| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
Articles |
From the Division of Cardiology, Department of Medicine, and Department of Pathology, Cedars-Sinai Medical Center, and UCLA School of Medicine, Los Angeles, Calif.
| Abstract |
|---|
|
|
|---|
30 ms (22±8 ms) or
80 ms (94±15 ms). The
differences among these four intervals were significant
(P<.001). We conclude that the effects of strong electrical
stimulation on the reentrant wavefronts in VF are dependent on the
recovery interval since the previous local activation. A protective
zone occurred between 20 and 60 ms, during which time a strong
electrical stimulus could terminate reentry and abort VF. This zone was
followed by a vulnerable period during which new activation wavefronts
could be induced. If a strong electrical stimulus was given shortly
after or sufficiently long after the previous local activation, the
same figure-eight reentrant pattern continued.
Key Words: vulnerability defibrillation sudden cardiac death electrophysiology protective zone
| Introduction |
|---|
|
|
|---|
| Materials and Methods |
|---|
|
|
|---|
After the data were analyzed for dog 1, we found that the
interelectrode distance of the electrodes with the silver ball at the
end was too large to record discrete activations during VF.
Therefore, the remaining five dogs were studied with an electrode array
that was made of the same material and had the same interelectrode and
interpolar spacing as the first electrode array used in dog 1. This
electrode array consisted of 317 electrodes forming 21 columns and 16
rows when dog 2 was studied. The same electrode array was then expanded
to 509 channels, with 21 columns and 25 rows, and this version was used
to study the last four dogs. The upper edge of the electrode array was
within 2 cm of the pulmonic valve. Therefore, the mapped region
included both the right ventricular outflow tract and the
right ventricular free wall. Fig 1
shows the
electrode location and the patterns of activation after the
S1.
|
Surgical Preparation
Adult mongrel dogs of either sex were studied. The dogs were
anesthetized by intravenous administration of 25 to
35 mg/kg of sodium pentobarbital,9 intubated with a cuffed
endotracheal tube, and ventilated via a Harvard respirator (Harvard
Apparatus). The depth of anesthesia was
monitored by eyelid and pedal reflexes. A venous line was inserted
through a femoral vein to infuse pentobarbital at a rate of 0.05
mg · kg-1 · min-1 throughout the
experiment. Additional doses of pentobarbital were given when
needed.
An arterial line was inserted into the femoral artery to continuously monitor blood pressure. Blood was periodically sampled to determine the pH, PO2, PCO2, base excess, and bicarbonate concentrations. Rectal temperature was monitored continuously and maintained at 35°C to 37°C by heating the table with warm circulating water. The chest was opened through a median sternotomy, and the heart was suspended in a pericardial cradle. A plaque electrode array was sutured to the right ventricular epicardium to record activations and to deliver electrical stimuli. To ensure that a figure-eight pattern of reentrant activation was observed after the S2 stimulus, the line connecting the S1 and the S2 was roughly parallel to the myocardial fiber orientation.7
Stimulation Protocol
An S1 stimulus at twice bipolar
diastolic pacing threshold was given at the right edge of
the electrode array (Fig 1
). After eight S1 stimuli, an
S2 stimulus of 10-mA strength and 10-ms duration was given
to scan the T wave. The S1-S2 interval started
at 90 ms. If VF was not induced, the S1-S2
interval was increased at 10-ms increments until 240 ms was reached. If
VF was not induced, the S2 strength was increased in 5-mA
steps until VF was induced. This last S2 strength was used
as the conventional VF threshold.
To ensure a high probability of VF induction, the S2 and S3 strengths used in the subsequent study protocol were 40 mA higher than the conventional VF threshold.8 The S1-S2 interval was fixed at the interval that first induced VF. Five consecutive episodes of VF were then induced with this S2 strength and coupling interval to ensure inducibility. An S3 of the same current strength as the S2 but with half the duration (5 ms) was then added to the stimulation protocol with an initial S2-S3 interval of either 15 or 20 ms. The S2-S3 intervals were increased at 20-ms intervals until 500 ms was reached. The S3 was then turned off, and several episodes of VF were induced by the S2 alone to demonstrate that the S2 was still effective in inducing VF at the end of the study. A defibrillation shock was given immediately after 8 seconds of data was acquired by the mapping system. There were 5-minute intervals between each fibrillation-defibrillation episode.
