ライフサイエンスコーパス: charge

1 rface layer with a higher detectable analyte charge.

2 rried a sufficiently large positive solution charge.

3 tal sulfides rather than S(8) after the full charge.

4 gnitude, depending upon the size and surface charge.

5 out an equivalent spatiotemporal transfer of charge.

6 e source-drain current from small numbers of charges.

7 r hospital stays and greater hospitalization charges.

8 bridge and can be modified by altering these charges.

9 nterface, dissociating efficiently into free charges.

10 and inflation-adjusted hospital readmission charges.

11 en excitons, charge-transfer states and free charges.

12 % more and ~20% fewer emissions than daytime charging.

13 easured sleep was collected using the Fitbit Charge 2 (FC2), from which sleep duration, sleep duratio

14 discovered that inclusion of the positively charged A1 insert in mouse neuroligin-1 increases its bi

15 on, resulting in the fractional shift of the charge across the disk membrane.

16 ge density due to the presence of negatively charged aggrecan glycosaminoglycans that provide swellin

17 An aqueous suspension of either positively charged (amine-modified polystyrene; a-PS) or negatively

18 platform combines the natural catabolism of charged amino acids with a catalytically efficient and t

19 esults in the suppression of the transferred charge amount.

20 e important double-layer properties, such as charge amplification, energy storage, and differential c

21 EVs, zeta potential measurements for surface charge analysis, and fluorophore-based confocal imaging

22 ether, with the sum corrected for effects of charge and 5d metals.

23 d peptides of 4-11 residues, varying in both charge and composition, as the substrates of PfCRT in vi

24 By contrast, another group decreases in net charge and consists of sites that are further away from

25 nt near Val27, which dynamically responds to charge and inhibitor binding.

26 ich replaces the external flux by the offset charge and introduces a new collective quasicharge varia

27 exhibit higher IDR contents, higher mean net charge and lower hydropathy and prefer to bind to RNA.

28 The interconversion of charge and spin currents via spin-Hall effect is essenti

29 eering to sculpt the spatial distribution of charge and spin states and thus the energy and dynamics

30 her testing of 34 of these 36 signals in the CHARGE and SpiroMeta consortia showed that 16 replicated

31 bimodal compositional distribution early in charge and, also, a dramatic increase of the charge-disc

32 isome, while a stretch of conserved positive charges and a central pleckstrin homology-like domain ar

33 ate complex to be stored after photochemical charging and used as a reagent in dark reactions, such a

34 ty are commonly observed in individuals with CHARGE, and neuronal differentiation is reduced in CHARG

35 5 transport that provides three net negative charges appeared self-inhibitory because of ClC-5's volt

36 ent organellar membranes vary, their surface charges are similarly expected to diverge.

37 electrostatic interaction between positively charged arginine in extracellular loop 2 (K210) and a ne

38 disordered acidic tracts and the positively charged arginine-rich region.

39 st, the proteins containing the same type of charge as the surface showed little or no difference, ex

40 extracellular loop 2 (K210) and a negatively charged aspartate (D112) in extracellular loop 1 that he

41 oved from near zero to 2 M due to the highly charged asymmetric structure formed in alkaline environm

42 ngly, UVPD fragments also indicated that the charge at the "unfolding" N-terminus of ADH decreased at

43 Because of this asymmetry, the net-negative charge at the inner leaflet exceeds that at the outer le

44 favored, stabilized by hydroxyl ligands and charge balancing calcium ions in the interlayer space.

45 i/Al ratio of the anionic framework, and the charge-balancing cations.

46 Fast-charging batteries typically use electrodes capable of a

47 A UbV targeting Ube2D1 did not affect charging but greatly attenuated chain elongation.

48 and general, and the amount and polarity of charge can be flexibly tunable.

