DNA nanotechnology offers a promising approach to leverage the benefits of the PAINT concept while establishing a programmable target-probe interaction system. DNA-based PAINT (DNA-PAINT) has been developed as a straightforward approach to overcome some limitations of current localization-based super-resolution techniques (Dai
et al. 2016; Iinuma
et al. 2014; Jungmann
et al. 2010,
2014,
2016). DNA-PAINT decouples blinking from the photophysics of dye and introduces the programmability and specificity of using DNA molecules as imaging and labeling probes. A DNA-PAINT system comprises a docking strand and a complementary imager strand, both of which are short single-stranded DNA oligomers, usually 8–10 nucleotides long. The docking strand is attached to the target of interest using immunolabeling approaches with DNA-conjugated antibody pair targeting proteins of interest. The imager strand is conjugated to an organic dye and diffuses freely in the imaging buffer (
Fig. 1A). Generally, unbound imager strand signals appear imperceptible in the camera because they diffuse across multiple camera pixels during the exposure time. However, imager strands can transiently bind to docking strands owing to their complementary sequence. In a bound state, when imager strands remain anchored in place for an extended period, accumulating sufficient photons to be detected by a single camera pixel. The properties of DNA-PAINT offer several advantages over other SMLM approaches. Firstly, the use of DNA-based imaging probes enables high multiplexing using Exchange-PAINT limited only by the number of orthogonal DNA sequences, in contrast to the spectrally distinct dyes used in conventional multiplexing experiments (Jungmann
et al. 2014). Secondly, the predictability and tunability of DNA binding and unbinding events, coupled with the absence of bleaching, allow for accurate quantitative image interpretation, as implemented in quantitative PAINT (qPAINT) (Jungmann
et al. 2016). Thirdly, DNA-PAINT simplifies the selection of suitable dyes for imaging, as the parameter space is reduced from rather complex photophysical properties to basically one single parameter — the photon budget. Lastly, by programming the binding duration, a significantly higher number of photons can be detected from a single binding (or blink) event, leading to optimal localization precision.