(Circulation. 2001;103:2857.)
© 2001 American Heart Association, Inc.
Basic Science Reports |
From the Cardiovascular Division, Department of Internal Medicine, the University of Virginia Health System, Charlottesville, Va.
Correspondence to David E. Haines, MD, University of Virginia Health System, Cardiovascular Division, PO Box 800158, Charlottesville, VA 22908. E-mail dhaines{at}virginia.edu
| Abstract |
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Methods and ResultsA total of 15 dogs (weight, 28.2±3.4 kg) were rapidly paced for 48 to 72 hours to induce AF. Coil electrodes with a surface area of 1.80 cm2 were then placed in the left and right atria to form a wide bipole. Wide bipolar electrograms were digitally filtered, and a fast Fourier transform was performed over a sliding 2-s window every 0.5 s. The organization index (OI) was calculated as the ratio of the area of the dominant peak and its harmonics to the total area of the magnitude spectrum. The atrial defibrillation threshold (ADFT50) was determined using a 3-ms/3-ms biphasic shock and an up-down-up protocol. Additional shocks with higher and lower energies were delivered in a random sequence to develop a distribution curve. The OI varied over time, with a mean of 0.42±0.03, a maximum of 0.65±0.07, and a minimum of 0.20±0.06. The OI changed rapidly, with durations of high organization (OI>0.5) ranging from 1 to 5 s. The ADFT50 for QRS complexsynchronized shocks was 183±56 V, versus 142±49 V for shocks synchronized to an OI>0.5 (P<0.001). The distribution curve shifted leftward when shocks were synchronized to an OI>0.5.
ConclusionsAF signals show a high degree of variability. Shock efficacy is increased when shocks are delivered during periods of high AF organization as determined by the OI method.
Key Words: arrhythmia fibrillation defibrillation Fourier analysis
| Introduction |
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It has been theorized that the most common mechanism of AF is reentry with multiple simultaneous wavelets circulating in the atria.17 It has also been shown that 4 to 6 wavelets are needed in order to sustain continuous propagation of AF.18 The number of wavelets circulating in the atria probably varies over time, changing with changing global and regional atrial refractoriness.19 A decrease in wavelength likely will decrease the prevalence of anatomic (as opposed to functional) reentrant waves, thereby decreasing the regions of excitable gap.17 20
We hypothesized that decreasing numbers of wavelets and increasing regions of excitable gaps might increase atrial defibrillation efficacy, and visa versa. A method that could quantify these periods of high and low AF organization, respectively, might improve the likelihood of atrial defibrillation. We sought to accomplish this with frequency domain analysis of a filtered wide bipolar atrial electrogram, analogous to an interatrial defibrillation lead system. We conjectured that discrete harmonic wavelet activity would predict higher defibrillation efficacy and lower defibrillation energy requirements.
| Methods |
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After 48 to 72 hours of rapid atrial pacing, the animals were anesthetized and the femoral vessels were accessed via cutdown incision. Two transseptal catheterizations were performed using a Brockenbrough needle and two 9.5F 60-cm sheaths. Decapolar catheters with 10-mm spacing between each bipole were placed in the right and left atrium for electrogram recording. Defibrillation catheters were placed contiguous to the right and left atrial free walls, and from them, an interatrial bipole electrogram was acquired. A 6F quadripolar sensing catheter was placed retrogradely into the left ventricle for atrial shock synchronization. At the completion of the protocol, the dogs were euthanized with a barbiturate overdose.
Signal Processing
The wide bipole signal obtained from the
defibrillation catheters
(Figure 1A
) was digitized at 1000 Hz using a 66-MHz computer
with a 486 processor and an AT-DSP2200 data acquisition card (National
Instruments Corp) programmed in Turbo C++. An ideal QRS was determined
by averaging 100 QRS complexes. This ideal QRS was then subtracted from
each individual QRS complex in the signal. After QRS subtraction, the
resulting AF wave form
(Figure 1B
) was band-pass filtered using a 40- to 250-Hz
second-order digital Butterworth filter. The absolute value of the
filtered wave form was low-pass filtered using a 20-Hz second-order
digital Butterworth filter
(Figure 1C
). This filtering process extracts a time-varying
wave form proportional to the amplitude of the high-frequency
components in the original atrial electrogram, enhancing the
periodicity or nonperiodicity of the signal. This algorithm was used to
transform a complex wave form into a series of atrial activations while
diminishing the effects of changing electrogram morphology or
amplitude.21 22
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Frequency Domain Analysis
A fast Fourier transform (FFT) was calculated on the
digitally filtered wave form over a sliding 2-s window of 2048 points
every 0.5 s
(Figure 2
). The data were tapered using a split-cosine bell
window. The largest peak of the resulting magnitude spectrum was
identified, and on the basis of its position, the positions of the
harmonic peaks were determined. The areas under the largest peak and 3
of its harmonic peaks were calculated over a 1-Hz window, producing an
area under 4 peaks. The total area of the spectrum was calculated from
2.5 Hz up to, but not including, the fifth harmonic peak. Higher
frequencies were excluded because they were assumed to exceed the
physiological range of frequencies for AF wavelets.