Histological Studies
At the end of the study, the tissue was excised and fixed in
formalin for at least 48 hours. The upper, lower, right, and left edges
were stained with black, green, blue, and yellow dyes, respectively.
The tissue was then embedded in paraffin. A section was taken parallel
to the epicardium and was stained with hematoxylin and eosin for
light-microscopic examination to determine the myocardial fiber
orientation.
Data Analysis
One or two episodes of baseline VF were analyzed for
each dog to document the consistent induction of figure-eight
reentry. To determine whether or not the S3 terminated the
reentrant wavefronts, we selectively analyzed a consecutive set
of five to seven episodes per dog. These episodes were 20 ms apart so
as to cover an interval of at least 100 ms. This coverage is necessary
because the average cycle length of VF in this model approximates 100
ms.6 The times of activation were determined by computer
according to the following algorithm (Fig 2
): The
maximal dv/dt of the range for data analysis was first
determined by the computer. In Fig 2
, the range for data
analysis included the entire tracing after the end of the
S2 artifact. The S2 artifact, which had an
artificially large dv/dt, was excluded. The investigators then had the
option to choose a threshold dv/dt value (a percentage of the maximal
dv/dt) and a threshold interval (in ms). In the example shown in Fig 2
,
the threshold values were 20% and 50 ms, respectively. The
computer selected a time as the time of local activation if the dv/dt
at that time exceeded the threshold value and if the interval between
that time and the time of previous activation exceeded the threshold
interval. Because each channel has a different signal-to-noise ratio,
the threshold value could vary from channel to channel at the
investigator's discretion. A threshold interval of roughly 50 ms was
usually used as a starting interval, but any interval could be used at
the discretion of the investigator. The vertical line in Fig 2
indicates the times of selected activations. The number at the top of
each line indicates the interval between that activation and the onset
of the S2 stimulation artifact. The unfilled arrows point
to the tick marks on the 0-mV baseline. These tick marks were separated
by 200 ms.
|
Because it was unlikely that the computers would be 100% specific and
sensitive in selecting activations, as was the case for channel I6 in
Fig 2
, manual editing was always performed for each activation. If two
deflections (double potentials) were observed, both deflections were
selected as activations regardless of the duration of this isoelectric
interval. Therefore, some activations selected may represent an
electrotonic activation rather than a true local activation. The solid
arrows in Fig 2
point to the deflections that would be manually
selected as activations. A dynamic display of activation patterns was
then visualized on a computer screen in which each electrode site was
illuminated when an activation was registered.
The advantage of selecting all deflections as activations is that the
investigators did not have to apply artificial criteria to reject or
accept a deflection as a local activation. The disadvantage is that it
is difficult to illustrate the dynamic display with a limited number of
still-frame pictures. For purposes of illustration, it was necessary to
also construct conventional isochronal activation
maps.6 10 The criteria for selecting local activations for
conventional isochronal map generation have been reported
elsewhere.7 11 Briefly, for the biphasic and the
multiphasic wave forms, the maximal slope of the activation complex was
selected by the computer to be the time of activation, and only one
activation time was assigned to the entire complex if no isoelectric
period was present within the complex. If the activation complexes
were monophasic with a single maximum or minimum, the time of
activation was assigned to be at the peak of the maximal deflection.
Only one activation was selected on the channel with multiple
activations to represent the time of these multiple complexes.
The activation that we selected was the one that was the largest and
had the steepest slope among all the neighboring activations. This
activation time was then used to match the activations on the other
channels, thus generating the isochronal map. For channel I6, shown
in Fig 2
, the deflections marked by the solid arrow B were selected to
match the activations in channel I19 for the isochronal map
generation. The deflections marked by arrows A, C, and D were not
selected for the purpose of generating isochronal maps. The
isochronal maps were then compared with the dynamic display to
ensure that the isochronal maps adequately represented
the direction of the wavefront propagation shown in the display.
