Electrostatic interactions of fluorescent molecules with dielectric interfaces studied by total internal reflection fluorescence correlation spectroscopy

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Abstract

Electrostatic interactions between dielectric surfaces and different fluorophores used in ultrasensitive fluorescence microscopy are investigated using objective-based Total Internal Reflection Fluorescence Correlation Spectroscopy (TIR-FCS). The interfacial dynamics of cationic rhodamine 123 and rhodamine 6G, anionic/dianionic fluorescein, zwitterionic rhodamine 110 and neutral ATTO 488 are monitored at various ionic strengths at physiological pH. As analyzed by means of the amplitude and time-evolution of the autocorrelation function, the fluorescent molecules experience electrostatic attraction or repulsion at the glass surface depending on their charges. Influences of the electrostatic interactions are also monitored through the triplet-state population and triplet relaxation time, including the amount of detected fluorescence or the count-rate-per-molecule parameter. These TIR-FCS results provide an increased understanding of how fluorophores are influenced by the microenvironment of a glass surface, and show a promising approach for characterizing electrostatic interactions at interfaces. © 2010 by the authors; licensee Molecular Diversity Preservation International.

Figures

  • Figure 1. Schematic of the objective-based TIR-FCS setup. L1–L3: lenses; TS: translator; DM: dichroic mirror; OL: objective lens; EMF: emission filter; M: mirror; TL: tube lens; BSP: beamsplitter plate; SPAD: single photon avalanche diode.
  • Figure 2. Schematic model of electric double layer. The negative surface charges (−) are counterbalanced by bound and free ions (+). The electrostatic surface potential is plotted for salt concentrations of 100 mM, 10 mM, 1 mM, and 0.1 mM, which gives Debye lengths of 0.95 nm (black curve), 3 nm (blue curve), 9.5 nm (green curve), and 30 nm (orange curve), respectively. The evanescent penetration depth is for comparison plotted in the red curve.
  • Figure 3. Autocorrelation curves for the cationic rhodamine 123 at ionic strengths of 100 mM (red curve), 10 mM (green curve) and 0.1 mM (blue curve). The correlation curves are fitted with Equation (4) to estimate the unknown parameters N , z , T , and t . To visualize the effect of the electrostatic interactions on the diffusion time, the curves have been normalized. The inset shows the unnormalized curves, which are used to visualize changes in concentration of molecules in the vicinity of the glass interface. At ionic strength of 100 mM: N = 0.62, z = 4.9 µs, T = 0.057 and t = 1.6 µs; at 10 mM: N = 0.96, z = 9.7 µs, T = 0.1 and t = 2.1 µs; at 0.1 mM: N = 1.93, z = 23.5 µs, T = 0.17 and t = 3.1 µs. Concentration of Rh123 was 20 nM.
  • Figure 4. Mean number of rhodamine 123 molecules in the TIR-FCS probe volume, N (red pentagon), and the ratio of molecules, Nx (green triangles), as a function of ionic strength. The inset shows the deduced mean surface potential of the electric double layer without (blue stars) and with (orange stars) correction for background contributions. Data points at 14 mM and 150 mM is done in PBS at pH = 7.2. Data points at 0.1 mM, 1 mM, 10 mM, and 100 mM are done at pH = 6.6.
  • Figure 5. The axial passage-time, z, for rhodamine 123, as function of ionic strength (purple squares), deduced by fitting the autocorrelation data with Equation (2). The inset shows the normalized axial passage-time (pink triangles).
  • Figure 6. (a) The SPAD detected fluorescence, F, as function of ionic strength (green hexagons). The inset shows the detected CCD intensities at 0.1 mM (left) and 150 mM (right) ionic strength. The camera images are presented with the same peak intensity setting and the diameter correspond to 20 µm in sample space. (b) The counts-rate-permolecule, CPM, as a function of ionic strength (red squares).
  • Figure 7. The triplet amplitude, T , describing the probability of the rhodamine 123 molecules to be in the triplet state, as function of ionic strength (green triangles). The inset shows the triplet relaxation time, T (pink squares).
  • Figure 8. The number of rhodamine 6G molecules, N (pink circles) in the TIR-FCS probe volume, as a function of ionic strength. The sample concentration was 50 nM and the values have been corrected for background contributions. The inset shows the axial passage-time, z (blue triangles).

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APA

Blom, H., Hassler, K., Chmyrov, A., & Widengren, J. (2010). Electrostatic interactions of fluorescent molecules with dielectric interfaces studied by total internal reflection fluorescence correlation spectroscopy. International Journal of Molecular Sciences, 11(2), 386–406. https://doi.org/10.3390/ijms11020386

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