The ratio of the power under the harmonic peaks to the total power in
this range was calculated, and the resulting number was termed the
organization index (OI). We theorized that the OI represents
the organization of AF during the 2-s time window. A spectrum
with a dominant peak and discrete harmonics would represent
fewer wavelets circulating within the atria and thus a higher OI. With
a higher number of wavelets, more frequency components are added to the
atrial signal, which would appear in the spectrum and result in a lower
OI. An OI threshold >0.5 was selected to represent periods
with relatively organized AF signals.
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Defibrillation Protocol
In all cases, atrial defibrillation was performed
after spontaneous or induced AF of
30 s sustained duration. After
each cardioversion, AF was reinitiated with 10-s bursts of rapid atrial
pacing at a 50-ms cycle length, an output of 10 mA, and a 9.9-ms pulse
width. The defibrillation catheters were specially constructed 7F
catheters with stainless steel defibrillation coils (Boston Scientific
Corp) with a surface area of 1.80 cm2. These
coils were connected to a Ventritex HVS-02 programmable defibrillator
(Ventritex, St. Jude Corp) with a capacitance of 150 µF. Each shock
was a truncated biphasic, exponential wave form with a pulse width of 3
ms/3 ms synchronized to the left ventricular apical
electrogram. Each phase of the wave form had a 35% tilt with a
100-µs gap between the positive and negative phases. The leading-edge
voltage was adjustable over a range of 50 to 990 V in 10-V steps. All
shocks were synchronized either to the left ventricular
apical electrogram alone or to the ventricular signal found
in the signal collected from the defibrillation catheters and to
periods of high measured AF organization.
The atrial defibrillation threshold (ADFT50) was determined using an up-down-up protocol starting at 50 V and (1) increased in 20-V increments until a successful conversion to sinus rhythm was accomplished; then (2) decreased in 20-V decrements until 2 consecutive shocks failed to convert the rhythm; and (3) increased in 20-V increments until 2 consecutive shocks converted the rhythm to sinus. AF was reinitiated as needed during the protocol and allowed to persist for at least 30 s before each shock. The defibrillation threshold was defined as the mean voltage of the 2 consecutive unsuccessful shocks from step 2 and the 2 consecutive successful shocks from step 3. A successful cardioversion was defined as restoration of sinus rhythm within 1 s of energy delivery. In 8 dogs, the ADFT50 was first determined using QRS-synchronized shocks. In 7 dogs, the ADFT50 was first determined using shocks synchronized both to the QRS and to periods when the OI exceeded the threshold level of 0.5. To obtain additional shocks higher and lower than the ADFT50 on the distribution curve, shocks were delivered at fixed energy levels between the lower and upper threshold energy levels, which were identified while determining the ADFT50. Shocks were selected in 20-V steps that were delivered while randomly alternating between QRS-synchronized shocks and shocks synchronized both to the QRS and to periods of OI>0.5.
Statistical Analysis
Data were expressed as the mean±SD. A 2-tailed,
paired Students t test was
used to compare ADFT50 values. Energy levels
closest to ±10% and ±20% of the ADFT50 were
pooled in order to generate a distribution function for the 2 groups
(random OI and OI>0.5). The actual energies representing
the ADFT50 and the ±10% and ±20% values were
presented in the distribution function graphs as mean±SD.
Differences between the curves were determined with a 2-factor ANOVA.
Data were tested for normality using the Kolmogorov-Smirnov test.
Statistical significance was defined as
P<0.05.
| Results |
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ADFT50 results for random shocks and
for shocks synchronized to an OI>0.5 for each of the dogs are shown in
Figure 4
. The mean ADFT50 for
QRS-synchronized shocks was 183±56 V, versus 142±49 V for shocks
synchronized both to the QRS and to the point when the OI exceeded 0.5
(P=0.00064). Of the 15 animals,
13 showed a decrease in the ADFT50 when shocks
were synchronized to an OI>0.5. Of note is the fact that the 2
animals that did not show a change in the ADFT50
had the lowest mean OI overall and a higher OI variance (0.38±0.07
versus 0.43±0.024; P<0.03). A
probability distribution curve was generated for each animal, and the
average of these curves is shown in
Figure 5
. The curve for shocks synchronized both to the QRS
and to an OI>0.5 is shifted leftward toward lower energy levels
(P<0.001).