49 In this study, negatively charged CAR-NPs and positively charged polyethylenimine

50 the doubled vacancy concentration raises the charge carrier density and suppresses bipolar diffusion,

51 Charge carrier insertion into the graphene makes the EEV

52 femtoseconds to the seconds, reveal that the charge carrier lifetimes as well as the charge injection

53 any states deep within the bandgap that trap charge carriers and cause them to recombine non-radiativ

54 s the energy-dependent mean free path of the charge carriers and is affected by crystal structure, sc

55 roperties with a high fraction of long-lived charge carriers and the availability of a reductive and

56 n for more than 2600 years but the nature of charge carriers and their transfer mechanisms still rema

57 ar O(2) trapped in the bulk structure of the charged cathode, which is reduced on discharge.

58 k heterojunctions reveals the influence that charge-collecting electrodes have on the electronic nois

59 strated it was homogeneous in terms of size, charge, conformation, absence of glycosylation, and cont

60 nic constitution and defect structure: ionic charges contribute to charge transfer and screening at o

61 ikelihood of lithium metal plating if proper charging controls are used, alleviating a major safety c

62 a narrow tetrameric channel with a strongly charged core.

63 We further demonstrate how the charge current can switch the magnetization of the ferro

64 E), a mechanism by which materials convert a charge current into a spin current, invokes interesting

65 The potential-dependent charging current upon the formation of the microscopic e

66 lly and experimentally the effect of induced charging currents on the fast-scan cyclic voltammetry.

67 Increased cation charge decreases selectivity for oxo-site bonding, leadi

68 and two-dimensional electron gases where the charge degree of freedom can be actively controlled by c

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

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

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

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

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

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

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

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

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

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

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

80 ique chemical recognition of anions with low charge density.

81 polydimethylsiloxane (PDMS) channel created charge-dependent accumulation 2 to 4 min after the onset

82 onset of channel flow creates an unexpected, charge-dependent accumulation of colloidal particles, wh

83 al ion mass spectrometry (I(2)MS) method for charge detection enables the characterization of highly

84 , rather than surface wettability or surface charge, determines the anti-wetting performance of the c

85 ion state in which there is partial positive charge developing on the C-O carbon atom progressing C-H

86 an speed, contact cycles, contact region and charge diffusion on the transistor were investigated, re

87 entiostatic hold following the galvanostatic charge-discharge cycle.

88 charge and, also, a dramatic increase of the charge-discharge voltage hysteresis at x > 0.88.

89 it significant degradation issues under fast-charge/discharge conditions and unsatisfying long-term c

90 rejection, i.e., during doping/de-doping and charging/discharging.

91 pacitance reflecting the phase of electrical charge displacement required for the motor to overcome t

92 Yet, charge disproportionation lacks technological relevance

93 re, we present a systematic investigation of charge distribution between different classes of GPL und

94 under the direct current modifies the space-charge distribution in the electric double layer, which

95 he detection probe by conjugating negatively charged DNA oligonucleotides.

96 lmost all oxygen-redox compounds, is lost on charging, driven in part by formation of molecular O(2)

97 ynamic ejection, deformation and assembly of charged droplets by control of Taylor cone instability a

98 nts that result in compensatory decreases in charge elsewhere on the protein.

99 oil emulsions were prepared using negatively charged emulsifier under acidic conditions.

100 lipids that preferentially interact with the charged ends of an I-BAR domain, we find clustering of p

101 Charge-enhanced Bronsted acid organocatalysts with elect

102 ES differential mobility analyzer, nES DMA), charge equilibration is based on bionanoparticle interac

103 Organic semiconductors are commonly used as charge-extraction layers in metal-halide perovskite sola

104 sed to space radiation, a spectrum of highly-charged, fast-moving particles that includes (56)Fe and

105 They suggest that charge fluctuation in the metallic phase of intrinsic VO

106 tions are regulated by the interplay between charge fluctuation, charge redistribution, and structura

107 were directly self-assembled through highly-charged [Ge(4) ](4-) units and transition metal cations,

108 oconduction, a complicated process involving charge generation and recombination in the time domain a

109 effects-as seen in characterizations of the charge generation and transfer that occur at solid-liqui

110 phase vs solid-solution) and localization of charge give rise to additional kinetic barriers in NCA a

111 The very low energy combined with lack of charge gives the technique great potential for studying

112 Adenosine radicals tagged with a fixed-charge group were generated in the gas phase and structu

113 EIS) (which measure the movement of only the charged, i.e., dissociated, ions) with the molar conduct

114 onclusively demonstrate the role of electric charge in detection sensitivity as well as the prospect

115 tructural stability which allows the protein charge in solution to be controlled via pH adjustment wi

116 by long-range interactions because opposite charges in trypsin and BPTI draw them together.

