Abstract

The observation of molecular diffusion at different spatial scales, and in particular below the optical diffraction limit (<200 nm), can reveal details of the subcellular topology and its functional organization. Stimulated-emission depletion microscopy (STED) has been previously combined with fluorescence correlation spectroscopy (FCS) to investigate nanoscale diffusion (STED-FCS). However, stimulated-emission depletion fluorescence correlation spectroscopy has only been used successfully to reveal functional organization in two-dimensional space, such as the plasma membrane, while, an efficient implementation for measurements in three-dimensional space, such as the cellular interior, is still lacking. Here we integrate the STED-FCS method with two analytical approaches, the recent separation of photons by lifetime tuning and the fluorescence lifetime correlation spectroscopy, to simultaneously probe diffusion in three dimensions at different sub-diffraction scales. We demonstrate that this method efficiently provides measurement of the diffusion of EGFP at spatial scales tunable from the diffraction size down to ∼80 nm in the cytoplasm of living cells.

Highlights

  • The observation of molecular diffusion at different spatial scales, and in particular below the optical diffraction limit (

  • fluorescence correlation spectroscopy (FCS) has been combined with stimulatedemission depletion (STED) microscopy[5] (STED-FCS) to study diffusion of molecules at a spatial scale well below the limit imposed by the diffraction of light[6–8]

  • As a matter of fact, even if Stimulated-emission depletion microscopy (STED) microscopy is fully compatible with 3D samples, as it has been largely demonstrated for imaging[15], direct observations of nanoscale diffusion in 3D environments by STED-FCS have been quite limited[6, 8, 16–18], and mostly do not deal with the analysis of molecular diffusion within the cell interior

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Summary

Introduction

The observation of molecular diffusion at different spatial scales, and in particular below the optical diffraction limit (

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