Nanoscale elongating control of the self-assembled protein filament with the cysteine-introduced building blocks.

Self-assembly of artificially designed proteins is extremely desirable for nanomaterials. Here we show a novel strategy for the creation of self-assembling proteins, named "Nanolego." Nanolego consists of "structural elements" of a structurally stable symmetrical homo-oligomeric protein and "binding elements," which are multiple heterointeraction proteins with relatively weak affinity. We have established two key technologies for Nanolego, a stabilization method and a method for terminating the self-assembly process. The stabilization method is mediated by disulfide bonds between Cysteine-residues incorporated into the binding elements, and the termination method uses "capping Nanolegos," in which some of the binding elements in the Nanolego are absent for the self-assembled ends. With these technologies, we successfully constructed timing-controlled and size-regulated filament-shape complexes via Nanolego self-assembly. The Nanolego concept and these technologies should pave the way for regulated nanoarchitecture using designed proteins.

Dynamic force spectroscopy of the specific interaction between the PDZ domain and its recognition peptides.

To characterize the molecular basis of specific interactions of PDZ proteins, dynamic force spectroscopy (DFS) for the PDZ protein Tax-interacting protein-1 (TIP-1) and its recognition peptide (PDZ-pep) derived from beta-catenin was performed using an atomic force microscope (AFM), together with measurement of thermodynamic and kinetic parameters using surface plasmon resonance (SPR). The unbinding force of this pair was measured under different conditions of AFM tip-retraction velocity. The relationship between the unbinding force and the logarithmic force-loading rate, that is, the dynamic force spectrum, exhibited two different rate regimes, for each of which the forces increased linearly with the force-loading rate. On the basis of the theoretical treatment of the Bell-Evans model, the positions of two different activation barriers in the reaction coordinate and dissociation rate constants in each barrier were evaluated from slopes and x-intercepts of the two linear regimes (first barrier: 0.04 nm and 1.10 x 10 s(-1); second barrier: 0.21 nm and 2.77 x 10(-2) s(-1), respectively). Although two-step unbinding kinetics between TIP-1 and PDZ-pep was suggested from the DFS analysis, SPR results showed single-step dissociation kinetics with a rate constant of 2.89 x 10(-1) s(-1). Different shapes of the free energy profile of the unbinding process were deduced from each result of DFS and SPR. The reason for such topographic differences in the energy landscape is discussed in relation to the differences in the pathways of forced unbinding and spontaneous dissociation.

Force measurement for antigen-antibody interaction by atomic force microscopy using a photograft-polymer spacer.

To determine the intermolecular force on protein-protein interaction (PPI) by atomic force microscopy (AFM), a photograft-polymer spacer for protein molecules on both surfaces of the substrate and AFM probe tip was developed, and its effectiveness was assessed in a PPI model of a pair of human serum albumin (HSA) and its monoclonal antibody (anti-HSA). A carboxylated photoiniferter, N-(dithiocarboxy)sarcosine, was derivatized on both surfaces of the glass substrate and AFM probe tip, and subsequently water-soluble nonionic vinyl monomers, N,N-dimethylacrylamide (DMAAm), were graft-polymerized on them upon ultraviolet light irradiation. DMAAm-photograft-polymerized spacers with carboxyl groups at the growing chain end but with different chain lengths on both surfaces were prepared. The proteins were covalently bound to the carboxyl terminus of the photograft-polymer chain using a water-soluble condensation agent. The effects of the graft-spacer length on the profile of the force-distance curves and on the unbinding characteristics (unbinding force and unbinding distance) were examined in comparison with those in the case of the commercially available poly(ethylene glycol) (PEG) spacer. The frequency of the nonspecific adhesion force profile was markedly decreased with the use of the photograft spacers. Among the force curves detected, a high frequency of single-peak curves indicating the unbinding process of a single pair of proteins and a very low frequency of multiple-peak profiles were observed for the photograft spacers, regardless of the graft chain length, whereas a high frequency of no-force peaks was noted. These observations were in marked contrast with those for the PEG spacer. The force peak values determined ranged from 88 to 94 pN, irrespective of the type of spacer, while the standard deviation of force distribution observed for the photograft spacer was lower than that for the PEG spacer, indicating that the photograft spacers provide a higher accuracy of force determination.