Advanced Three-Dimensional Optical Mapping

2021 ◽  
pp. 199-208
Author(s):  
Olivier Bernus ◽  
Richard D. Walton
ACS Nano ◽  
2016 ◽  
Vol 10 (5) ◽  
pp. 5468-5478 ◽  
Author(s):  
Shrey Sindhwani ◽  
Abdullah Muhammad Syed ◽  
Stefan Wilhelm ◽  
Dylan R. Glancy ◽  
Yih Yang Chen ◽  
...  

2017 ◽  
Vol 7 ◽  
pp. A24 ◽  
Author(s):  
Eric Hivon ◽  
Jean Mouette ◽  
Thierry Legault

We describe the steps necessary to create three-dimensional (3D) movies of Northern Lights or Aurorae Borealis out of real-time images taken with two distant high-resolution fish-eye cameras. Astrometric reconstruction of the visible stars is used to model the optical mapping of each camera and correct for it in order to properly align the two sets of images. Examples of the resulting movies can be seen at http://www.iap.fr/aurora3d.


2005 ◽  
Vol 289 (4) ◽  
pp. H1428-H1435 ◽  
Author(s):  
Steven Poelzing ◽  
Bradley J. Roth ◽  
David S. Rosenbaum

Previously, we showed that intercellular uncoupling through gap junctions is an important mechanism for maintaining transmural heterogeneities of repolarization that are responsible for ventricular arrhythmias in disease states such as heart failure. However, rotational anisotropy between transmural muscle layers also may influence coupling. To determine the effect of rotational anisotropy on transmural coupling, we developed a numerical three-dimensional model of passive cardiac tissue in which rotational anisotropy was varied in a controlled fashion. Simulations of optical mapping demonstrated that spatial averaging produced a voltage decay in space best fit by a single decaying exponential compared with the theoretically predicted decay. As fiber orientation varied by 90° with respect to the transmural surface, the effective transmural space constant (λTM) changed by only 0.31% in simulations. In contrast, reducing intercellular conductivity by 24% decreased λTM by 7.7%. In the canine wedge preparation ( n = 5), λ measured by optical mapping of the epicardial and subepicardial surface was similar transverse (λTV = 0.73 ± 0.10 mm) and transmural (λTM = 0.70 ± 0.08 mm) to subepicardial fibers. We confirmed previous findings that λTM in subepicardial layers was significantly reduced by 14 ± 2% compared with deeper layers of myocardium, providing evidence for transmural uncoupling in the epicardial-midmyocardial interface. These data establish the theoretical and experimental basis for measuring intercellular coupling between muscle layers spanning the ventricular wall with optical mapping techniques. Furthermore, this study demonstrates that transmural uncoupling at the epicardial-midmyocardial interface may be attributable to heterogeneous expression of cardiac gap junctions and not rotational anisotropy.


2004 ◽  
Vol 16 (Supplement) ◽  
pp. 221-222
Author(s):  
Shiho Nashimoto ◽  
Yuhei Takata ◽  
Takahiro Yamaguchi ◽  
Tatsuhiko Arafune ◽  
Etsuko Kobayashi ◽  
...  

2016 ◽  
Vol 371 (1705) ◽  
pp. 20150360 ◽  
Author(s):  
Ying Ma ◽  
Mohammed A. Shaik ◽  
Sharon H. Kim ◽  
Mariel G. Kozberg ◽  
David N. Thibodeaux ◽  
...  

Although modern techniques such as two-photon microscopy can now provide cellular-level three-dimensional imaging of the intact living brain, the speed and fields of view of these techniques remain limited. Conversely, two-dimensional wide-field optical mapping (WFOM), a simpler technique that uses a camera to observe large areas of the exposed cortex under visible light, can detect changes in both neural activity and haemodynamics at very high speeds. Although WFOM may not provide single-neuron or capillary-level resolution, it is an attractive and accessible approach to imaging large areas of the brain in awake, behaving mammals at speeds fast enough to observe widespread neural firing events, as well as their dynamic coupling to haemodynamics. Although such wide-field optical imaging techniques have a long history, the advent of genetically encoded fluorophores that can report neural activity with high sensitivity, as well as modern technologies such as light emitting diodes and sensitive and high-speed digital cameras have driven renewed interest in WFOM. To facilitate the wider adoption and standardization of WFOM approaches for neuroscience and neurovascular coupling research, we provide here an overview of the basic principles of WFOM, considerations for implementation of wide-field fluorescence imaging of neural activity, spectroscopic analysis and interpretation of results. This article is part of the themed issue ‘Interpreting BOLD: a dialogue between cognitive and cellular neuroscience’.


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