Super-resolution microscopy is a series of super-resolution imaging techniques in optical microscopy that allow such images to have resolutions higher than those imposed by the diffraction limit, which is due to the diffraction of light. Super-resolution imaging techniques rely on the near-field (photon-tunneling microscopy as well as those that use the Pendry Superlens and near field scanning optical microscopy) or on the far-field. Among techniques that rely on the latter are those that improve the resolution only modestly (up to about a factor of two) beyond the diffraction-limit, such as confocal microscopy with closed pinhole or aided by computational methods such as deconvolution or detector-based pixel reassignment (e.g. re-scan microscopy, pixel reassignment), the 4Pi microscope, and structured-illumination microscopy technologies such as SIM and SMI. There are two major groups of methods for super-resolution microscopy in the far-field that can improve the resolution by a much larger factor:
Deterministic super-resolution: the most commonly used emitters in biological microscopy, fluorophores, show a nonlinear response to excitation, which can be exploited to enhance resolution. Such methods include STED, GSD, RESOLFT and SSIM. Stochastic super-resolution: the chemical complexity of many molecular light sources gives them a complex temporal behavior, which can be used to make several nearby fluorophores emit light at separate times and thereby become resolvable in time. These methods include super-resolution optical fluctuation imaging (SOFI) and all single-molecule localization methods (SMLM), such as SPDM, SPDMphymod, PALM, FPALM, STORM, and dSTORM. On 8 October 2014, the Nobel Prize in Chemistry was awarded to Eric Betzig, W.E. Moerner and Stefan Hell for "the development of super-resolved fluorescence microscopy", which brings "optical microscopy into the nanodimension". The different modalities of super-resolution microscopy are increasingly being adopted by the biomedical research community, and these techniques are becoming indispensable tools to understanding biological function at the molecular level.
History By 1978, the first theoretical ideas had been developed to break the Abbe limit, which called for using a 4Pi microscope as a confocal laser-scanning fluorescence microscope where the light is focused from all sides to a common focus that is used to scan the object by 'point-by-point' excitation combined with 'point-by-point' detection. However the publication from 1978 had drawn an improper physical conclusion (i.e. a point-like spot of light) and had completely missed the axial resolution increase as the actual benefit of adding the other side of the solid angle. Some of the following information was gathered (with permission) from a chemistry blog's review of sub-diffraction microscopy techniques. In 1986, a super-resolution optical microscope based on stimulated emission was patented by Okhonin.
Super-resolution techniques
Photon tunneling microscopy (PTM) Photon tunneling microscopy (PTM) provides real-time whole-field non-scanning imaging with sub-wavelength lateral resolution and vertical resolution as low as 1 nanometer, as demonstrated by John M. Guerra. (Note the differentiation of PTM with photon scanning tunneling microscopy (PSTM), which is essentially a re-naming of near-field scanning optical microscopy (NSOM) that exploits the near-field from a sharp optical fiber tip positioned extremely close to the sample surface, typically within a few nanometers, such that when the fiber is scanned along the sample surface an image is built up). PTM provides sub-wavelength spatial resolution due to its capture of bound high-frequency diffracted light at the sample and conversion into image-forming propagating light. Easy insertion of the sample surface into the evanescent field at the distal end of the microscope is provided by a flexible "transducer" of a polymer or thin glass that is placed proximal to the sample. This transducer is flexible enough to follow macro-curves on the sample while providing a stiff flat reference locally. The vertical resolution is limited only by the photometric resolution of the whole-field detector, and can be as low as 1 nanometer. The technique has been applied to biological and solid-state samples, offering insights into surface morphology and optical properties at the nanoscale.
Phase-shifted PTM aka Phase-shifted Evanescent field Microscopy (PEM) In further development of this work in 1996, John M. Guerra showed that super-resolved lateral topography even higher than is achieved with PTM is attained by phase-shifting the evanescent field. In propagating light, planes of equal phase are parallel to planes of equal amplitude, such that phase-shifting produces sub-wavelength super-resolution along the vertical axis, such as achieved with interferometers produced by WYKO and ZYGO for measurement of optical surfaces. However, the evanescent field is inhomogeneous in that the planes of equal amplitude are parallel to the sample surface (thus the high vertical resolution in PTM), while the planes of equal phase are perpendicular to them and to the surface. Shifting the phase therefore now can produce sub-wavelength super-resolution in the lateral axis that is even higher than that of PTM. While there are many ways to initiate this phase shift, as taught by Guerra in several U.S. patents assigned to the Polaroid Corporation, the first demonstration employed a Meadowlark Optics phase retarder and polarizer combination. Subtracting consecutive images for which the phase was shifted by a small value produced resolution Licenses to this technology were procured by Dyer Energy Systems, Calimetrics Inc., and Nanoptek Corp. for use of this super-resolution technique in optical data storage and microscopy. In 2001, with Dmitri Vezenov, Guerra published a fully-resolved image of 200nm spheres, close-packed hexagonally, while illuminated with 650nm light, for a resolution of 0.3 lambda. While impressive, potential resolution can be much higher, as it is limited only by the magnitude of the phase-shift.
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