117 the charge carrier lifetimes as well as the charge injection and charge recombination dynamics depen

118 harge redistribution is allowed, even though charge injection happens at a position far from the anti

119 rface presents a lower barrier than gold for charge injection.

120 ater ions in opposite directions, leading to charge interactions that can affect the distribution of

121 ift in the absorbance spectrum and injects a charge into a helical conjugated pai-system without inje

122 crine cells to transduce low cellular energy charge into the mobilization of energy stores, which in

123 lyte effectively turns the macropores into a charged ion-selective layer and thus increases the condu

124 uniquely catalyze the exchange of oppositely charged ions (Cl(-) for H(+)).

125 g creates a spontaneous array of differently charged ions and is associated with electronic phenomena

126 ant complexes into the gas phase as multiply charged ions suitable for mass spectrometric analysis.

127 s differ profoundly from binding of multiply charged ions, often leading to overall compaction of the

128 TMs are almost parallel, and the positively charged JM segments are expected to be close to each oth

129 ies showed that enzyme molecules with no net charge leached at the slowest rate from CNT/E films.

130 an essential tRNA synthetase that accurately charges leucine to tRNA(Leu) for protein translation.

131 ubtle conformational effects seen for singly charged metals differ profoundly from binding of multipl

132 ed by ionic interactions with the negatively charged microtubule surface.

133 ompact structures that are resistant to both charge migration and unfolding.

134 ates of UVPD fragments enabled monitoring of charge migration to the unfolded regions.

135 equired for transport III) component CHMP1B (charged multivesicular protein 1B), whereas NS-associate

136 rimary topological excitations are extended, charge-neutral disclination loops that undergo complex d

137 Among these, the negatively charged nitrogen-vacancy (NV(-)) defect in diamond is at

138 Here, we explore whether patterns of local charge of H1N1 HA can explain this discrepancy and thus

139 In an effort to reduce the charge of membrane proteins, we examined the utility of

140 lipid bilayers are possible and that the net charge of the bilayer as well as the presence of divalen

141 ound to be strongly dependent on the surface charge of the CDs.

142 Changes in overall charge of the complex modulate contrast enhancement, esp

143 pH and the electrical charge of the emulsifier modulated the antioxidant effec

144 rcs that correspond to projected topological charges of +/-1 in the surface Brillouin zone.

145 plemented approaches to estimate the surface charges of the cytosolic membranes of various organelles

146 In contrast, all other tRNAs retain charging of their cognate amino acids in a manner that i

147 n and reduced total translation, the reduced charging of tRNA(Gln) in amino-acid-deprived cells also

148 in the electrostatic interaction between the charges on each end of the bridge and can be modified by

149 t significantly altering their size, surface charge, or stability in aqueous buffer.

150 ons cannot generally be classified as either charge- or frontier orbital-controlled; instead, our res

151 We propose a series of charge-ordered states at commensurate filling fractions

152 Charge ordering creates a spontaneous array of different

153 that determines the type and temperature of charge ordering.

154 ure magnetism in these superlattices and the charge-ordering pattern in the m = 3 member.

155 This model provides new insights into charge-ordering phenomena in transition-metal oxides in

156 in many cases of spreading out the positive charge over several atoms.

157 s characterising molecules in terms of their charge, oxidation state, and chirality via optoplasmonic

158 eins with selective permeability to specific charged particles.