To determine whether or not the effects of the S3 were influenced by the recovery interval preceding the S3, we determined the times of activation recorded by the electrodes near the S2 and the S3 sites. Instead of selecting a single channel to represent the times of activation in that region, we used a group of channels near the S2. The reentrant wavefronts were displayed dynamically on the screen. The time was advanced in 10-ms steps. The site near the S2 and the S3 was deemed activated if more than three channels around the stimulation site were activated within that 10-ms window. The interval between the S3 and the immediately preceding activation at the site of the S3 was defined as the recovery interval for the S3. This recovery interval was an estimate of the status of repolarization of the cells near the S3. A short recovery interval implies that the cells had only a short time to recover from a previous activation and therefore were most likely still refractory at the time of S3 stimulus. On the other hand, a long recovery interval implies that the cells had a long time to recover, allowing S3 to elicit a full response. An intermediate recovery interval implies that the cells were relatively refractory. A strong stimulus given during this time might induce graded responses12 and not full action potentials. These graded responses may prolong the duration of refractoriness and contribute to the induction of new reentrant wavefronts and VF.6 7
All statistical analysis was performed by use of
SYSTAT.13 Analysis of variance was
used to compare the recovery intervals for the S3
associated with different responses: S3 that aborted
reentry, S3 that changed patterns of reentry, and
S3 that did not change the baseline figure-eight reentrant
pattern. A value of P
.05 was considered significant.
| Results |
|---|
|
|
|---|
|
|
A total of 40 episodes were analyzed. Among them, 7 episodes were baseline VF and 6 episodes had S2-S3 intervals that were too short to allow the reentrant wavefront to complete one rotation. In the remaining 27 episodes, the S3 was followed by sinus rhythm in 9 episodes and followed by VF in 18 episodes.
S3 Did Not Terminate VF
Among the 18 episodes in which the S3 was followed by
VF, 10 episodes were associated with continuation patterns of
figure-eight reentry. Fig 5
shows one example, when the
S3 was given 155 ms after the S2. The patterns
of activation after the S3 were similar to those before the
S3, with persistence of the figure-eight reentry.
There was juxtaposition of early and late sites in consecutive
activations. Fig 6
shows the actual activations
recorded. The recovery interval for the S3 in this
example was 37 ms measured at site I8. This short recovery interval
implies that the S3 occurred at the early stages of
repolarization. Among the 10 episodes with continuation of figure-eight
reentry and VF, 5 episodes had short recovery intervals (
30 ms). The
average recovery interval of these 5 episodes was 22±8 ms. In the
remaining 5 episodes, the recovery intervals were long (
80 ms), with
an average of 94±15 ms.
|
|
When the S3 was given with an S3 recovery
interval of 61±20 ms, the patterns of activation changed from a
figure-eight reentry into a focal pattern (n=2), single loop of reentry
(n=2), or complex activation patterns showing neither a clear focus nor
a reentrant wavefront (n=4). In all 8 episodes, VF continued despite
the loss of the figure-eight reentrant pattern on the epicardium. Figs 7
and 8
show an example of the
S3 changing the pattern of activation from a figure-eight
into a focal pattern. Fig 7A
shows a figure-eight pattern with the
latest activation occurring roughly 155 ms after the S2
stimulation. Fig 7B
shows the second activation after the
S2. The S3 was given at 195 ms, which
interrupted the figure-eight reentrant pattern. Fig 7C
shows that the
wavefront shown in B continued to activate the remaining parts
of the mapped region after the time of the S3. Fig 7D
shows
that a new pattern of activation occurred 70 ms after the
S3 (arrow). Fig 7E
shows subsequent activation, which
differs from the previous activation because a large area was
activated by stimulations within 10 ms of each other (red).
Although the early site in E and the late site in D (the blue area
above the arrow in D) were spatially close to each other, they were
temporally quite separated. The earliest site in E occurred 390 ms
after the S2, which was 70 ms after the activation
wavefront last visited this area. These patterns of activation in Fig 7D
and 7E
are most compatible with epicardial breakthrough from a focus
or intramural reentrant pathway inside the myocardium. Fig 8
shows the actual activations recorded. The recovery interval for
the S3 as measured at electrode sites I8 and I9 in this
episode was
80 ms, which was associated with a significant
alteration of the figure-eight reentrant pattern.
|
|
S3 Terminates Reentry and Protects the Heart From
VF
When the S3 was given slightly earlier (n=9), both
reentry and VF were abruptly terminated. Figs 9
and 10
show an example. The S2-S3
interval was 155 ms. Fig 9A
shows a figure-eight reentrant pattern
induced by an S2. The reentrant excitation was interrupted
by the S3 stimulus (Fig 9B
). Fig 9C
shows the wavefront
propagation after the S3. This wavefront was a continuation
of that shown in B. Reentry did not continue, and VF was prevented. Fig 10
shows actual activations recorded from the same episode. Channel
M9 shows that reentrant excitation occurred after the S2.
However, the S3 terminated reentry between O13 and M13.
