Biomedical Engineering Reference
In-Depth Information
CHAPTER 18
Fluorescence Phase Microscopy (FPM)
and Nanoscopy
Alberto Bilenca
1
, Brett Bouma
2
,
3
, Guillermo Tearney
2
,
4
, Iwan M¨rki
5
,
Noelia Bocchio
5
, Stefan Geissbuehler
5
, Theo Lasser
5
1
Department of Biomedical Engineering, Ben Gurion University of the Negev, Be'er-Sheva, Israel
2
Harvard Medical School and Wellman Center for Photomedicine, Massachusetts General Hospital,
Boston, MA
3
The Harvard-MIT Division of Health Sciences and Technology, Cambridge, MA
4
Department of Pathology, Massachusetts General Hospital, Boston, MA
Laboratoire d'Optique Biom´dicale,
´
cole Polytechnique F´d´rale de Lausanne,
Lausanne, Switzerland
5
Editor: Natan T. Shaked
18.1 Introduction
Fluorescence imaging at the nanoscale and mesoscale level is a rapidly evolving research
field that provides a unique set of technological tools for tackling quantitatively
measurement problems in the natural and the life sciences with high specificity and at
various spatial resolution scales ranging from 1
10
m (mesoscopic resolution) to smaller
than
B
100 nm (nanoscopic resolution) in all three dimensions (3D). In general, state-of-the-
art 3D optical nanoscopy offers sub-100 nm spatial resolution in all 3D and penetration
depth of several micrometers
[1
11]
, whereas state-of-the-art 3D fluorescence microscopy
provides a 3D optical resolution of several micrometers along an extended penetration
depth of up to a few millimeters
[12
17]
. Typically, 3D fluorescence imaging techniques
aim at discriminating fluorescence photons emerging from one given point within the
specimen against most of other fluorescent light. To accomplish this task, various
fluorescence-discrimination mechanisms have been employed. In 3D nanoscopy, these
mechanisms include (i) one or two photon activatable fluorescence that enables lateral
centroid-based localization of individual fluorophores with nanometer precision
[1
5,7
10]
. Nanometer-scale localization of the fluorophores in the axial (depth)
dimension can be achieved by interferometry
[2,4]
or by detecting an aberrated point-spread
μ
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