Co-immunoprecipitation (co-IP) has become a standard technique, but its protein-band output provides only static, qualitative information about protein–protein interactions. Here we demonstrate a real-time single-molecule co-IP technique that generates real-time videos of individual protein–protein interactions as they occur in unpurified cell extracts. By analysing single Ras–Raf interactions with a 50-ms time resolution, we have observed transient intermediates of the protein–protein interaction and determined all the essential kinetic rates. Using this technique, we have quantified the active fraction of native Ras proteins in xenograft tumours, normal tissue and cancer cell lines. We demonstrate that the oncogenic Ras mutations selectively increase the active-Ras fraction by one order of magnitude, without affecting total Ras levels or single-molecule signalling kinetics. Our approach allows us to probe the previously hidden, dynamic aspects of weak protein–protein interactions. It also suggests a path forward towards precision molecular diagnostics at the protein–protein interaction level.

The bHLH transcription factor PHYTOCHROME INTERACTING FACTOR1 (PIF1) binds G-box elements in vitro and inhibits light-dependent germination in Arabidopsis thaliana. A previous genome-wide analysis of PIF1 targeting indicated that PIF1 binds 748 sites in imbibed seeds, only 59% of which possess G-box elements. This suggests the G-box is not the sole determinant of PIF1 targeting. The targeting of PIF1 to specific sites could be stabilized by PIF1-interacting transcription factors (PTFs) that bind other nearby sequence elements. Here, we report PIF1 targeting sites are enriched with not only G-boxes but also with other hexameric sequence elements we named G-box coupling elements (GCEs). One of these GCEs possesses an ACGT core and serves as a binding site for group A bZIP transcription factors, including ABSCISIC ACID INSENSITIVE5 (ABI5), which inhibits seed germination in abscisic acid signaling. PIF1 interacts with ABI5 and other group A bZIP transcription factors and together they target a subset of PIF1 binding sites in vivo. In vitro single-molecule fluorescence imaging confirms that ABI5 facilitates PIF1 binding to DNA fragments possessing multiple G-boxes or the GCE alone. Thus, we show in vivo PIF1 targeting to specific binding sites is determined by its interaction with PTFs and their binding to GCEs.

Extremely weak protein-protein interactions (PPIs), signified by micromolar or even millimolar dissociation constants, are one of the keys to understanding the rapid responses of cellular systems. Although single-molecule methods are particularly useful in determining kinetics of biological processes, their application is largely limited to rather strong interactions because of the diffraction-limited observation volume. In this study, we report a single-molecule method that allows the characterization of PPIs using a prey concentration 4 orders of magnitude lower than the dissociation constant. Instead of increasing the concentration of diffusing molecules, which is inevitably limited by the optical diffraction limit, we employed an increased density of surface bait protein. The low occupancy of the surface baits permitted determination of the kinetics with single-molecule resolution. We used this approach to study a PPI network consisting of Ras and its downstream proteins including full-length Rafs and catalytic subunits of phosphoinositide 3-kinase.

Intrinsically disordered proteins (IDPs) usually fold during binding to target proteins. In contrast to interactions between folded proteins, this additional folding step makes the binding process more complex. Understanding the mechanism of coupled binding and folding of IDPs requires analysis of binding pathways that involve formation of the transient complex (TC). However, experimental characterization of TC is challenging because it only appears for a very brief period during binding. Here, we use single-molecule fluorescence spectroscopy to investigate the mechanism of diffusion-limited association of an IDP. A large enhancement of the association rate is observed due to the stabilization of TC by non-native electrostatic interactions. Moreover, photon-by-photon analysis reveals that the lifetime of TC for IDP binding is at least two orders of magnitude longer than that for binding of two folded proteins. This result suggests the long lifetime of TC is generally required for folding of IDPs during binding processes.

We describe theory, experiments, and analyses of three-color Förster resonance energy transfer (FRET) spectroscopy for probing sub-millisecond conformational dynamics of protein folding and binding of disordered proteins. We devise a scheme that uses single continuouswave laser excitation of the donor instead of alternating excitation of the donor and one of the acceptors. This scheme alleviates photophysical problems of acceptors such as rapid photobleaching, which is crucial for high time resolution experiments with elevated illumination intensity. Our method exploits the molecular species with one of the acceptors absent or photobleached, from which two-color FRET data is collected in the same experiment. We show that three FRET efficiencies and kinetic parameters can be determined without alternating excitation from a global maximum likelihood analysis of two-color and three-color photon trajectories. We implement co-parallelization of CPU-GPU processing, which leads to a significant reduction of the likelihood calculation time for efficient parameter determination.