Among the nine episodes in which an S3 aborted reentry and
protected the heart from VF, the recovery interval for the
S3 averaged 39±12 ms.
|
|
Relation Between Recovery Interval and the Effects of
S3
Fig 11
shows the distribution of the recovery
intervals. The protective zone was distributed from 20 to 60 ms, and
the vulnerable zone (new patterns of activation) was distributed from
30 to 90 ms. The recovery intervals associated with no change of
activation were distributed at the two ends of the spectrum. The
differences among the recovery intervals for these four groups of
recovery intervals were statistically significant (P<.001
by analysis of variance).
|
Histological Examinations
Histological sections showed normal canine
ventricular myocardium (Fig 12
). There was no evidence of tissue necrosis or scar
formation that could form anatomic barriers to prevent electrical
activation. If the lower edge of the mapping plaque was used as 0°
reference, with the angles taken counterclockwise, the angle of the
fiber orientation averaged 35±21°. The angle between the fiber
orientation and the line connecting the S1 and the
S2 averaged 22±27°.
|
| Discussion |
|---|
|
|
|---|
|
Protective Zone
A "protective zone" is known to be present in the
cardiac cycle, during which a stimulus can prevent the induction of VF
by an earlier stimulus (S2) delivered during the vulnerable
period.1 2 It has been hypothesized that the stimulus
exerts its protective effects by terminating local reentrant activity
induced by an earlier stimulus.3 The results of this study
confirmed this hypothesis. However, we also demonstrated that the
stimulus can prevent the continuation of reentry and VF only when it
falls within a specific period during reentrant excitation. This
specific period occurred 39 ms after the previous activation, an
interval insufficiently long for the ventricular cells to
fully recover from previous activation.11 A strong
stimulus occurring before complete recovery may induce graded
responses12 16 and hence prolong the action potential
duration and refractoriness.17 18 When the leading edge of
the reentrant wavefront revisited this area, it could not reenter. This
circumstance thus resulted in bidirectional conduction block and the
termination of reentry.
Vulnerable Period
Shortly after the protective zone, an S3 changed the
patterns of activation but did not terminate VF. The changes were not
subtle. In some parts of the mapped region, the wavefronts traveled in
opposite directions before and after the S3. This finding
indicates that the S3 initiated new patterns of activation,
while the reentrant wavefronts preceding the S3 were
terminated. The recovery interval associated with new patterns of
activation averaged 61 ms. This interval roughly corresponded to the
relative refractory period that exists in fibrillating
ventricular cells.11
No Change of Activation
When the recovery interval (94±15 ms) was almost as long as the
VF cycle length, the S3 occurred at a time when the cells
would have been activated by the reentrant wavefront. The
S3 therefore did not significantly change the patterns of
activation. On the other hand, if the recovery interval was 22±8 ms,
the S3 had occurred in the early stages of repolarization.
Because a stimulus occurring in the very early stages of repolarization
may not result in significant alteration of the action
potential,12 the S3 did not significantly
change the patterns of activation. In either case, the figure-eight
reentrant pattern was allowed to continue undisturbed.
Although the figure-eight reentry was unchanged, the patterns of
activation shown in Fig 5
indicate that the S3 nevertheless
had some influence on the reentrant wavefronts. One evidence is that
the frame line of Fig 5C
moved closer to the S1 site than
the frame line shown in Fig 5A
. These findings indicate that the
S3 might have activated cells that would not have
been activated by the original reentrant wavefronts. Depending
on the strength and the timing of the S3, the number
of the cells activated may also change. Therefore, even when
figure-eight reentry was maintained, the S3 may still
influence the patterns of the reentrant activation.