159 , and neuronal differentiation is reduced in CHARGE patient-derived iPSCs and conditional knockout mo

160 We determined the effects of charge patterning on phase behavior through sequence shu

161 ordination, and the associated electrostatic charge patterns, on the complex structural space of the

162 r for the two uncharged PDIs compared to the charged PDIs, reflecting electrostatic interactions of t

163 ative correlation with the supplied electric charge, Pearson's r = 0.994.

164 lysis of neutral arylsulfonate monoesters or charged phosphate diesters and fluorophosphates.

165 ich bind to membranes that expose negatively charged phospholipids in a Ca(2+)-dependent manner.

166 y, negatively charged CAR-NPs and positively charged polyethylenimine (PEI)-coated CAR-(PEI)NPs were

167 ne-modified polystyrene; a-PS) or negatively charged (polystyrene; PS) particles that flowed into a p

168 In HLA-B*57:03, the charged POmega-2 residues protruded out from the cleft a

169 orous network structure with tunable surface charge, pore size, and interlayer spacing.

170 pH 7), despite the loss of effective surface charge potential.

171 nia and New York, respectively, overnight EV charging produces ~70% more and ~20% fewer emissions tha

172 The higher charges, proportion of patients on Medicaid, and rates o

173 ed NPs were more stable at the point of zero charge (PZC) than at neutral pH (pH 7), despite the loss

174 cs features, retention time (rt) and mass-to-charge ratio (mz) pairs, that often possess similar stat

175 ifetimes as well as the charge injection and charge recombination dynamics depend largely on the pres

176 trons toward cathode side, which reduces the charge recombination there.

177 lds are explained by donor-independent, fast charge recombination with rates of ~0.2 ps(-1), thus inh

178 rent charge-separation, charge-transfer, and charge-recombination routes have been demonstrated, both

179 tibody-antigen association are enhanced when charge redistribution is allowed, even though charge inj

180 This charge redistribution modifies the Li(+) substructure ca

181 by the interplay between charge fluctuation, charge redistribution, and structural transition.

182 ng in-source activation was not observed for charge-reduced ADH, which likely adopted compact structu

183 concanavalin A, and C-reactive protein under charge reducing conditions.

184 mined the utility of alkali metal salts as a charge-reducing agent.

185 native net dopant concentration in the space charge region, (ii) sputter deposition of ZnO damages th

186 Segregated charged regions within the RNF4 N-terminus promote compa

187 ee energy in the LD oil phase and positively charged residues near predicted hairpin hinges that beco

188 Therefore, an increased ion charge results in a dramatic decrease in the sensor sens

189 semiconductors is to avoid the formation of charge scattering and trap sites from adjacent dielectri

190 Also, charge sensing between quantum dots in closely spaced wi

191 The ensuing charge separated radical ion paired complex is spectrosc

192 d, and hence triplet transfer proceeds via a charge separated state.

193 ron transfer reactions that ultimately yield charge separated states with lifetimes as long as 61 mic

194 E(4)NDI can be selectively excited to form a charge-separated state via ultrafast photoinduced electr

195 excited at 370 nm, but it does not produce a charge-separated state when excited at 420 nm (T(4)).

196 s within 0.1-20 ps and revealed little or no charge separation and oxidation of the special pair, P70

197 tion of the prosthetic group retinal, and 2) charge separation between the protonated retinal Schiff

198 catalytic activity, i.e., light absorption, charge separation, transfer of charges to the reaction c

199 ctions as an electron acceptor to facilitate charge separation, while holes could transfer to CuO(x)

200 s the migration of electrons and interfacial charge separation.

201 Different charge-separation, charge-transfer, and charge-recombina

202 Dynamic charge shifting within the antibody during its interacti

203 robes containing a fluorophore with negative charge showed high M(2)R affinities (pK(i) (radioligand

204 c interactions of the latter with oppositely charged sites on the cationic surfactant headgroups and

205 ractions that can affect the distribution of charged species in the domain.

