1991
DOI: 10.1016/s0006-3495(91)82232-9
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Two-dimensional crystals of streptavidin on biotinylated lipid layers and their interactions with biotinylated macromolecules

Abstract: Streptavidin forms two-dimensional crystals when specifically bound to layers of biotinylated lipids at the air/water interface. The three-dimensional structure of streptavidin determined from the crystals by electron crystallography corresponds well with the structure determined by x-ray crystallography. Comparison of the electron and x-ray crystallographic structures reveals the occurrence of free biotin-binding sites on the surface of the two-dimensional crystals facing the aqueous solution. The free biotin… Show more

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Cited by 328 publications
(359 citation statements)
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“…Such crystals display two accessible biotin-binding sites per tetramer that can be used to bind biotinylated proteins (26). However, contrary to streptavidin, S-layer proteins form two-dimensional protein crystals by a robust self-assembly process that has been optimized by evolution.…”
Section: Discussionmentioning
confidence: 99%
“…Such crystals display two accessible biotin-binding sites per tetramer that can be used to bind biotinylated proteins (26). However, contrary to streptavidin, S-layer proteins form two-dimensional protein crystals by a robust self-assembly process that has been optimized by evolution.…”
Section: Discussionmentioning
confidence: 99%
“…The two-dimensional crystals of streptavidin can easily be formed on highly fluidic PLBs containing lipids with unsaturated alkyl chains (such as DOPC, dioleoylphosphatidylcholine) and a biotin-containing lipid (11,20). Their surface is particularly useful for the selective and stable immobilization of homo-oligomeric protein complexes because pinning the complexes at multiple biotinylated sites is possible (109).…”
Section: Substrate Surfacesmentioning
confidence: 99%
“…As discussed above, by linking the dyes to the AuNRs surface with the biotin/streptavidin conjugation, they are kept at an average distance of 5 nm from the metal, thus, avoiding the quenching of the plasmonicfluorescent nanoprobes. 30,31 At this distance, the still-appreciable field enhancement produced by the AuNR (see Figure 2 To demonstrate the potential of the AuNRs for NP-STED, we functionalized a glass cover-slip to attach the AuNRs to the surface (see Methods for further details) and compared the resolution improvement relative to confocal microscopy for the AuNR and for 20 nm diameter crimson red beads as a function of the power of the depletion-beam. Assuming that the depletion beam pulse length, , is much smaller than the fluorescence lifetime of the fluorophore, 1 , the resolution achievable with pulsed STED depends on the wavelength, λ, the numerical aperture (NA) of the objective, the peak intensity of the depletion beam, , and the saturation intensity of the fluorophore, , as given by: 16,32 Hence, we can write the STED resolution improvement with respect to confocal microscopy as Γ = √1 + ∅.…”
Section: Green (Blue) Line Is the Absorption (Emission) Spectrum Of Tmentioning
confidence: 99%