Abstract

Actions of molecular species, for example binding of transcription factors to chromatin, may comprise several superimposed reaction pathways. The number and the rate constants of such superimposed reactions can in principle be resolved by inverse Laplace transformation of the corresponding distribution of reaction lifetimes. However, current approaches to solve this transformation are challenged by photobleaching-prone fluorescence measurements of lifetime distributions. Here, we present a genuine rate identification method (GRID), which infers the quantity, rates and amplitudes of dissociation processes from fluorescence lifetime distributions using a dense grid of possible decay rates. In contrast to common multi-exponential analysis of lifetime distributions, GRID is able to distinguish between broad and narrow clusters of decay rates. We validate GRID by simulations and apply it to CDX2-chromatin interactions measured by live cell single molecule fluorescence microscopy. GRID reveals well-separated narrow decay rate clusters of CDX2, in part overlooked by multi-exponential analysis. We discuss the amplitudes of the decay rate spectrum in terms of frequency of observed events and occupation probability of reaction states. We further demonstrate that a narrow decay rate cluster is compatible with a common model of TF sliding on DNA.

Highlights

  • IntroductionFor example binding of transcription factors to chromatin, may comprise several superimposed reaction pathways

  • Actions of molecular species, for example binding of transcription factors to chromatin, may comprise several superimposed reaction pathways

  • We further considered measurements of reaction lifetimes by single molecule fluorescence microscopy using fluorescent labels subject to photobleaching

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Summary

Introduction

For example binding of transcription factors to chromatin, may comprise several superimposed reaction pathways. To obtain the underlying reaction rates of TF – chromatin interactions, current analysis approaches avoid inverting the Laplace transform by describing the measured fluorescence survival time distributions with multi-exponential models with a fixed number of exponential functions but varying decay rates and amplitudes[8,10,11,31]. Such exponential fitting is robust but requires knowledge of the number of decay rates and is ill suited to resolve complex decay rate spectra with an unknown number of components

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