Abstract
Atrial fibrillation is the most common arrhythmia. However, the mechanisms of AF are not completely understood. It is known that fractionated signals are measured in AF but the etiology of fractionated signals is still not clear. The central question is to evaluate the effects of segmented fibrotic areas in histological tissue sections on the extracellular potential in a simulation study. We calculated the transmembrane voltages and extracellular potentials from the excitation wave front around a 3D fibrotic area from mouse hearts that were reconstructed from histological tissue sections. Extracellular potentials resulted in fragmented signals and differed strongly by stimulations from different directions. The transmural angle of the excitation waves had a significantly influence on the signal morphologies. We suggest for future clinical systems to implement the possibility for substrate mapping by stimulations from different directions in sinus rhythm.
1 Introduction
AF is a common arrhythmia and frequently fractionated signals are measured [1], [2]. The mechanisms of AF and the correlation with typically unipolar signals and in particular fractionated signals are not well understood [3], [4], [5]. There are simulation studies of correlations of intracardiac signals in AF [6], [7] and correlations with fibrosis, but the fibrotic patterns were in the whole myocardium between endocardium and epicardium and the implementation was based on random numbers [8] or implemented in a 2D area [9]. For the first time we calculated extracellular potentials from the excitation around a 3D fibrotic area reconstructed from real fibrotic areas obtained in histological heart tissue sections. In this proof of concept the correlation between fibrotic area and fractionated signals is presented. Also, the influences of the transmural angle of the wave front and stimulations from different directions on the extracellular potential are presented.
2 Methods
2.1 Histological tissue sections
In order to investigate cardiac fibrosis in vivo, we used a mouse model of chronic CVB3 myocarditis. Hearts were obtained 4 weeks after CVB3 infection of ABY/SnJ mice, at a time point when fibrosis is obvious. The hearts were fixed in 4% paraformaldehyde and embedded in paraffin. 5 μm thick tissue sections covering the right and left ventricle were cut with a distance of 10 μm and stained with Sirius red. The red staining illustrates myocardial fibrosis. Images from the same area of 60 consecutive tissue sections were taken with a Zeiss Axioskop 40 microscope and used for reconstruction by manual registering. Figure 1 shows exemplarily histological tissue sections of the right and left ventricle of 10x and 100x magnification.

High resolution image of ventricular histological tissue sections at a microscopic magnification of × 10 (A). (B) is the inset of (A) at a magnification of × 100. The Sirius red staining illustrates myocardial fibrosis.
2.2 3D reconstructions from histological tissue sections
The dimensions of the histological images were 750 μm by 1000 μm. In order to obtain a 3D reconstruction of the fibrotic tissue by using identified landmarks, we manually segmented fibrosis of each image obtained from the same area of consecutive heart tissue sections. We created binary images in which the pixels corresponding to fibrotic tissue are marked with 1, and the other tissue types with 0. Then we rescaled the images in order to get cubic voxels with edge length of 12.5 μm. Then we applied of a scaling factor of 20 to get from mouse-size atrium to human-size atrium.
In a further step we created a 3D model of the fibrotic tissue by stacking the single segmented images on top of each other, see Figure 2. The 3D reconstruction of the fibrotic area consisted of voxels with edge length of 0.25 mm.

3D Reconstruction of the fibrotic tissue from segmented histological tissue sections in (A) front view, (B) behind view.
2.3 Calculation of cardiac potentials and modelling of fibrosis
Transmembrane voltages were calculated using the monodomain equation with the parallel solver aCELLerate [10].
VM, represents the transmembrane voltage, σM the bulk conductivity and β the cell- surface to volume ratio [8]. By forward calculation [8] extracellular potentials were calculated based on transmembrane source current density [9] with a sampling rate of 1 kHz. To describe ventricular behaviour the cell model of Ten Tusscher et al. was used. The simulation geometry consisted on a regular grid of cubic elements. The 3D patch had the size of 200 × 200 × 200 voxels with the voxel length 0.25 mm. The manually segmented fibrotic area was implemented in healthy tissue. Segmented collagenous structures from the histological tissue sections were modelled as fibrotic elements without consideration of tissue conductivity and sodium handling [8].
3 Results
3.1 Transmembrane voltages of plane wave stimulation
The tissue was stimulated in the upper part of the tissue. In Figure 3 the meandering of the excitation wave fronts around the fibrotic area is depicted at different times. The transmural angle and the conduction velocity of the splitted excitation fronts varied at different times. Because of the reaction diffusion behaviour the excitation became a nearly plane wave again in the lower part.

Transmembrane voltages of an excitation around fibrotic area at the times 10 ms, 28 ms, 38 ms and 42 ms.
3.2 Transmembrane voltages and extracellular potentials of stimulation with transmural angle
Transmembrane and extracellular potentials of the stimulation in the left upper corner (10 × 10 × 10 voxels) resulted in fractionated extracellular signals, see Figure 4.

Left: Excitation wave front of the transmembrane voltage at time 18 ms and corresponding signal at the measurement point. Right: Excitation wave front of the extracellular potential at time 18 ms and corresponding signal.
3.3 Signal analysis
Figure 4 shows the resulting transmembrane potential at the selected measurement point in the first tissue layer close to the blood layers. Furthermore the corresponding extracellular potential at the first blood layer close to the tissue is presented. The measured unipolar signal was strongly deformed from ideal signal form of healthy tissue. Unipolar signals measured at the endocardium were on the one hand dependent on the fibrosis and on the other hand dependent on the direction of the wave front. Especially the transmural angle of the wave front had a significant influence on the signal form.
4 Discussion and summary
This work presents the first simulation study of 3D fibrosis reconstructed from histologically reconstructed murine heart tissue. We present a proof of principle that fractionated signals can be measured from real fibrotic areas reconstructed from histological tissue sections. The patterns of fibrosis are similar to those observed in humans. On the one hand fractionated signal morphologies from unipolar recordings could be correlated with fibrotic areas, on the other hand the signal morphologies were strongly dependent on the parameters of the excitation wave direction and transmural angle. Future clinical systems might implement fibrosis mapping by stimulations from various directions in sinus rhythm. We used several simplifications in this proof of concept simulation study in the 3D reconstruction of fibrosis. Furthermore we translated animal heart fibrosis to a human model of fibrosis.
Author’s Statement
Research funding: The author state no funding involved. Conflict of interest: Authors state no conflict of interest. Material and methods: Informed consent: Informed consent is not applicable. Ethical approval: The research related to animal use complies with all the relevant national regulations and institutional policies for the care and use of animals.
References
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©2016 Markus Rottmann et al., licensee De Gruyter.
This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.
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