Expand this Topic clickable element to expand a topic
Skip to content
Optica Publishing Group

All-solid-state lock-in imaging for wide-field fluorescence lifetime sensing

Open Access Open Access

Abstract

Fluorescence Lifetime Imaging Microscopy (FLIM) is a powerful technique that is increasingly being used in the life sciences during the past decades. However, a broader application of FLIM requires more cost-effective and user-friendly solutions. We demonstrate the use of a simple CCD/CMOS lock-in imager for fluorescence lifetime detection. The SwissRanger SR-2 time-of-flight detector, originally developed for 3D vision, embeds all the functionalities required for FLIM in a compact system. The further development of this technology and its combination with light-emitting- and laser diodes could drive a wider spreading of the use of FLIM including high-throughput applications.

©2005 Optical Society of America

Full Article  |  PDF Article
More Like This
High-speed wide-field time-gated endoscopic fluorescence-lifetime imaging

J. Requejo-Isidro, J. McGinty, I. Munro, D. S. Elson, N. P. Galletly, M. J. Lever, M. A. A. Neil, G. W. H. Stamp, P. M. W. French, P. A. Kellett, J. D. Hares, and A. K. L. Dymoke-Bradshaw
Opt. Lett. 29(19) 2249-2251 (2004)

3D-resolved fluorescence and phosphorescence lifetime imaging using temporal focusing wide-field two-photon excitation

Heejin Choi, Dimitrios S. Tzeranis, Jae Won Cha, Philippe Clémenceau, Sander J. G. de Jong, Lambertus K. van Geest, Joong Ho Moon, Ioannis V. Yannas, and Peter T. C. So
Opt. Express 20(24) 26219-26235 (2012)

Fluorescence lifetime imaging with a low-repetition-rate passively mode-locked diode-pumped Nd:YVO4 oscillator

S. Lévêque-Fort, D. N. Papadopoulos, S. Forget, F. Balembois, and P. Georges
Opt. Lett. 30(2) 168-170 (2005)

Cited By

Optica participates in Crossref's Cited-By Linking service. Citing articles from Optica Publishing Group journals and other participating publishers are listed here.

Alert me when this article is cited.


Figures (3)

Fig. 1.
Fig. 1. The lock-in imager sensor. Panel A shows microphotography of the sensor. Each single pixel, arranged in a 124×160 array has a dimension of about 40μm × 55μm. Each pixel has two gates that are controlled with voltages in opposite phase (Panel B). Thus, the photoelectrons generated in the photosensitive area, will accumulate in the two storage areas according to the relative phase of the photon flux and the gate potentials.
Fig. 2.
Fig. 2. Response of the lock-in imager. Panel A and B show the average intensity at each detected phase. The grey curve represents the average intensity (I0) and the circles are the experimental points connected by a spline curve (dashed). Gray circles correspond to images acquired by the injection of the additional delay by the external delay unit. The left side panels (A, C and E) represent measurements of a reflective foil, while B, D and F refer to a fluorescent slide acquisition. C and D depict the demodulation of the signal measured over the entire illuminated field of view; E and F show the correspondent phases. The latter are inhomogeneous over the field of view (arrows). Considering the lifetime of the samples, i.e. 0 ns and 4.8 ns for the reflective foil and fluorescent slide, respectively, the initial phase of the detection is shown to be constant, while the demodulations suffer from a color-effect of the lock-in imager.
Fig. 3.
Fig. 3. Fluorescence lifetime sensing. The lock-in imager distinguishes compounds with different fluorescent lifetimes. Panel A shows the phase-lifetime maps and distributions of: EGFP in solution (gray line), a fluorescent slide (dashed curve) and DNA-bound GelStar (black solid line) in solution. The lifetimes were 2.6±0.4 ns, 4.8±0.4 ns and 6.6±0.7 ns, respectively. Both the phase- (panel B, gray curve) and demodulation- (black line) lifetimes can be measured at a modulation frequency of 20MHz. A Turbo-Sapphire GFP bead showed values of 2.67±0.09 ns and 3.7±0.2 ns, respectively. Panel B inset (R6G) shows the phase (4.3±0.2) and modulation (4.3±0.4) lifetime of the mono-exponential decaying fluorophore standard Rhodamine 6G.

Equations (4)

Equations on this page are rendered with MathJax. Learn more.

{ ϕ = arctan ( S 3 π 2 S π 2 S 0 S π ) ϕ m = ( S 3 π 2 S π 2 ) 2 + ( S 0 S π ) 2 m ( S 0 + S π 2 + S π + S 3 π 2 )
{ τ ϕ = ω 1 tan ϕ τ m = ω 1 1 m 2 1
{ F DC = k = 0 7 S 4 F SIN = k = 0 7 S 4 sin ( 4 ) F COS = k = 0 7 S 4 cos ( 4 )
{ ϕ = arctan ( F SIN F COS ) ϕ m = F SIN 2 + F COS 2 m F DC
Select as filters


Select Topics Cancel
© Copyright 2024 | Optica Publishing Group. All rights reserved, including rights for text and data mining and training of artificial technologies or similar technologies.