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1.
Opt Express ; 15(13): 8146-56, 2007 Jun 25.
Article in English | MEDLINE | ID: mdl-19547141

ABSTRACT

We have observed the motion of metallic particles above various optical waveguides injected by 1064nm radiation. Small gold particles (250nm diameter) are attracted towards the waveguide where the intensity of the optical field is maximum, and are propelled at high velocity (up to 350mum/s) along the waveguide due to radiation pressure. The behaviour of larger metallic particles (diameter >600nm) depends on the polarization of the evanescent field: for TM polarization they are attracted above the waveguide and propelled by the radiation pressure; for TE polarization they are expelled on the side of the waveguide and propelled at much smaller velocity. This is consistent with calculations of radiative forces on metallic particles by Nieto-Vesperinas et al. 3D-finite element method calculations carried out for our experimental situations confirm the observed dependence with the polarization of the field and the size of the particles. These observations open the way to the development of new microsystems for particles manipulations and sorting applications.

2.
Opt Lett ; 31(8): 1142-4, 2006 Apr 15.
Article in English | MEDLINE | ID: mdl-16625930

ABSTRACT

Fluorescence fluctuation spectroscopy is applied to study molecules passing through a small observation volume, usually subjected to diffusive or convective motion in a liquid phase. We suggest that such a technique could be used to measure the areal absolute concentration of fluorophores deposited on a substrate or embedded in a thin film, with a resolution of a few micrometers. The principle is to translate the solid substrate in front of a confocal fluorescence microscope objective and to record the subsequent fluctuations of the fluorescence intensity. The validity of this concept is investigated on model substrates (fluorescent microspheres) and DNA biochips.

3.
Biophys J ; 90(7): 2548-62, 2006 Apr 01.
Article in English | MEDLINE | ID: mdl-16428281

ABSTRACT

We present a comprehensive and analytical treatment of continuous photobleaching in a compartment, under single photon excitation. In the very short time regime (t<0.1 ms), the diffusion does not play any role. After a transition (or short time regime), one enters in the long time regime (t>0.1-5 s), for which the diffusion and the photobleaching balance each other. In this long time regime, the diffusion is either fast (i.e., the photobleaching probability of a molecule diffusing through the laser beam is low) so that the photobleaching rate is independent of the diffusion constant and dependent only of the laser power, or the diffusion is slow (i.e., the photobleaching probability is high) and the photobleaching rate is mainly dependent on the diffusion constant. We illustrate our theory by using giant unilamellar vesicles ranging from approximately 10 to 100 microm in diameter, loaded with molecules of various diffusion constants (from 20 to 300 microm2/s) and various photobleaching cross sections, illuminated under laser powers between 3 and 100 microW. We also demonstrated that information about compartmentation can be obtained by this method in living cells expressing enhanced green fluorescent proteins or that were loaded with small FITC-dextrans. Our quantitative approach shows that molecules freely diffusing in a cellular compartment do experience a continuous photobleaching. We provide a generic theoretical framework that should be taken into account when studying, under confocal microscopy, molecular interactions, permeability, etc.


Subject(s)
Biophysics/methods , Microscopy, Fluorescence/methods , Computer Simulation , Dextrans/pharmacology , Diffusion , Fluorescein-5-isothiocyanate/analogs & derivatives , Fluorescein-5-isothiocyanate/pharmacology , Fluorescence Recovery After Photobleaching , Green Fluorescent Proteins/chemistry , HeLa Cells , Humans , Image Processing, Computer-Assisted , Light , Microscopy, Confocal , Models, Statistical , Models, Theoretical , Permeability , Photobleaching , Photons , Programming Languages , Reproducibility of Results , Software , Time Factors
4.
Opt Express ; 13(18): 6956-63, 2005 Sep 05.
Article in English | MEDLINE | ID: mdl-19498716

ABSTRACT

We demonstrate the optical manipulation of cells and dielectric particles on the surface of silicon nitride waveguides. Glass particles with 2microm diameter are propelled at velocities of 15microm/s with a guided power of 20mW. This is approximately 20 times more efficient than previously reported, and permits to use this device on low refractive index objects such as cells. Red blood cells and yeast cells can be trapped on the waveguide and pushed along it by the action of optical forces. This kind of system can easily be combined with various integrated optical structures and opens the way to the development of new microsystems for cell sorting applications.

