Literature DB >> 26849052

Correction: A Computational Study of the Factors Influencing the PVC-Triggering Ability of a Cluster of Early Afterdepolarization-Capable Myocytes.

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Abstract

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Year:  2016        PMID: 26849052      PMCID: PMC4743987          DOI: 10.1371/journal.pone.0148663

Source DB:  PubMed          Journal:  PLoS One        ISSN: 1932-6203            Impact factor:   3.240


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Figs 5 and 6 are incorrect. The figure captions of Figs 5 and 6 are swapped. The publisher apologizes for the error. The authors have provided the corrected versions here.
Fig 5

The dependence of the triggering of PVCs on the coupling strength of the EAD clump.

The clumps in the top, middle, and the bottom panels have radii R = 2 cm. The clump with D = Do (top panel) does not trigger PVCs, whereas the clumps with D = 0.7xDo, (middle panel) and D = 0.2xDo (bottom panel) trigger PVCs. The clump with D = 0.2xDo supports small-wavelength spirals inside the clump as shown at times 6600 ms and 6620 ms.

Fig 6

Dependence of the number N of PVC triggerings on the radius R, normalized coupling strength D/Do, and the percentage of fibrosis Pf.

The blue and red curves are for PCL = 1000 ms and 1400 ms, respectively. (A) Plots of N versus R, which show that the number of PVCs increases roughly with R. (B) Plots of N versus D/Do. The number of PVC triggerings increases initially with the reduction of D/Do, but saturates roughly when D/Do ≲ 0.4 and ≲0.65 for PCL = 1000 and 1400 ms, respectively. (C) Plots of N versus the percentage of fibrosis Pf show a maximum at Pf ≃ 40%. A comparison of the plots in (A), (B), and (C) for the two different values of PCL, namely, PCL = 1000 ms and PCL = 1400 ms, shows that these plots depend sensitively on PCL.

The dependence of the triggering of PVCs on the coupling strength of the EAD clump.

The clumps in the top, middle, and the bottom panels have radii R = 2 cm. The clump with D = Do (top panel) does not trigger PVCs, whereas the clumps with D = 0.7xDo, (middle panel) and D = 0.2xDo (bottom panel) trigger PVCs. The clump with D = 0.2xDo supports small-wavelength spirals inside the clump as shown at times 6600 ms and 6620 ms.

Dependence of the number N of PVC triggerings on the radius R, normalized coupling strength D/Do, and the percentage of fibrosis Pf.

The blue and red curves are for PCL = 1000 ms and 1400 ms, respectively. (A) Plots of N versus R, which show that the number of PVCs increases roughly with R. (B) Plots of N versus D/Do. The number of PVC triggerings increases initially with the reduction of D/Do, but saturates roughly when D/Do ≲ 0.4 and ≲0.65 for PCL = 1000 and 1400 ms, respectively. (C) Plots of N versus the percentage of fibrosis Pf show a maximum at Pf ≃ 40%. A comparison of the plots in (A), (B), and (C) for the two different values of PCL, namely, PCL = 1000 ms and PCL = 1400 ms, shows that these plots depend sensitively on PCL.
  1 in total

1.  A Computational Study of the Factors Influencing the PVC-Triggering Ability of a Cluster of Early Afterdepolarization-Capable Myocytes.

Authors:  Soling Zimik; Alok Ranjan Nayak; Rahul Pandit
Journal:  PLoS One       Date:  2015-12-16       Impact factor: 3.240

  1 in total

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