Coimmunoprecipitation (co-IP) analysis is a useful method for studying protein-protein interactions. It currently involves electrophoresis and western blotting, which are not optimized for detecting weak and transient interactions. In this protocol we describe an advanced version of co-IP analysis that uses real-time, single-molecule fluorescence imaging as its detection scheme. Bait proteins are pulled down onto the imaging plane of a total internal reflection (TIR) microscope. With unpurified cells or tissue extracts kept in reaction chambers, we observe single protein-protein interactions between the surface-immobilized bait and the fluorescent protein-labeled prey proteins in real time. Such direct recording provides an improvement of five orders of magnitude in the time resolution of co-IP analysis. With the single-molecule sensitivity and millisecond time resolution, which distinguish our method from other methods for measuring weak protein-protein interactions, it is possible to quantify the interaction kinetics and active fraction of native, unlabeled bait proteins. Real-time single-molecule co-IP analysis, which takes ∼4 h to complete from lysate preparation to kinetic analysis, provides a general avenue for revealing the rich kinetic picture of target protein-protein interactions, and it can be used, for example, to investigate the molecular lesions that drive individual cancers at the level of protein-protein interactions.

The cosolvent effect arises from the interaction of cosolute molecules with a protein and alters the equilibrium between native and unfolded states. Denaturants shift the equilibrium toward the latter, while osmolytes stabilize the former. The molecular mechanism whereby cosolutes perturb protein stability is still the subject of considerable debate. Probing the molecular details of the cosolvent effect is experimentally challenging as the interactions are very weak and transient, rendering them invisible to most conventional biophysical techniques. Here, we probe cosolute–protein interactions by means of NMR solvent paramagnetic relaxation enhancement together with a formalism we recently developed to quantitatively describe, at atomic resolution, the energetics and dynamics of cosolute–protein interactions in terms of a concentration normalized equilibrium average of the interspin distance, 〈r−6〉norm, and an effective correlation time, τc. The system studied is the metastable drkN SH3 domain, which exists in dynamic equilibrium between native and unfolded states, thereby permitting us to probe the interactions of cosolutes with both states simultaneously under the same conditions. Two paramagnetic cosolute denaturants were investigated, one neutral and the other negatively charged, differing in the presence of a carboxyamide group versus a carboxylate. Our results demonstrate that attractive cosolute–protein backbone interactions occur largely in the unfolded state and some loop regions in the native state, electrostatic interactions reduce the 〈r−6〉norm values, and temperature predominantly impacts interactions with the unfolded state. Thus, destabilization of the native state in this instance arises predominantly as a consequence of interactions of the cosolutes with the unfolded state.

Rotation of single membrane receptors can be observed by examination of polarized optical signals from receptor-bound asymmetric nanoparticles such as fluorescent quantum dots (QD) or nanogold. For example, we have examined the slow, hindered rotation of the Type I Fce receptor (FceRI) on 2H3 RBL cells using polarized fluorescence imaging of receptor-bound Qdot655. With imaging methods, only receptor rotational correlation times (RCT) slower than the camera frame time can be examined and suitable low-light cameras typically require 1ms or longer per frame. However, time-resolved phosphorescence anisotropy shows the hydrodynamic RCT of FcεRI to be about 40 ms at 25 C. To examine such rapid reorientation, an alternate approach is to illuminate individual QD on the cell surface with a focused laser beam, collect fluorescence using a confocal detector and direct signals polarized parallel and perpendicular to the laser polarization into separate APD detectors. A timetagged single photon counter records the channel of each detected photon and its arrival time with a precision of 165 ps. The auto-and crosscorrelations of the two signals are calculated directly from arrival times without binning, combined using adjustable constants such as the g-factor, and these constants optimized to obtain the maximum statistical independence between the anisotropy and intensity time-autocorrelation functions (TAC). While RCTs below 1 ns are theoretically accessible, useful rotational information exists only when RCT*photon count rate R 1. Thus, given photon count rates, our data potentially provide information on RCTs R 20 ms. However, intensity changes due to QD blinking may feed through to some extent into calculated anisotropies and thus slightly distort apparent anisotropy TAC decay shapes. Efforts aimed at removing this possible complication are underway.