Implications Regarding the Mechanisms of
Defibrillation
It is well known that successful defibrillation depends on the
strength of the electric shock; the higher the shock strength, the
greater the probability of successful defibrillation.19
However, the importance of the timing of the shock on the results of
defibrillation has not been fully appreciated. In this study, we
demonstrated that a second premature stimulus (S3) could
either terminate reentry or perpetuate reentry induced by an earlier
premature stimulus (S2), depending on the time in the
activation cycle at which the stimulus occurs. A vulnerable period
(61±20 ms after the preceding activation) was identified. The timing
of this vulnerable period was similar to the timing of the preshock
intervals at the early sites after an unsuccessful defibrillation shock
(64±11 ms).10 This relationship supports the
hypothesis10 20 21 22 23 that an unsuccessful shock terminates
all activation wavefronts but fails to halt VF because it initiates new
activation wavefronts by falling into the vulnerable period. Successful
defibrillation occurs if the shock strength is above the upper limit of
vulnerability so that it cannot reinitiate VF. Alternatively, if the
shock strength is below the upper limit of vulnerability in only a
small area of the ventricles but the timing of activation in that area
happens to be in the protective zone, then the shock can also
successfully defibrillate. Because the activation patterns during VF
are complex, whether a shock will occur during the protective or the
vulnerable zone is determined by chance. Furthermore, because the upper
limit of vulnerability is also a probability
function,24 25 whether or not a shock delivered during the
vulnerable period will reinduce VF is also determined partially by
chance. Therefore, defibrillation threshold testing is a probability
function,19 and the probability-of-success curve for
defibrillation threshold testing may be shallower than the
probability-of-success curve for the upper limit of vulnerability
testing.26
Limitation of the Study
One limitation of this study is in the methods used for the
measurement of the recovery interval near the site of the
S3. The activations near this site often had small
amplitudes and a slow rate of rise (channel I8 in Fig 6
). These
deflections may represent electrotonic responses and not true
local activation. To partially circumvent this uncertainty, we measured
the times of activation recorded by the activation of a group of
three or more electrodes near the site of the S3,
rather than by any single arbitrarily selected electrode. If three or
more electrodes near the S3 were activated within
10 ms of each other, that 10-ms window was used as the time of
activation. The difference between this 10-ms window and the 10-ms
window that included the S3 was the recovery interval for
that episode. In the example shown in Fig 6
, the recovery interval of
channel I8 was 37 ms, whereas the recovery interval entered into
statistical analysis and Fig 11
was 30 ms.
For future clinical applications, these small and low-amplitude electrograms near the site of the S3 may not be detectable by the implanted devices. We also analyzed the recovery intervals based on the large-amplitude electrograms near the earliest site of the reentrant circuit. In this model, the earliest sites were between the sites of the S1 and the S2. The results showed that the recovery intervals for the protective, vulnerable, and no-change zones were also statistically different. Whether this latter method will prove to be more clinically useful is unknown.
| Acknowledgments |
|---|
| Footnotes |
|---|
Received October 26, 1994; accepted April 14, 1995.
| References |
|---|
|
|
|---|
2.
Tamargo J, Moe B, Moe GK. Interaction of
sequential stimuli applied during the relative refractory period in
relation to determination of fibrillation threshold in canine
ventricle. Circ Res. 1975;37:534-541.
3. Euler DE, Moore NE. Continuous fractionated electrical activity after stimulation of the ventricles during the vulnerable period: evidence for local reentry. Am J Cardiol. 1980;46:783-791. [Medline] [Order article via Infotrieve]
4. Krinsky VI, Biktashev VN, Pertsov AM. Autowave approaches to cessation of reentrant arrhythmias. Ann N Y Acad Sci. 1990;591:232-246. Review. [Medline] [Order article via Infotrieve]
5. Winfree AT. Ventricular reentry in three dimensions. In: Zipes DP, Jalife J, eds. Cardiac Electrophysiology: From Cell to Bedside. Philadelphia, Pa: WB Saunders Co; 1990:224-234.
6.
Chen P-S, Wolf P, Dixon EG, Danieley ND, Frazier DW,
Smith WM, Ideker RE. Mechanism of ventricular
vulnerability to single premature stimuli in open chest dogs.
Circ Res. 1988;62:1191-1209.
7.
Chen P-S, Cha Y-M, Peters BB, Chen LS. Effects
of myocardial fiber orientation on the electrical induction of
ventricular fibrillation. Am J Physiol. 1993;264:H1760-H1773.
8.
Cha Y-M, Peters BB, Birgersdotter-Green U, Chen P-S.
A reappraisal of ventricular fibrillation threshold
testing. Am J Physiol. 1993;264:H1005-H1010.
9. Amlie JP, Owren T. The effect of prolonged pentobarbital anaesthesia on cardiac electrophysiology and inotropism of the dog heart in situ. Acta Pharmacol Toxicol. 1979;44:264-271. [Medline] [Order article via Infotrieve]
10.
Chen P-S, Wolf PD, Melnick SD, Danieley ND, Smith WM,
Ideker RE. Comparison of activation during
ventricular fibrillation and following unsuccessful
defibrillation shocks in open chest dogs. Circ
Res. 1990;66:1544-1560.
