Cellular basis for QT dispersion. Antzelevitch, C., Shimizu, W., Yan, G., & Sicouri, S. j-JE, 30(Suppl):168--75, 1998. bibtex @Article{RSM:Ant98,
author = "C. Antzelevitch and W. Shimizu and G.X. Yan and S.
Sicouri",
title = "Cellular basis for {QT} dispersion.",
journal = j-JE,
year = "1998",
volume = "30",
number = "Suppl",
pages = "168--75",
robnote = "The start of the T wave is caused by a more rapid
decline of the plateau, or phase 2 of the epicardial
action potential, creating a voltage gradient across
the wall. The gradient increases as the epicardial
action potential continues to repolarize, reaching a
maximum with full repolarization of epicardium; this
juncture marks the peak of the T wave. The next region
to repolarize is endocardium, giving rise to the
initial descending limb of the upright T wave. The last
region to repolarize is the M region, contributing to
the final segment of the T wave. LQTS",
}
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{"_id":"5v2KrxwiWPQfdgNkB","bibbaseid":"antzelevitch-shimizu-yan-sicouri-cellularbasisforqtdispersion-1998","downloads":0,"creationDate":"2016-07-01T21:38:29.368Z","title":"Cellular basis for QT dispersion.","author_short":["Antzelevitch, C.","Shimizu, W.","Yan, G.","Sicouri, S."],"year":1998,"bibtype":"article","biburl":"http://www.sci.utah.edu/~macleod/Bibtex/biglit.bib","bibdata":{"bibtype":"article","type":"article","author":[{"firstnames":["C."],"propositions":[],"lastnames":["Antzelevitch"],"suffixes":[]},{"firstnames":["W."],"propositions":[],"lastnames":["Shimizu"],"suffixes":[]},{"firstnames":["G.X."],"propositions":[],"lastnames":["Yan"],"suffixes":[]},{"firstnames":["S."],"propositions":[],"lastnames":["Sicouri"],"suffixes":[]}],"title":"Cellular basis for QT dispersion.","journal":"j-JE","year":"1998","volume":"30","number":"Suppl","pages":"168--75","robnote":"The start of the T wave is caused by a more rapid decline of the plateau, or phase 2 of the epicardial action potential, creating a voltage gradient across the wall. The gradient increases as the epicardial action potential continues to repolarize, reaching a maximum with full repolarization of epicardium; this juncture marks the peak of the T wave. The next region to repolarize is endocardium, giving rise to the initial descending limb of the upright T wave. The last region to repolarize is the M region, contributing to the final segment of the T wave. LQTS","bibtex":"@Article{RSM:Ant98,\n author = \"C. Antzelevitch and W. Shimizu and G.X. Yan and S.\n Sicouri\",\n title = \"Cellular basis for {QT} dispersion.\",\n journal = j-JE,\n year = \"1998\",\n volume = \"30\",\n number = \"Suppl\",\n pages = \"168--75\",\n robnote = \"The start of the T wave is caused by a more rapid\n decline of the plateau, or phase 2 of the epicardial\n action potential, creating a voltage gradient across\n the wall. The gradient increases as the epicardial\n action potential continues to repolarize, reaching a\n maximum with full repolarization of epicardium; this\n juncture marks the peak of the T wave. The next region\n to repolarize is endocardium, giving rise to the\n initial descending limb of the upright T wave. The last\n region to repolarize is the M region, contributing to\n the final segment of the T wave. LQTS\",\n}\n\n","author_short":["Antzelevitch, C.","Shimizu, W.","Yan, G.","Sicouri, S."],"key":"RSM:Ant98","id":"RSM:Ant98","bibbaseid":"antzelevitch-shimizu-yan-sicouri-cellularbasisforqtdispersion-1998","role":"author","urls":{},"downloads":0,"html":""},"search_terms":["cellular","basis","dispersion","antzelevitch","shimizu","yan","sicouri"],"keywords":[],"authorIDs":[],"dataSources":["5HG3Kp8zRwDd7FotB"]}