enhanced charge transport via a mechanism distinct from the well-

279 r from adjacent materials, making them ideal charge-transport layers in phototransistor devices.

280 optimization of the thin-film morphology and charge-transport properties of conjugated polymers.

281 memory devices using artificially-structured charge trap layers through the functionalization of the

282 at serve as a basis for electrically-induced charge trapping and optically-mediated charge release.

283 ith spontaneous electron-hole separation and charge trapping induced by the atomic disorder.

284 rt peptide sequences, we determined that the charge type and identity of amino acids surrounding FG s

285 A negatively charged uncoated, "bare" CNP with high luminescence lose

286 This protein is strongly positively charged under measurement conditions and therefore captu

287 accepted that the detection of polarization charges using a conventional conductive atomic force mic

288 The mean payment per charge was the same for men and women, $66 in 2012 and $

289 By engineering C-terminal charges, we develop CRY2high and CRY2low with elevated o

290 symmetric charge distribution is obtained by charge-weighted averaging of outer and inner radii.

291 Small variations on geometry and atomic charge were detected on the carbonate ions, implying tha

292 ately concentrated markets, although overall charges were 8.3% lower (95% CI, -14.0% to -2.3%; P = .0

293 properties, such as size, polydispersity and charge, were assessed for each surfactant type and mass

294 rejection despite the differences in surface charge, which suggests that rejection by these membranes

295 enables the direct detection of the monopole charge with current techniques.

296 When the receiving arm is charged with KCN, transport is much faster (ca. 100 h) a

297 RNA) decodes mRNA codons when aminoacylated (charged) with an amino acid at its 3' end.

298 described by the embedding of a compensating charge within an aromatic cyclononatetraenide ring by th

299 city of about 130 mA h g(-1) at 35 C (fully charged within 100 s) and sustain more than 10,000 cycl

300 monomers self-assemble using electrostatic 'charge zippers'.