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Cd-Hmm For Normal Sinus Rhythm<br />

1<br />

0 t<br />

<br />

1<br />

2<br />

H (t ) 1<br />

1 t 1 (2)<br />

2<br />

0 others ,<br />

Fig. 1: Continuous wavelet transform of the raw time data series (left panel – premature ventricular<br />

contraction, right panel – normal sinus rhythm).<br />

Scales were finally chosen from an interval of . The signals were extracted as periods of 250<br />

samples (f s =360 Hz) containing R-waves of each QRS complex. After transforming by CWT, the wavelet<br />

coefficients were squared and normalized.<br />

2.2 Continuous Density Hidden Markov Model (Cd-Hmm)<br />

The Hidden Markov model is a finite state machine having a set of states Q, each of which is associated<br />

with probability distribution, an output alphabet O, transition probabilities A, output probabilities B, and initial<br />

state probabilities Π. The current state is not observable. Instead, each state produces an output with a certain<br />

probability B. The CD-HMM stage is proceeded by the pre-processing step (CWT).<br />

Continuous emission probability B = {b j (O t )}, where O = O 1 ,O 2 , . . . ,O T , the emission probability density<br />

function of each state is defined by a finite multivariate Gaussian mixture:<br />

M<br />

b j (O t ) ∑d jm N (O t , jm , C jm ), 1 j N (3)<br />

M1<br />

where O t is the feature vector of the sequence being modelled, d jm is the mixture coefficient from the mth<br />

mixture in state j and N is a Gaussian probability with mean vector µ jm and covariance matrix C jm for the mth<br />

mixture component in state j. We will refer to these models as a continuous density HMM (CD-HMM).<br />

The used CD-HMM had left-to-right topology. The number of states is possible to change. The first state<br />

is designated as the initial state and the last state as the output state.<br />

www.<strong>ijcer</strong>online.com ||May ||2013|| Page 120

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