Optimal 3D single-molecule localization for superresolution microscopy with aberrations and engineered point spread functions
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Edited* by Margaret M. Murnane, University of Colorado at Boulder, Boulder, CO, and approved October 27, 2011 (received for review June 3, 2011)

Abstract
Photo-activation localization microscopy is a far-field superresolution imaging technique based on the localization of single molecules with subdiffraction limit precision. Known under acronyms such as PALM (photo-activated localization microscopy) or STORM (stochastic optical reconstruction microscopy), these techniques achieve superresolution by allowing only a sparse, random set of molecules to emit light at any given time and subsequently localizing each molecule with great precision. Recently, such techniques have been extended to three dimensions, opening up unprecedented possibilities to explore the structure and function of cells. Interestingly, proper engineering of the three-dimensional (3D) point spread function (PSF) through additional optics has been demonstrated to theoretically improve 3D position estimation and ultimately resolution. In this paper, an optimal 3D single-molecule localization estimator is presented in a general framework for noisy, aberrated and/or engineered PSF imaging. To find the position of each molecule, a phase-retrieval enabled maximum-likelihood estimator is implemented. This estimator is shown to be efficient, meaning it reaches the fundamental Cramer–Rao lower bound of x, y, and z localization precision. Experimental application of the phase-retrieval enabled maximum-likelihood estimator using a particular engineered PSF microscope demonstrates unmatched low-photon-count 3D wide-field single-molecule localization performance.
Footnotes
- ↵1To whom correspondence should be addressed. E-mail: piestun{at}colorado.edu.
Author contributions: S.Q. and R.P. designed research; S.Q. and S.R.P.P. performed research; S.Q. and R.P. analyzed data; and S.Q. and R.P. wrote the paper.
The authors declare no conflict of interest.
*This Direct Submission article had a prearranged editor.
This article contains supporting information online at www.pnas.org/lookup/suppl/doi:10.1073/pnas.110901108/-/DCSupplemental.
*Note that precise position estimation from a point response does not require full reconstruction of the signal. Further, an optimum sampling rate can be calculated for a given system and noise level (11).
†Note that an intrinsic, random error greater than 0.6 nm is associated with the estimation of σest due to the finite distribution sample size of N = 100 used in the simulation. This random error is responsible for the fluctuations of σest about the CRLB.
Freely available online through the PNAS open access option.