11.
Cha Y-M, Birgersdotter-Green U, Wolf PL, Peters BB,
Chen P-S. The mechanisms of termination of reentrant activity in
ventricular fibrillation. Circ
Res. 1994;74:495-506.
12. Kao CY, Hoffman BF. Graded and decremental response in heart muscle fibers. Am J Physiol. 1958;194:187-196.
13. Wilkinson L. SYSTAT: The System for Statistics. Evanston, Ill: SYSTAT, Inc; 1989.
14. Wiggers CJ. The mechanism and nature of ventricular fibrillation. Am Heart J. 1940;20:399-412.
15. Winfree AT. Electrical instability in cardiac muscle: phase singularities and rotors. J Theor Biol. 1989;138:353-405. [Medline] [Order article via Infotrieve]
16. Weidmann S. Effects of current flow on the membrane potential of cardiac muscle. J Physiol. 1951;115:227-236.
17. Gotoh M, Chen P-S, Mandel WJ, Karagueuzian HS. Graded responses and reentrant rotors induced by a premature stimulus. Circulation. 1993;88(suppl I):I-626. Abstract.
18. Gotoh M, Chen P-S, Mandel WJ, Peter CT, Fan W, Karagueuzian HS. Upper limit of vulnerability for rotor induction in normal ventricular myocardium in vitro. PACE Pacing Clin Electrophysiol. 1993;16:897. Abstract.
19. Davy JM, Fain ES, Dorian P, Winkle RA. The relationship between successful defibrillation and delivered energy in open-chest dogs: reappraisal of the `defibrillation threshold' concept. Am Heart J. 1987;113:77-84. [Medline] [Order article via Infotrieve]
20. Chen P-S, Shibata N, Wolf P, Dixon EG, Danieley ND, Sweeney MB, Smith WM, Ideker RE. Activation during ventricular defibrillation in open-chest dogs: evidence of complete cessation and regeneration of ventricular fibrillation after unsuccessful shocks. J Clin Invest. 1986;77:810-823.
21.
Chen P-S, Shibata N, Dixon EG, Martin RO, Ideker RE.
Comparison of the defibrillation threshold and the upper limit
of ventricular vulnerability.
Circulation. 1986;73:1022-1028.
22.
Chen P-S, Wolf PD, Ideker RE. The mechanism of
cardiac defibrillation: a different point of view.
Circulation. 1991;84:913-919.
23.
Johnson EE, Alferness CA, Wolf PD, Smith WM, Ideker RE.
Effect of pulse separation between two sequential biphasic
shocks given over different lead configurations of
ventricular defibrillation efficacy.
Circulation. 1992;85:2267-2274.
24.
Chen P-S, Feld GK, Kriett JM, Mower MM, Tarazi RY,
Fleck RP, Swerdlow CD, Gang ES, Kass RM. Relation between upper
limit of vulnerability and defibrillation threshold in humans.
Circulation. 1993;88:186-192.
25. Kavanagh KM, Harrison JH, Dixon EG, Guse P, Smith WM, Wharton JM, Ideker RE. Correlation of the probability of success curves for defibrillation and for the upper limit of vulnerability. PACE Pacing Clin Electrophysiol. 1990;13:536. Abstract.
26. Idriss SF, Walker RG, Malkin RA, Ideker RE. Effect of rapid pacing and T-wave scan on upper limit defibrillation estimate. Am Heart J. 1994;128:632. Abstract.
