Why single-molecule techniques?

Life at the molecular scale is dominated by chemical reactions and interactions with energies close to the thermal energy, i.e. ~kT (k being the Boltzmann constant). These processes are stochastic and follow Boltzmann probability. Along their reaction pathway, biomolecules explore rare and metastable energy states, which may originate from a particular conformation or substrate. One of the signatures of these metastable states is a slow kinetic, i.e. a “pause” in the catalytic activity of the enzyme. In ensemble measurement, as usually performed in biology, such a rare event is averaged away from the ensemble behaviour. Therefore, a complete characterization of the dynamics of a biomolecule is unaccessible to ensemble techniques and requires different methods to access the dynamics of single molecules. To this end, single-molecule techniques are extremely appropriate, as they offer high spatial and temporal resolution to observe biomolecules one at a time. These techniques are divided between two main branches: force spectroscopy techniques, where macromolecules are spatially manipulated using laser, magnetic field or cantilever, and fluorescence spectroscopy techniques, where the biomolecule of interest is labeled with one or many fluorescent dyes to monitor its position and/or dynamics (1). The Dulin lab is specialized in magnetic tweezers and single-molecule FRET, which are respectively a force and a fluorescence spectroscopy technique, and are quickly described below.

Magnetic Tweezers

A magnetic tweezers assay is an inverted microscope that images a flow cell on top of which a magnetic field source, i.e. a pair of permanent magnets, is located. The magnetic field generate an attractive force on the surface-tethered magnetic bead, which stretches the nucleic acid tether (Figure 1A). The force increases when the distance between the magnets and the bead reduces. In addition to force, magnetic tweezers can also routinely apply torque to the a coilable nucleic acid molecule by rotating the magnets, which rotates the magnetic beads. Magnetic tweezers offers high throughput acquisition (2, 3, 4), i.e. up to ~800 nucleic acid tethered magnetic beads  can be followed simultaneously in real-time with a spatiotemporal resolution of sub nanometer at 1 s (Figure 1B). This capability is essential to explore rare kinetic events, as a large statistics is necessary to reconstitute their distribution in time – these events are stochastic – and understand their biochemical origin (6). Furthermore, magnetic tweezers are able to distinguish steps as small as a DNA base-pair from the noise (Figure 1C) (5).

Nucleic acids from all organisms are processed by different type of enzymes, such as polymerases and helicases (7). Polymerases belong to a family of enzymes responsible for the replication and the transcription of nucleic acids in all organisms. Single-molecule techniques have shown in the early 90s that the activity of these enzymes is interrupted by a variety of pauses with different biochemical origins. For example, magnetic tweezers have been used to study viral RNA-dependant RNA polymerase (RdRp) to explore the mechanism of mismatch nucleotide incorporation (Figure 2A) (3), a particularly rare event (~1 every 3000 incorporations in error-prone RNA viruses), or long non-catalytic pauses related to backtracking (8). High-throughput magnetic tweezers provides a unique tool to study quantitatively error incorporation (Figure 2B). Using a slightly different approach, where a hairpin replaces the double stranded nucleic acid to tether the magnetic bead, one is able to observe the unwinding activity of a replicative hexameric helicase (Figure 2C) (9). 

Single-molecule FRET

Fluorescence (or Förster, named after the first person who described this phenomenon theoretically) Resonance Energy Transfer (FRET) relies on the energy transfer between two close dyes (or fluorophores), of which the emission spectrum of one (donor) overlaps with the absorption spectrum of the other one (acceptor) (1). This technique can be employed either in ensemble or in single-molecule measurement. A fluorescent microscope is used to excite and observe the dyes, either in confocal or wide-field configuration (10). The later is represented in Figure 3A, in TIRFM (Total Internal Reflection Fluorescence Microscopy) conformation. Here, the total internal reflection of the excitation laser beam (green) produces an evanescent wave at the surface of the glass coverslip. This evanescent wave excites the donor dye and part of the energy from the donor is transferred to the acceptor as a function of the distance R. The fluorescence of both dyes is spectrally separated and collected on a sensitive camera. Because FRET efficiency varies as a function of the distance between the two dyes in the 2-10 nm range (Figure 3B), this technique offers an ideal tool to measure molecular distances in real-time (11).

For example, one can label with a FRET pair the two domains of a surface-attached biomolecule that experiences stochastic conformational changes between two states (Figure 4A). The magnitude of the conformational change is translated into the anti-correlated intensities of the donor and acceptor (Figure 4B). Using custom algorithm specialized in detecting step-like changes in FRET efficiency, e.g. Hidden Markhov Modelling (12), the dwell times of each state can be recovered (Figure 4C). From these dwell times, one builds up the dwell time distributions and models the kinetics of conformational change.


(1)    D. Dulin, J. Lipfert, C. M. Moolman, and N. H. Dekker
        Studying genomic processes at the single-molecule level : introducing the tools and applications

        Nat. Rev. Gen., 2012Vol. 14, 9

(2)    J. P. Cnossen, D. Dulin and N.H. Dekker
       An optimized software framework for real-time, high-throughput tracking of spherical beads
       Rev. Sci. Inst., 2014, Vol. 85, 103712

(3)    D. Dulin, I.D. Vilfan, B.A. Berghuis, S. Hage, D. Bamford, M. Poranen, M. Depken and N.H. Dekker
        Elongation-competent pauses govern the fidelity of a viral RNA-dependent RNA polymerase
        Cell Rep., 2015, Vol. 10, 983

(4)    B.A. Berghuis, D. Dulin, Z.-Q. Xu, T. van Laar, B. Cross, R. Janissen, S. Jergic, N. Dixon, M. Depken      and N.H. Dekker
        Strand separation suffices to establish a long-lived, foolproof DNA-protein lock at the Tus-Ter replication fork barrier
        Nat. Chem. Biol., 2015, Vol. 11, 579

(5)    D. Dulin, T.J. Cui, J. P. Cnossen, M. W. Docter, J. Lipfert and N.H. Dekker
        High Spatiotemporal Resolution Magnetic Tweezers : Calibration and Applications to DNA Dynamics
        Biophys. J., 2015, Vol. 109, 2113

(6)    D. Dulin, B. A. Berghuis, M. Depken and N.H. Dekker
        Untangling reaction pathways through modern approaches to high-throughput single-molecule force-spectroscopy experiments
        Curr. Op. Struct. Biol., 2015, Vol. 34, 116

(7)    B. Alberts

        Molecular Biology of the Cell


(8)    D. Dulin, I. D. Vilfan, B. A. Berghuis, M. Poranen, M. Depken and N.H. Dekker
        Backtracking behavior in viral RNA-dependent RNA polymerase provides the basis for a second initiation site
        Nucl. Acids Res., 2015, doi : 10.1093/nar/gkv1098

(9)    M. Manosas, M.M. Spiering,F. Ding,V. Croquette and S.J. Benkovic
        Collaborative coupling between polymerase and helicase for leading-strand synthesis.
        Nucl. Acids Res., 2012, 40, 6187

(10)  J Hohlbein, TD Craggs, T Cordes
        Alternating-laser excitation: single-molecule FRET and beyond

        Chem. Soc. Rev., 2012, 43 (17), 6472

(11)  R Roy, S Hohng, T Ha

        A practical guide to single-molecule FRET
        Nature methods, 2008, 5 (6), 507-516

(12)  SA McKinney, C Joo, T Ha

        Analysis of single-molecule FRET trajectories using hidden Markov modeling
        Biophys. J., 2006, 91 (5),  1941


Dulin Lab

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