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Single-Molecule Experiments

The details of the time-dependence of the ionic current bear information on the manner in which polymer molecules attempt to translocate through a pore and the underlying molecular mechanism of polymer threading. Experiments show that the average translocation time, for single-file translocation processes. [Pg.5]

This counterintuitive finding is in direct opposition to the linear increase of x with N for single-file transloeation through pores. [Pg.6]


Kulzer F, Koberling F, Christ T, Mews A and Basche T 1999 Terrylene in p-terphenyl single-molecule experiments at... [Pg.2508]

We hope to have convinced the reader by now that the tunneling centers in glasses are complicated objects that would have to be described using an enormously big Hilbert space, currently beyond our computational capacity. This multilevel character can be anticipated coming from the low-temperature perspective in Lubchenko and Wolynes [4]. Indeed, if a defect has at least two alternative states between which it can tunnel, this system is at least as complex as a double-well potential—clearly a multilevel system, reducing to a TLS at the lowest temperatures. Deviations from a simple two-level behavior have been seen directly in single-molecule experiments [105]. In order to predict the energies at which this multilevel behavior would be exhibited, we first estimate the domain wall mass. Obviously, the total mass of all the atoms in the droplet... [Pg.144]

In general, neither the force nor the molecular extension can be controlled in the experiments so definitions in Eqs. (96), (98), and (99) result in approximations to the true mechanical work that satisfy Eqs. (40) and (41). The control parameter in single molecule experiments using optical tweezers is the distance between the center of the trap and the immobilized bead [88]. Both the position of the bead in the trap and the extension of the handles are fluctuating quantities. It has been observed [94—96] that in pulhng experiments the proper work that satisfies the FT includes some corrections to Eqs. (97) and (99) mainly due to the effect of the trapped bead. There are two considerations to take into account when analyzing experimental data. [Pg.69]

F. Ritort, Single molecule experiments in biological physics methods and applications. J. Phys. (Condensed Matter) 18, R531-R583 (2006). [Pg.118]

G. Hummer and A. Szabo, Free-energy reconstruction from nonequilibrium single-molecule experiments. Proc. Natl. Acad. Set USA 98, 3658-3661 (2001). [Pg.118]

Selection of each laser depends on whether or not the experiment involves time-resolved measurement and what wavelength is suitable to exciting the target molecules. Note, that for single-molecule experiments a laser beam was circularly polarized using a Babinet-Soleil compensator to irradiate uniformly target molecules. All of the experiments otherwise unspecified were carried out at room temperature (23°C) in a clean-air booth (class 1000). [Pg.461]

The single-molecule experiments illustrated that the interaction between CV molecules and the polymer matrix is strongly site-dependent and bimodal nature. [Pg.486]

RNA fragments longer than 40—50 nucleotides are most often synthesized by in vitro transcription with T7 RNA polymerase. Heterogeneity of transcripts obtained by this method must be recognized by researchers aiming to use such transcripts for ligations, as it can lead to serious artifacts that are especially notable in single molecule experiments. [Pg.57]

In addition to proflavin and rhodamine, the photobleaching-resistant Cy3 and Cy5 fluorophores are also frequently used in single-molecule experiments and have been incorporated in the form of hydrazide derivatives into tRNAs via D residues (Pan et al., 2009) (Fig. 4.2). However, quantitative uptake of these hydrazide dyes requires modification of three reaction parameters higher concentrations of the hydrazide dyes (40 mM) than that required for proflavin or rhodamine (22 mM), pH 3.7 rather than pH 3.0, and 2 h reaction time instead of 45—90 min. The requirement of higher concentration is to promote formation of hydrazide adduct, while the slighdy elevated pH prevents hydrolysis of the adduct, which is acid labile. Thus, while the labeling method can be adapted to incorporate new fluorophores besides proflavin and rhodamine, it is prudent to systematically evaluate for the fluorophores under consideration for coupling efficiency as a function of dye concentration, pH, and reaction time. [Pg.83]

As a comparison, fluorescent labeling of tRNA with PyC is achieved in one step by the CCA enzyme, and thus is conceptually and technically simpler than labeling of tRNA with proflavin, rhodamine, or Cy3 and Cy5-hydrazides via D residues. However, the fluorescence emission intensity of PyC is not as high as those of the other fluorophores and thus may not be suitable for single-molecule experiments. Nonetheless, enzymatic labeling of tRNA with PyC is easy to implement and should be applicable to all tRNA sequences (both wild type and mutants), which can be generated by in vitro transcription without the requirement for a specific modification or for native tRNA species. [Pg.89]

Since PELDOR is not a single molecule experiment, the PELDOR signal V(t) contains not only the contribution from the interaction between the two spins in one molecule but also from the interaction between spins on different molecules and is thus considered a product of two contributions (Eq. (16.1), Fig. 16.2A) (Milov etal, 1984). [Pg.333]

M in concentration. This is in the range required for single-molecule detection. These sensitivity levels have been obtained on colloidal clusters at near-infrared excitation. Figure 10.3 is a schematic representation of a single-molecule experiment performed in a gold or silver colloidal solution. The analyte is provided as a solution at concentrations smaller than 10-11 M, Table 10.1 lists the anti-Stokes/Stokes intensity ratios for crystal violet (CY) at 1174 cm-1 using 830-nm near-infrared radiation well away from the resonance absorption of CY with a power of 106 W/cm2 [34]. CV is attached to various colloidal clusters as indicated in the table. Raman cross sections of 10-16 cm2/molecule or an enhancement factor of 1014 can be inferred from the data. [Pg.420]

Eckel, R., Wilking, S.D., Becker, A., Sewald, N., Ros, R. and Anselmetti, D. (2005b) Single molecule experiments in synthetic biology - A new approach for the affinity ranking of DNA-binding peptides. Angew. Chem. Int. Ed. 44,3921-3924. [Pg.319]

Although it has been difficult to separate the effects of excitation and emission enhancement, both of these effects should be extremely sensitive functions of the shape of the metal particle, the orientation of the fluorophore, and the distance between the fluorophore and the metal, because the local-field effects depend strongly on these parameters. Many groups have studied variations in fluorescence intensity as a function of the distance between a layer of fluorophores and a number of nanostructured metal surfaces, adsorbed colloidal particles or suspended colloidal particles. Single-molecule experiments have even provided strong evidence for the existence of a local maximum in the fluorescence intensity versus distance curve. ... [Pg.92]

How Biomolecular Motors Work Synergy Between Single Molecule Experiments and Single Molecule Simulations... [Pg.4]


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See also in sourсe #XX -- [ Pg.3 ]




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