This article has been cited by other articles:
![]() |
P.-S. Chen, T.-J. Wu, C.-T. Ting, H. S. Karagueuzian, A. Garfinkel, S.-F. Lin, and J. N. Weiss A Tale of Two Fibrillations Circulation, November 11, 2003; 108(19): 2298 - 2303. [Full Text] [PDF] |
||||
![]() |
S. Zhou, C.-M. Chang, T.-J. Wu, Y. Miyauchi, Y. Okuyama, A. M. Park, A. Hamabe, C. Omichi, H. Hayashi, L. A. Brodsky, et al. Nonreentrant focal activations in pulmonary veins in canine model of sustained atrial fibrillation Am J Physiol Heart Circ Physiol, September 1, 2002; 283(3): H1244 - H1252. [Abstract] [Full Text] [PDF] |
||||
![]() |
J. N. Weiss, P.-S. Chen, Z. Qu, H. S. Karagueuzian, and A. Garfinkel Ventricular Fibrillation : How Do We Stop the Waves From Breaking? Circ. Res., December 8, 2000; 87(12): 1103 - 1107. [Abstract] [Full Text] [PDF] |
||||
![]() |
M. Yashima, T. Ohara, J.-M. Cao, Y.-H. Kim, M. C. Fishbein, W. J. Mandel, P.-S. Chen, and H. S. Karagueuzian Nicotine increases ventricular vulnerability to fibrillation in hearts with healed myocardial infarction Am J Physiol Heart Circ Physiol, June 1, 2000; 278(6): H2124 - H2133. [Abstract] [Full Text] [PDF] |
||||
![]() |
Y.-H. Kim, F. Xie, M. Yashima, T.-J. Wu, M. Valderrabano, M.-H. Lee, T. Ohara, O. Voroshilovsky, R. N. Doshi, M. C. Fishbein, et al. Role of Papillary Muscle in the Generation and Maintenance of Reentry During Ventricular Tachycardia and Fibrillation in Isolated Swine Right Ventricle Circulation, September 28, 1999; 100(13): 1450 - 1459. [Abstract] [Full Text] [PDF] |
||||
![]() |
R. N. Doshi, T.-J. Wu, M. Yashima, Y.-H. Kim, J. J. C. Ong, J.-M. Cao, C. Hwang, P. Yashar, M. C. Fishbein, H. S. Karagueuzian, et al. Relation Between Ligament of Marshall and Adrenergic Atrial Tachyarrhythmia Circulation, August 24, 1999; 100(8): 876 - 883. [Abstract] [Full Text] [PDF] |
||||
![]() |
J.-M. Cao, Z. Qu, Y.-H. Kim, T.-J. Wu, A. Garfinkel, J. N. Weiss, H. S. Karagueuzian, and P.-S. Chen Spatiotemporal Heterogeneity in the Induction of Ventricular Fibrillation by Rapid Pacing : Importance of Cardiac Restitution Properties Circ. Res., June 11, 1999; 84(11): 1318 - 1331. [Abstract] [Full Text] [PDF] |
||||
![]() |
T. Uchida, M. Yashima, M. Gotoh, Z. Qu, A. Garfinkel, J. N. Weiss, M. C. Fishbein, W. J. Mandel, P.-S. Chen, and H. S. Karagueuzian Mechanism of Acceleration of Functional Reentry in the Ventricle : Effects of ATP-Sensitive Potassium Channel Opener Circulation, February 9, 1999; 99(5): 704 - 712. [Abstract] [Full Text] [PDF] |
||||
![]() |
T. Ohara, M. Yashima, A. Hamzei, M. Favelyukis, A. Park, Y.-H. Kim, W. J. Mandel, P.-S. Chen, and H. S. Karagueuzian Nicotine Increases Spatiotemporal Complexity of Ventricular Fibrillation Wavefront on the Epicardial Border Zone of Healed Canine Infarcts Journal of Cardiovascular Pharmacology and Therapeutics, January 1, 1999; 4(2): 121 - 127. [Abstract] [PDF] |
||||
![]() |
Z. Qu, J. N. Weiss, and A. Garfinkel Cardiac electrical restitution properties and stability of reentrant spiral waves: a simulation study Am J Physiol Heart Circ Physiol, January 1, 1999; 276(1): H269 - H283. [Abstract] [Full Text] [PDF] |
||||
![]() |
C. A. Athill, T. Ikeda, Y.-H. Kim, T.-J. Wu, M. C. Fishbein, H. S. Karagueuzian, and P.-S. Chen Transmembrane Potential Properties at the Core of Functional Reentrant Wave Fronts in Isolated Canine Right Atria Circulation, October 13, 1998; 98(15): 1556 - 1567. [Abstract] [Full Text] [PDF] |
||||
![]() |
T.-J. Wu, M. Yashima, F. Xie, C. A. Athill, Y.-H. Kim, M. C. Fishbein, Z. Qu, A. Garfinkel, J. N. Weiss, H. S. Karagueuzian, et al. Role of Pectinate Muscle Bundles in the Generation and Maintenance of Intra-atrial Reentry : Potential Implications for the Mechanism of Conversion Between Atrial Fibrillation and Atrial Flutter Circ. Res., August 24, 1998; 83(4): 448 - 462. [Abstract] [Full Text] [PDF] |