206 However, charge spin coherence is limited by interaction with the

207 his nickelate that reflects a coupling among charge, spin, and lattice degrees of freedom that differ

208 eating a penalty for compounds with positive charge spread over a larger compound surface area as occ

209 ent charge states, (3) the smoothness of the charge state distribution, and (4) symmetry and separati

210 iron-sulfur clusters in the [Fe(4)S(4)](3+) charge state have been proposed as short-lived intermedi

211 We determined the charge state of nonviable P. syringae as a function of p

212 interstitial coatings would yield a surface charge state of zero in more-alkaline fluids and prevent

213 macromolecules that exist in three different charge states and have a tendency to phase separate.

214 than expected for the predicted high atomic charge states due to significant impact of ion caging an

215 reased, the abundance of each of the six ESI charge states for wt CI-2 and each mutant is found to va

216 onversion due to their excellent interfacial charge states in tuning the electronic properties of dif

217 e at high flow rates, ions related to higher charge states of proteins dominated the spectra.

218 f ammonium acetate, at low flow rates, lower charge states of proteins showed high intensities, while

219 unfolding started at the N-terminus, and the charge states of UVPD fragments enabled monitoring of ch

220 The charge states produced by native MS of membrane proteins

221 nsistency of the peak shape across different charge states, (3) the smoothness of the charge state di

222 In particular, hot spots of charge storage are identified.

223 hrinkage of the Li-layer size, the intrinsic charge storage mechanism (two-phase vs solid-solution) a

224 a membrane anchor group based on negatively charged sulfonate and dodecyl chain.

225 sirable diameter (203.2 nm) and a negatively charged surface (-12.7 mV).

226 Thiocyanate anions at positively charged surface sites and negatively charged surface sit

227 itively charged surface sites and negatively charged surface sites and those participating in contact

228 This observation offers insights into charge-symmetry-breaking forces acting in atomic nuclei.

229 Synaptotagmin-1 (Syt1), by adding a positive charge (Syt1(D232N)) or increasing its hydrophobicity (S

230 For seven singly charged test ions (m/z 124-1131), the ambient pressure i

231 ons suggest that the formation of the highly charged tetra-reduced carbanion is stabilized through Li

232 iency via virtual polariton modes with image charges that we dub 'image polaritons'.

233 g acoustic streaming electrolyte flow during charging, the device enables dense Li plating and avoids

234 epletion gradients in the electrolyte during charging, they rapidly develop porosity, dendrites, and

235 HA forms an adsorbed surface layer, but its charge, thicknesses, compressibility, and mass are signi

236 ular concentrations and electrolyte state of charge through, e.g., bimolecular decomposition mechanis

237 tific Workforce Diversity office has led the charge to develop and implement evidence-informed interv

238 t absorption, charge separation, transfer of charges to the reaction centres and catalytic turnover,

239 rating organic phosphors achieve an internal charge-to-light conversion of unity(10), their refractiv

240 ai* transitions are dominant, intramolecular charge transfer (ICT) also contributes in the excited st

241 The metal-to-ligand charge transfer (MLCT) excited states of Ru polypyridyl

242 the electrode and electrolyte to facilitate charge transfer and mass transport, plays a vital role i

243 efect structure: ionic charges contribute to charge transfer and screening at oxide interfaces, trigg

244 netic field, we show that the spin-dependent charge transfer between WSe(2) and CrI(3) is dominated b

245 scenarios, it is an interesting question, if charge transfer can be coupled with RNA function.

246 oquinodimethane (F4TCNQ), is of interest for charge transfer complex formation and as a p-dopant in o

247 of SQOR proceeds via formation of an intense charge transfer complex that subsequently decays to elim

248 ant NP-assembled electrodes through improved charge transfer efficiency.

249 The dimer N levels include local and charge transfer excitons within each dimer.

250 Its application to the antiferromagnetic charge transfer insulator YBa(2)Cu(3)O(6.1) revealed rap

251 ects could play an explicit role even if the charge transfer is inhibited(8).

252 st plot provides an insight into the rate of charge transfer on the electrode/electrolyte interface.

