Ratiometric Optical Sensing of Chloride Ions with Organic Fluorophore-Gold Nanoparticle Hybrids: A Systematic Study of Design Parameters and Surface Charge Effects

Small ◽  
2010 ◽  
Vol 6 (22) ◽  
pp. 2590-2597 ◽  
Author(s):  
Andreas Riedinger ◽  
Feng Zhang ◽  
Fabian Dommershausen ◽  
Carlheinz Röcker ◽  
Stefan Brandholt ◽  
...  
2013 ◽  
Vol 1 (2) ◽  
pp. 1300079 ◽  
Author(s):  
Li Shang ◽  
Linxiao Yang ◽  
Jürgen Seiter ◽  
Marita Heinle ◽  
Gerald Brenner-Weiss ◽  
...  

2020 ◽  
Author(s):  
Victor Kwan ◽  
Styliani Consta

<div>Charged droplets play a central role in native mass spectrometry, atmospheric aerosols and in serving as micro-reactors for accelerating chemical reactions. The surface excess charge layer in droplets has often been associated with distinct chemistry. Using molecular simulations for droplets with Na+ and Cl- ions we have found that this layer is ≈ 1.5−1.7 nm thick and depending on the droplet size it includes 33%-55% of the total number of ions. Here, we examine the effect of droplet size and nature of ions in the structure of the surface excess charge layer by using molecular dynamics. We find that in the presence of simple ions the thickness of the surface excess charge layer is invariant not only with respect to droplet size but also with respect to the nature of the simple ions and it is not sensitive to fine details of different force fields used in our simulations.</div><div> In the presence of macroions the excess surface charge layer may extend to 2.0. nm. For the same droplet size, iodide and model hydronium ions show considerably higher concentration than the sodium and chloride ions. <br></div><div>We also find that differences in the average water dipole orientation in the presence of cations and anions in this layer are reflected in the charge distributions. Within the surface charge layer, the number of hydrogen bonds reduces gradually relative to the droplet interior where the number of hydrogen bonds is on the average 2.9 for droplets of diameter < 4 nm and 3.5 for larger droplets. The decrease in the number of hydrogen bonds from the interior to the surface is less pronounced in larger droplets. In droplets with diameter < 4 nm and high concentration of ions the charge of the ions is not compensated only by the solvent polarization charge but by the total charge that also includes the other free charge. This finding shows exceptions to the commonly made assumption that the solvent compensates the charge of the ions in solvents with very high dielectric constant. The study provides molecular insight into the bi-layer droplet structure assumed in the equilibrium partitioning model of C. Enke and assesses critical assumptions of the Iribarne-Thomson model for the ion-evaporation mechanism. <br></div>


2021 ◽  
pp. 2101549
Author(s):  
Anna R. Ziefuss ◽  
Torben Steenbock ◽  
Dominik Benner ◽  
Anton Plech ◽  
Jörg Göttlicher ◽  
...  

Nanoscale ◽  
2020 ◽  
Vol 12 (27) ◽  
pp. 14524-14537 ◽  
Author(s):  
Jeffrey K. Wuenschell ◽  
Youngseok Jee ◽  
Derek K. Lau ◽  
Yang Yu ◽  
Paul R. Ohodnicki Jr.

Coupled plasmonic and Drude response of gold-nanoparticle incorporated LSTO demonstrates visible and NIR fiber-based sensing of hydrogen at high-temperature (600–800 °C).


2019 ◽  
Vol 91 (9) ◽  
pp. 5530-5536 ◽  
Author(s):  
Je Hyun Bae ◽  
Dengchao Wang ◽  
Keke Hu ◽  
Michael V. Mirkin

2005 ◽  
Vol 125 (5) ◽  
pp. 493-503 ◽  
Author(s):  
Nazzareno D'Avanzo ◽  
Hee Cheol Cho ◽  
Illya Tolokh ◽  
Roman Pekhletski ◽  
Igor Tolokh ◽  
...  

Ion channel conductance can be influenced by electrostatic effects originating from fixed “surface” charges that are remote from the selectivity filter. To explore whether surface charges contribute to the conductance properties of Kir2.1 channels, unitary conductance was measured in cell-attached recordings of Chinese hamster ovary (CHO) cells transfected with Kir2.1 channels over a range of K+ activities (4.6–293.5 mM) using single-channel measurements as well as nonstationary fluctuation analysis for low K+ activities. K+ ion concentrations were shown to equilibrate across the cell membrane in our studies using the voltage-sensitive dye DiBAC4(5). The dependence of γ on the K+ activity (aK) was fit well by a modified Langmuir binding isotherm, with a nonzero intercept as aK approaches 0 mM, suggesting electrostatic surface charge effects. Following the addition of 100 mM N-methyl-d-glucamine (NMG+), a nonpermeant, nonblocking cation or following pretreatment with 50 mM trimethyloxonium (TMO), a carboxylic acid esterifying agent, the γ–aK relationship did not show nonzero intercepts, suggesting the presence of surface charges formed by glutamate or aspartate residues. Consistent with surface charges in Kir2.1 channels, the rates of current decay induced by Ba2+ block were slowed with the addition of NMG or TMO. Using a molecular model of Kir2.1 channels, three candidate negatively charged residues were identified near the extracellular mouth of the pore and mutated to cysteine (E125C, D152C, and E153C). E153C channels, but not E125C or D152C channels, showed hyperbolic γ–aK relationships going through the origin. Moreover, the addition of MTSES to restore the negative charges in E53C channels reestablished wild-type conductance properties. Our results demonstrate that E153 contributes to the conductance properties of Kir2.1 channels by acting as a surface charge.


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