||||
![]() |
J. S. Strobel, B. H. KenKnight, D. L. Rollins, W. M. Smith, and R. E. Ideker The effects of ventricular fibrillation duration and site of initiation on the defibrillation threshold during early ventricular fibrillation J. Am. Coll. Cardiol., August 1, 1998; 32(2): 521 - 527. [Abstract] [Full Text] [PDF] |
||||
![]() |
T.-J. Wu, J. J. C. Ong, C. Hwang, J. J. Lee, M. C. Fishbein, L. Czer, A. Trento, C. Blanche, R. M. Kass, W. J. Mandel, et al. Characteristics of wave fronts during ventricular fibrillation in human hearts with dilated cardiomyopathy: role of increased fibrosis in the generation of reentry J. Am. Coll. Cardiol., July 1, 1998; 32(1): 187 - 196. [Abstract] [Full Text] [PDF] |
||||
![]() |
Y. Y. Kwan, W. Fan, D. Hough, J. J. Lee, M. C. Fishbein, H. S. Karagueuzian, and P.-S. Chen Effects of Procainamide on Wave-Front Dynamics During Ventricular Fibrillation in Open-Chest Dogs Circulation, May 12, 1998; 97(18): 1828 - 1836. [Abstract] [Full Text] [PDF] |
||||
![]() |
M. R. Ujhelyi, J. J. Sims, and A. W. Miller High-dose lidocaine does not affect defibrillation efficacy: implications for defibrillation mechanisms Am J Physiol Heart Circ Physiol, April 1, 1998; 274(4): H1113 - H1120. [Abstract] [Full Text] [PDF] |
||||
![]() |
T. Ikeda, M. Yashima, T. Uchida, D. Hough, M. C. Fishbein, W. J. Mandel, P.-S. Chen, and H. S. Karagueuzian Attachment of Meandering Reentrant Wave Fronts to Anatomic Obstacles in the Atrium : Role of the Obstacle Size Circ. Res., November 19, 1997; 81(5): 753 - 764. [Abstract] [Full Text] |
||||
![]() |
T. Ikeda, L. Czer, A. Trento, C. Hwang, J. J. C. Ong, D. Hough, M. C. Fishbein, W. J. Mandel, H. S. Karagueuzian, and P.-S. Chen \E Induction of Meandering Functional Reentrant Wave Front in Isolated Human Atrial Tissues Circulation, November 4, 1997; 96(9): 3013 - 3020. [Abstract] [Full Text] |
||||
![]() |
K. Kamjoo, T. Uchida, T. Ikeda, M. C. Fishbein, A. Garfinkel, J. N. Weiss, H. S. Karagueuzian, and P.-S. Chen Importance of Location and Timing of Electrical Stimuli in Terminating Sustained Functional Reentry in Isolated Swine Ventricular Tissues : Evidence in Support of a Small Reentrant Circuit Circulation, September 16, 1997; 96(6): 2048 - 2060. [Abstract] [Full Text] |
||||
![]() |
M. Gotoh, T. Uchida, W. J. Mandel, M. C. Fishbein, P.-S. Chen, and H. S. Karagueuzian Cellular Graded Responses and Ventricular Vulnerability to Reentry by a Premature Stimulus in Isolated Canine Ventricle Circulation, April 15, 1997; 95(8): 2141 - 2154. [Abstract] [Full Text] |
||||
![]() |
T. Ikeda, T. Uchida, D. Hough, J. J. Lee, M. C. Fishbein, W. J. Mandel, P.-S. Chen, and H. S. Karagueuzian Mechanism of Spontaneous Termination of Functional Reentry in Isolated Canine Right Atrium: Evidence for the Presence of an Excitable but Nonexcited Core Circulation, October 15, 1996; 94(8): 1962 - 1973. [Abstract] [Full Text] |
||||
![]() |
J. J. Lee, K. Kamjoo, D. Hough, C. Hwang, W. Fan, M. C. Fishbein, C. Bonometti, T. Ikeda, H. S. Karagueuzian, and P.-S. Chen Reentrant Wave Fronts in Wiggers' Stage II Ventricular Fibrillation : Characteristics and Mechanisms of Termination and Spontaneous Regeneration Circ. Res., April 1, 1996; 78(4): 660 - 675. [Abstract] [Full Text] |
||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
|
Circulation Research Home | Subscriptions | Archives | Feedback | Authors | Help | AHA Journals Home | Search Copyright © 1995 American Heart Association, Inc. All rights reserved. Unauthorized use prohibited. |