Plenary Special Lectures doi:10.1017/S1431927611000705 NANOSCOPY WITH FOCUSED LIGHT
StefanW.Hell Max Planck Institute for Biophysical Chemistry, Department of NanoBiophotonics, 37077 Göttingen & German Cancer Research Center (DKFZ), Optical Nanoscopy Division, 69120 Heidelberg, Germany
For more than a century, it has been generally accepted that the resolution of a lens-based optical microscope is limited to about d l/~2NA!. 200 nm in the focal plane and .500 nm along the optic axis, with NA denoting the numerical aperture of the lens and l the wavelength of light. The discovery in the 1990s that elementary transitions between the states of a fluorophore can be used to eliminate the limiting role of diffraction has led to light microscopy concepts with resolution on the nanometer scale @1, 2#. Currently, all existing and successfully applied nanoscopy methods share a common enabling element: they switch the fluorescence capability of fluorophores on and off, so that adjacent features are registered sequentially in time @3, 4#. For example, in a typical Stimulated Emission Depletion ~STED! microscope @1#, the fluorophores are switched off
registration. The resolution is now given by the smaller diameter d l/~2NAM1I/Is! of this area in which the fluorophores are still fluorescent. I is the intensity of the STED beam, which, for I
~ kept dark! by overlapping the excitation beam with a de-exciting ~STED! beam which effectively confines the fluorophores to the ground state everywhere in the focal region except at a tiny area where the STED beam is close to zero. Fluorophores that are located in this subdiffraction-sized smaller area are registered. Scanning the beams further in space registers those fluorophores that had been switched off initially. An image of the whole object is assembled by sequential
Is, entails d r 0, meaning that the
resolution is conceptually no longer limited by l. An unprecedented, all-physics-based, far-field optical resolution of ,6nm was realized with nitrogen-vacancy centers in diamonds ~Fig. 1!@5#. The combination with 4Pi microscopy enabled an axial spatial resolution ,35 nm @2#. STED microscopy has been used to investigate the fate of synaptic vesicle proteins after exocytosis @6#, to reveal nanoscale patterns of synaptophysin on endosomes @7#, or to study the nanoscale distributions of TOM-complexes in the outer membrane of mitochondria @8#, thus demonstrating the potential of emerging “fluorescence nanoscopy” for the life sciences.A video-rate STED microscope was used to describe the mobility of vesicles inside the axons of cultured living neurons @9#. Live-cell STED microscopy has also been used to image activity-dependent morphological plasticity of dendritic spines @10#, while it also revealed that single sphingolipids, but not phospholipids, are transiently ~,10 ms! and locally ~,20 nm! trapped in a living cell membrane, mediated by cholesterol @11#.Multicolor operation @12, 13# facilitates colocalization of biomolecules. Importantly, the concept of STED microscopy has been expanded to lowintensity operation by switching the fluorophore
to a long-lived dark ~triplet! state or between a “fluorescence activated” and a “deactivated” ~conformational! state @2# as encountered in switchable fluorescent proteins @14#.More recent but seminal nanoscopy schemes such as PALM,STORM,and also GSDIM switch the molecules individually and stochastically. Switching is realized to a state that emits m .
. 1 detectable
photons in a rowbefore returning to a dark state, allowing the calculation of their position. These single fluorophore switching concepts @15–19# require only one switching cycle @3, 4# per fluorophore. This greatly extends the power of the switching concept for subdiffraction separation. These schemes have also been expanded tomulticolor operation ~Fig. 2! and combined with 4Pi-microscopy to also boost the axial resolution @20#. Altogether, lens-based optical nanoscopy is an unexpected and fascinating development in the physical sciences that is poised to impact many areas, in particular the life sciences.
References @1# S.W. Hell et al., Opt. Lett. 19 ~1994! 780. @2# S.W. Hell, Nature Biotech. 21 ~2003! 1347. @3# S.W. Hell, Science 316 ~2007! 1153. @4# S.W. Hell, Nature Meth. 6 ~2009! 24. @5# E. Rittweger et al., Nature Phot. 3 ~2009! 144. @6# K.I.Willig et al., Nature 440 ~2006! 935. @7# R. Schmidt et al., Nature Meth. 5 ~2008! 539. @8# G. Donnert et al., PNAS 103 ~2006! 11440. @9# V.Westphal et al., Science 320 ~2008! 246. @10# U.V. Nagerl et al., PNAS 105 ~2008! 18982.
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@11# C. Eggeling et al., Nature 457 ~2009! 1159. @12# I. Testa et al., Biophys. J. 99 ~2010! 2686. @13# J. Bückers et al., Opt. Express 19 ~2011! 3130. @14# M. Hofmann et al., PNAS 102 ~2005! 17565. @15# E. Betzig et al., Science 313 ~2006! 1642. @16# M.J. Rust et al., Nature Meth. 3 ~2006! 793. @17# S.T. Hess et al., Biophys. J. 91 ~2006! 4258. @18# A. Egner et al., Biophys. J. 93 ~2007! 3285. @19# J. Fölling et al., Nature Meth. 5 ~2008! 943. @20# D. Acquino et al., Nature Meth. 8 ~2011! 353.
Microscopy Microanalysis
AND © MICROSCOPY SOCIETY OF AMERICA 2011
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