MCL-1 promiscuity and the structural resilience of its binding partners.

The allosteric protein MCL-1 and its natural inhibitors, the BH3-only proteins PUMA, BIM, and NOXA regulate apoptosis by interacting promiscuously within an entangled binding network. Little is known about the transient processes and dynamic conformational fluctuations that are the basis for the formation and stability of the MCL-1/BH3-only complex. In this study, we designed photoswitchable versions of MCL-1/PUMA and MCL-1/NOXA, and investigated the protein response after an ultrafast photo-perturbation with transient infrared spectroscopy. We observed partial α-helical unfolding in all cases, albeit on strongly varying timescales (1.6 ns for PUMA, 9.7 ns for the previously studied BIM, and 85 ns for NOXA). These differences are interpreted as a BH3-only-specific "structural resilience" to defy the perturbation while remaining in MCL-1's binding pocket. Thus, the presented insights could help to better understand the differences between PUMA, BIM, and NOXA, the promiscuity of MCL-1, in general, and the role of the proteins in the apoptotic network.

The molecular mechanism of light-induced bond formation and breakage in the cyanobacteriochrome TePixJ.

Cyanobacteriochromes (CBCRs) are small and versatile photoreceptor proteins with high potential for biotechnological applications. Among them, the so-called DXCF-CBCRs exhibit an intricate secondary photochemistry: miliseconds after activation with light, a covalent linkage between a conserved cysteine residue and the light-absorbing tetrapyrrole chromophore is reversibly formed or broken. We employed time-resolved IR spectroscopy over ten orders of magnitude in time in conjunction with 2D-IR spectroscopy to investigate the molecular mechanism of this intriguing reaction in the DXCF-CBCR model system TePixJ from T. elongatus. The crosspeak pattern in the 2D-IR spectrum facilitated the assignment of the dominant signals to vibrational modes of the chromophore, which in turn enabled us to construct a mechanistic model for the photocycle reactions from the time-resolved IR spectra. Here, we assigned the time-resolved signals to several proton transfer steps and distinct geometric changes of the chromophore. We propose a model that describes how these events lead to the rearrangement of charges in the chromophore binding pocket, which serves as the trigger for the light-induced bond formation and breakage with the nearby cysteine.

Signal Propagation Within the MCL-1/BIM Protein Complex.

The protein MCL-1 is a crucial factor in regulating apoptosis, the programmed cell death, and thus plays a major role in numerous cancer types. The allosteric protein MCL-1 is naturally moderated by the BH3-only peptide BIM, which binds at its canonical binding groove. In its isolated form, BIM is disordered but assumes an α-helical shape when bound by MCL-1. The underlying binding mechanism (i.e., induced fit vs conformational selection), as well as the time scales of the signal cascade subsequent to binding, are not understood. Here, an artificially photoswitchable variant of the MCL-1/BIM complex was designed and investigated by transient infrared spectroscopy. By destabilizing the α-helix of BIM with a covalently linked azobenzene photoswitch, the dynamical response of the whole complex upon an ultrafast photo-perturbation was characterized. While the destabilized and partially unfolded BIM still binds to MCL-1, a step-like cascade of structural rearrangements of both, MCL-1 and BIM was detected, spanning a wide range of time scales from pico- to microseconds. The results indicate that BIM binds according to an induced fit mechanism, while the structural adaptations of MCL-1 may constitute an allosteric signal.

Sequence of Events during Peptide Unbinding from RNase S: A Complete Experimental Description.

The phototriggered unbinding of the intrinsically disordered S-peptide from the RNase S complex is studied with the help of transient IR spectroscopy, covering a wide range of time scales from 100 ps to 10 ms. To that end, an azobenzene moiety has been linked to the S-peptide in a way that its helicity is disrupted by light, thereby initiating its complete unbinding. The full sequence of events is observed, starting from unfolding of the helical structure of the S-peptide on a 20 ns time scale while still being in the binding pocket of the S-protein, S-peptide unbinding after 300 µs, and the structural response of the S-protein after 3 ms. With regard to the S-peptide dynamics, the binding mechanism can be classified as an induced fit, while the structural response of the S-protein is better described as conformational selection.

The Speed of Allosteric Signaling Within a Single-Domain Protein.

While much is known about different allosteric regulation mechanisms, the nature of the allosteric signal and the time scale on which it propagates remains elusive. The PDZ3 domain from postsynaptic density-95 protein is a small protein domain with a terminal third α-helix, i.e., the α3-helix, which is known to be allosterically active. By cross-linking the allosteric helix with an azobenzene moiety, we obtained a photocontrollable PDZ3 variant. Photoswitching triggers its allosteric transition, resulting in a change in binding affinity of a peptide to the remote binding pocket. Using time-resolved infrared and UV/vis spectroscopy, we follow the allosteric signal transduction and reconstruct the timeline in which the allosteric signal propagates through the protein within 200 ns.