5.
J Fluoresc ; 14(3): 255-67, 2004 May.
Article in English | MEDLINE | ID: mdl-15615207

ABSTRACT

In living cells the transport and diffusion of molecules is constrained by compartments of various sizes. This paper is an attempt to show that the size of these compartments can in principle be estimated experimentally from Fluorescence Correlation Spectroscopy (FCS) combined with the measurement of the photobleaching rate. In this work, confocal fluorescence microscopy experiments have been carried out on giant unilamellar vesicles, a system that mimics cellular compartmentalisation. We have developed numerical and analytical models to describe the fluorescence decay due to photobleaching in this geometry, which has enabled us to point out two regimes depending on the value of the parameter P(B) = sigma(B)P/D (where sigma(B) is the photobleaching cross section of the dye, D its diffusion constant, and P the laser power (in photon/s)). In particular, when P(B) << 1 (i.e. in the fast diffusion regime), the photobleaching rate is independent of the diffusion constant and scales like sigma(B)P/R2, in agreement with the experimental results. On the other hand, the standard diffusion models used to analyse the FCS data do not take into account the effects of the fluorescence decay on the autocorrelation curve. We show here how to correct the raw data for these drawbacks.


Subject(s)
Cell Compartmentation , Photobleaching , Spectrometry, Fluorescence/methods , Artifacts , Diffusion , Fluorescein-5-isothiocyanate/chemistry , Fluorescence , Fluorescent Dyes/chemistry , HeLa Cells , Humans
6.
C R Acad Sci III ; 323(6): 529-36, 2000 Jun.
Article in English | MEDLINE | ID: mdl-10923208

ABSTRACT

Hyperpolarized 129Xe was dissolved in a lipid emulsion and administered to anaesthetized rats by manual injections into the carotid (approximately 1-1.5 mL in a maximum time of 30 s). During injection, 129Xe NMR brain spectra at 2.35 T were recorded over 51 s, with a repetition time of 253 ms. Two peaks assigned to dissolved 129Xe were observed (the larger at 194 +/- 1 ppm assigned to intravascular xenon and the smaller at 199 +/- 1 ppm to xenon dissolved in the brain tissue). Their kinetics revealed a rapid intensity increase, followed by a plateau (approximately 15 s duration) and then a decrease over 5 s. This behaviour was attributed to combined influences of the T1 relaxation of the tracer, of radiofrequency sampling, and of the tracer perfusion rate in rat brain. Similar kinetics were observed in experiments carried out on a simple micro-vessel phantom. An identical experimental set-up was used to acquire a series of 2D projection 129Xe images on the phantom and the rat brain.


Subject(s)
Brain/anatomy & histology , Magnetic Resonance Spectroscopy , Animals , Emulsions , Fat Emulsions, Intravenous , Injections, Intra-Arterial , Male , Rats , Rats, Sprague-Dawley , Xenon Isotopes
7.
Magn Reson Med ; 41(6): 1084-7, 1999 Jun.
Article in English | MEDLINE | ID: mdl-10371438

ABSTRACT

The first 3He nuclear magnetic resonance (NMR) experiments using low-temperature prepolarization are presented. 3He cells were polarized at 4.2 K and 4.7 T, transported to another magnet, heated to room temperature, and used for NMR experiments at 2.35 T. Cells with and without a rubidium coating were tested. In both cases, the NMR signal was greater than 100 times the thermal equilibrium signal. No evidence of a rubidium coating effect on the longitudinal relaxation time T1 of 3He (500 mbar) at 4.2 K could be demonstrated. NMR gradient-echo images of the cells were acquired.


Subject(s)
Helium , Magnetic Resonance Imaging , Humans , Isotopes , Magnetic Resonance Spectroscopy , Rubidium
10.
Phys Rev Lett ; 60(4): 282-285, 1988 Jan 25.
Article in English | MEDLINE | ID: mdl-10038502
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