| Literature DB >> 32782637 |
Jing Quah1,2, Dhani Dharmaprani1, Anandaroop Lahiri1,2, Madeline Schopp1, Lewis Mitchell3, Joseph B Selvanayagam1,2,4, Rebecca Perry1,2,4, Fahd Chahadi2, Matthew Tung5, Waheed Ahmad6, Nikola Stoyanov7, Majo X Joseph1,2, Cameron Singleton1,2, Andrew D McGavigan1,2, Anand N Ganesan1,2,4.
Abstract
BACKGROUND: Unstable functional reentrant circuits known as rotors have been consistently observed in atrial fibrillation and are mechanistically believed critical to the maintenance of the arrhythmia. Recently, using a Poisson renewal theory-based quantitative framework, we have demonstrated that rotor formation (λf) and destruction rates (λd) can be measured using in vivo electrophysiologic data. However, the association of λf and λd with clinical, electrical, and structural markers of atrial fibrillation phenotype is unknown.Entities:
Keywords: atrial fibrillation; multimodal imaging; poisson distribution
Year: 2020 PMID: 32782637 PMCID: PMC7411212 DOI: 10.1002/joa3.12363
Source DB: PubMed Journal: J Arrhythm ISSN: 1880-4276
Figure 1Adapted from Dharmaprani et al8. Properties of a Poisson renewal process and an example from a human persistent atrial fibrillation (AF) case. A, Poisson renewal process is one in which the times between events are independent but events occur at a long‐term constant rate (i and ii). In the discrete case, the probability distribution function (PDF) takes the form of a geometric distribution, which converges to an exponential distribution when large numbers of phase singularity (PS) are considered. If data possess these properties, it implies that the generating process is a Poisson renewal process (iii). Examples of Poisson processes in other scientific disciplines include the timing of radioactive decay events. B, (i) Phase movie snapshots of human persistent atrial fibrillation. In the snapshots, the appearance and disappearance of several phase singularities is shown. The timing of phase singularity is tracked. It shows that phase singularity (marked with *) appear and disappear, although the time intervals between events are irregular. In (ii), we show a staircase diagram to plot the interevent (also known as interarrival) time between new‐phase singularity formation events, denoted by Xn. Although the times between new‐phase singularity events are irregular, the long‐term average rate of increase in phase singularity formation (shown by the slope) is constant (iii)
Figure 2Flow chart of patient recruitment into RENEWAL‐AF