11.01.2013 Views

5th EuropEan MolEcular IMagIng MEEtIng - ESMI

5th EuropEan MolEcular IMagIng MEEtIng - ESMI

5th EuropEan MolEcular IMagIng MEEtIng - ESMI

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<strong>5th</strong> <strong>EuropEan</strong> <strong>MolEcular</strong> <strong>IMagIng</strong> <strong>MEEtIng</strong> – EMIM2010<br />

A system for 4D (3D+Kinetics) molecular imaging in bioluminescence and fluorescence<br />

Maitrejean S. (1) , Kyrgyzov I. (1) , Bonzom S. (1) , Levrey O. (1) , Le Masne Q. (1) , Hernandez L. (1) , Raphael B. (2) .<br />

(1) Biospace Lab,<br />

(2) CEA/DSV/ I2BM / SHFJ / LIME.<br />

smaitrejean@biospacelab.com<br />

Introduction: Several technologies and systems are<br />

now capable of delivering tri-dimensional data in Bioluminescence<br />

and Fluorescence imaging. However, all<br />

are based on sequential acquisitions, and therefore any<br />

of them allow the production of real kinetic data in<br />

3D. In this work we demonstrate a new device which<br />

is able to acquire Bioluminescence and Fluorescence<br />

data from several views simultaneously, allowing the<br />

reconstruction of tri-dimensional images while keeping<br />

all kinetic properties of the acquisition.<br />

Methods: Multiple views of Bioluminescence and Fluorescence<br />

data are acquired simultaneously using a photon<br />

counting device (Photon ImagerTM) in which a<br />

specific add-on with four mirrors is installed. This device<br />

(named 4Views) allows the concurrent acquisition<br />

of the ventral, dorsal, right, and left views of the animal<br />

in a single image. The size and intensity of the four subimages<br />

(i.e. the four views) are corrected by taking the<br />

true optical path into account. The corrected photon<br />

counting data are recorded in a list mode file with time<br />

information (43 frame/s) as can be seen in Fig1.<br />

In a second step a micro video projector is used to<br />

project a moving spot on the animal. For each position<br />

of the spot, the<br />

height of the animal<br />

is calculated<br />

by triangulation<br />

and a map of the<br />

surface of the animal<br />

is produced.<br />

As the chosen<br />

reconstruction<br />

Fig1: simultaneous acquisition of four views<br />

in bioluminescence imaging.<br />

method is based<br />

on the finite elements<br />

method,<br />

the volume of the animal is represented by a tetrahedral<br />

mesh (about 30 000 tetrahedrons) using the Delaunay<br />

algorithm, while the surface is approximated<br />

by triangles, using a marching cube method. Then, the<br />

forward problem is solved for given light sources that<br />

are placed at the nodes of tetrahedrons and the light<br />

intensities on the surface of the triangles are computed.<br />

The forward problem is based in this first version on a<br />

diffusion model with average constant absorption and<br />

diffusion parameters. In a next version, a registration of<br />

the surface of the animal with an anatomical atlas will<br />

allow to use optical parameters associated with each<br />

organ. In the following step measured data is extracted<br />

from the list mode file and mapped on the triangulated<br />

surface. Since the detected events are stored separately,<br />

any time interval from 22 ms (one frame) up to the<br />

total scan duration can be used to create the data. In<br />

the last step of the process, the inner light sources are<br />

estimated as the result of the inverse problem using a<br />

least square criterion with a Tikhonoff regularization<br />

term. This regularisation term is chosen as an entropic<br />

term in order to favour connected solution. The two<br />

last steps can be performed using any time interval of<br />

the list mode file and therefore 3D kinetic data can be<br />

computed for times scales larger than 22 ms.<br />

Results: The validity of the method has been first tested<br />

using light beads (Microtek) inside a half cylinder of a<br />

scattering material (delrin). It has been demonstrated<br />

that two light beads as close as three millimetres could<br />

be separated, at a depth of one centimetre. A second<br />

set of tests has been realised on an animal (nude mice)<br />

by placing the light beads in the rectum of the animal.<br />

On the second image (Fig 2) , two beads 9 mm far from<br />

each other were placed in the rectum. It was possible to<br />

reconstruct the two positions of the light sources. The<br />

distance between the two reconstructed sources is 9.77<br />

mm in good agreement.<br />

Fig2: Reconstruction of two light sources based<br />

on the four views data of fig1.<br />

Conclusions: 3D optical reconstruction is known to<br />

be approximate, but can give useful and satisfactory<br />

results in a large number of applications. We have<br />

demonstrated that this four view approach is able to<br />

provide 3D kinetic molecular imaging data with a<br />

spatial accuracy similar to other methods.<br />

Acknowledgement: This work was supported in part<br />

by the DIMI and ENCITE networks.<br />

<strong>EuropEan</strong> SocIEty for <strong>MolEcular</strong> <strong>IMagIng</strong> – <strong>ESMI</strong><br />

day1<br />

Parallel Session 3: TECHNOLOGY

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!