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| Discussion |
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We then applied this methodology to intra-atrial
defibrillation. The OI algorithm proved very sensitive to the changes
in the appearance of the raw and filtered AF signals and changed
dynamically with each 0.5-s interval calculation. Shocks delivered
during periods of high OI (hypothesized to correlate with fewer
wavelets and increased excitable gap) had a higher efficacy than
randomly delivered shocks. When the algorithm was used to select the
timing of shock delivery during intra-atrial defibrillation, the
leading-edge voltage needed for a successful conversion to normal sinus
rhythm 50% of the time (the ADFT50) was reduced
by
30%. Application of the OI algorithm also shifted the
probability of successful defibrillation toward lower energy levels
over a wide range of leading-edge voltages.
Mechanisms of Atrial Defibrillation
The mechanism of atrial defibrillation is not fully
understood. Several studies have been performed analyzing the mechanism
of ventricular
fibrillation27 28 29
and experimenting with different techniques to improve
ventricular defibrillation
efficacy.30 31
From these studies, several theories have been developed about the
requirements for successful ventricular defibrillation,
among them: (1) A critical mass of myocardium must be
depolarized;27 (2) a
sufficient amount of current density must travel through the
myocardium;28
and (3) there must be a prolongation of refractoriness in the
myocardium after the
shock.29 Whether or not
these theories can be applied to atrial defibrillation is unknown. As
in ventricular defibrillation, however, it has been
theorized that in order to achieve a successful atrial defibrillation,
a critical mass of atrial tissue needs to be depolarized, thereby
terminating the wavelets.6 To
depolarize the atrial tissue, a dominating electrical current is needed
to overcome the varying states of activation of the atria caused by the
circulating wavelets associated with AF. A higher number of wavelets
might result in an increased mass of atrial myocardium that
is not fully excitable and might translate into higher energy
requirements for a successful defibrillation.
Previous Studies
High-density mapping frequently has been used as
a method to measure AF organization. It has been shown that there are
multiple wavelets circulating in the atria during
AF17 and that there are time
periods during which AF seems more
organized.32 Algorithms have
been developed in an attempt to quantify AF organization. Botteron et
al21 22 developed
an algorithm that measured the correlation of atrial activation from 5
equally spaced electrodes. The correlation-versus-electrode distance
was a decaying exponential function from which a spatial organization
constant was calculated. In this method, calculations were made over AF
recorded longer than 30 s that averaged out any temporal
variability in the AF organization. Sih et
al33 developed an algorithm
that measured AF organization by calculating the mean-squared error in
the linear prediction between AF signals from 2 electrodes. This
calculation was performed over a sliding 300-ms window every 10 ms.
Smaller mean-squared error values would indicate a more organized
signal. Although both of these algorithms measure AF organization, they
do so in a relatively small region of the atria, thus providing a
measurement of only local AF organization. These prior algorithms have
not been reported to improved likelihood of successful atrial
defibrillation. The algorithm presented in this study provides
a high temporal resolution of AF organization over a wide bipole across
both atria, giving a global measurement of organization, and was
demonstrated to improve shock delivery timing during AF in order to
optimize defibrillation efficacy.
Clinical Implications
A limitation for the use of the atrial implantable
defibrillator as a possible therapy for AF is shock-related discomfort.
Clinical studies have shown that the energy needed for successful
cardioversion in humans is much higher than the energy needed for
cardioversion in
animals.14 15 16 34
Clinical studies have also shown that shocks >2 J resulted in patient
discomfort and can be
painful14 15 34
and that a 2-J defibrillation energy level may be inadequate for a
successful cardioversion. If cardioversion efficacy could be increased
at lower energy levels, patient acceptance of this therapy may
grow. In the present study, there was a marked increase in
cardioversion efficacy when the shocks were timed to high levels of AF
organization.
Limitations
This study was performed in canine hearts; it is not
known if human hearts would respond in the same fashion. It is also not
known if the observations reported would be the same for chronic AF.
Because of the difficulty in accessing the coronary sinus in a
closed-chest procedure in canine, a right atriumleft atrium
defibrillation vector was chosen instead of the right
atriumcoronary sinus vector used in human patients.
QRS detection and subtraction may become invalid during intermittent
bundle-branch block. Finally, we acknowledge that multiple factors,
known and unknown, probably contribute to the success or failure of
atrial defibrillation. An OI>0.5 measured in the present study is
associated with defibrillation efficacy, but causality has not been
established.
Conclusions
The frequency domain analysis of an
intra-atrial AF electrogram is an indicator of AF organization. From
this analysis, a novel, hightemporal resolution algorithm
termed the organization index was developed to quantify AF
organization. AF organization is highly variable over time. Time
periods with high OIs may correlate with increased AF organization and
a smaller number of wavelets. Atrial defibrillation shocks delivered
during periods with high OIs correlated with improved defibrillation
efficacy.
| Acknowledgments |
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Received November 20, 2000; revision received February 8, 2001; accepted February 15, 2001.
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