253 tion and the factors that control asymmetric charge transfer remaining under investigation.

254 e higher surface area (97.895 m(2)/g), lower charge transfer resistance (16.2 kOmega) for the ZCNT 0.

255 dies observed that L-MT sample performed low charge transfer resistance (336.7 Omega cm(2)) that prom

256 cific surface area, which contributed to low charge transfer resistance and high transduction activit

257 s prepared on polyolefin films exhibit a low charge transfer resistance of about 20 Omega, high sensi

258 The estimated charge transfer resistance value of 300 Omega cm(2) obta

259 hage on the cytosensor surface increased the charge transfer resistance, enabling detection of colifo

260 ility enables direct excitation of low-lying charge transfer states by far-red light.

261 te insulation layers are used to inhibit the charge transfer(5,6) or when off-resonance excitations a

262 extending the IDT core to promote interchain charge transfer, is a logical strategy toward high-mobil

263 aterials due to the effect of intramolecular charge transfer.

264 erties is based on the concept of electronic charge transfer.

265 sion in the solid state, attributable to the charge-transfer character of these inclusion complexes.

266 ing, S-H...pai, C-H...pai, pai-pai stacking, charge-transfer complexation, etc.

267 igh optical activity study reveals important charge-transfer differences within the aromatic oligomer

268 sky-blue to deep-blue photoluminescence from charge-transfer excited states.

269 Photoinduced charge-transfer is an important process in nature and te

270 e forward reaction and catalyzed by a single charge-transfer process for the reverse switching.

271 lectron-hole encounters at later times, both charge-transfer states and emissive excitons are regener

272 setting up an equilibrium between excitons, charge-transfer states and free charges.

273 promotes the formation of hybridised exciton/charge-transfer states at the interface, dissociating ef

274 Different charge-separation, charge-transfer, and charge-recombination routes have be

275 er, the lack of fundamental understanding on charge transport (CT) mechanism as well as the correlati

276 The acceptors exhibit balanced ambipolar charge transport and surprisingly long exciton diffusion

277 gation of 2D transport anisotropy and chiral charge transport as a result of broken symmetry.

278 Charge transport in DNA-based junctions has been reporte

279 er sequences exhibit unexpected and distinct charge transport pathways that enhance molecular conduct

280 molecular semiconductors and of the inherent charge transport physics that takes place in them.

281 However, their charge transport properties remain elusive, plagued by t

282 ty of the band structure manifests itself in charge transport properties.

283 istribution, tunable pore size and excellent charge transport provides great opportunity to fabricate

284 port the observation of large non-reciprocal charge transport(3) in a magnetic topological insulator,

285 tronic band structure for efficient electron charge transport.

286 proteins because of their role in biological charge transport.

287 amolecular constructs to deliver outstanding charge-transport capabilities using metalloporphyrin-bas

288 ng of Y6 and CH1007 to ensure their superior charge-transport properties.

289 tate polymer batteries with good interfacial charge-transport properties.

290 This maintains normal charged tRNAGln levels despite Gln4p depletion, confirme

291 50 mm(2) can wirelessly light up 70 LEDs or charge up a 15 muF capacitor to 12.5 V in ~90 s.

292 hy were used to fractionate various size and charge variants from the stressed IgG(1).

293 was diminished in cells where the membrane's charge was experimentally reduced.

294 orate target proteins based on their surface charge, while cytoplasmic MLOs formed in AfrLEA6-transfe

295 ncy and thus further associate electrostatic charge with immune escape and viral evolutionary dynamic

296 The aptamer-nanotrain assembly, charged with doxorubicin, selectively kills liver cancer

297 re is insufficient guidance for policymakers charged with establishing evidence-based policy to deter

298 that its intent is to assist other agencies charged with protecting public health, without minimizin

299 ide (PDI) dyes, having different lengths and charges, within the one-dimensional (1D) nanoscale pores

300 We observe separate optima in the charge yield as a function of driving force for singlet