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Thesis - Instituto de Telecomunicações

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72 CHAPTER 4. SIGNAL PROCESSING AND FEATURE EXTRACTIONthat will be used in the <strong>de</strong>finition of the following EDA mo<strong>de</strong>ls.Equation 4.21 constitutes the base mo<strong>de</strong>l of an isolated SCR event, presenting 4 parameters:the rise time t r , the <strong>de</strong>cay time, t d , a gain g and the onset time, t o .The total EDA is mo<strong>de</strong>led by adding to the previous SCR, the skin conductance level(SCL), mo<strong>de</strong>led by a constant and a negative exponential (representing signal <strong>de</strong>cay), leadingto the function f m :f m (t) =a exp(−t/t d )+f s (t)+c. (4.23)The situation of two overlapping SCR events is mo<strong>de</strong>led by an 8-parameter function f g ,<strong>de</strong>fined byf g (t) =a exp(−t/t d )+f s1 (t)+f s2 (t)+c. (4.24)In this final mo<strong>de</strong>l, it is assumed that all SCR events share the same <strong>de</strong>cay (t d ), and risetime (t r ) parameter values. Two events will differ in the values taken for the amplitu<strong>de</strong>(gains g 1 and g 2 ) and onset time (t o1 and t o2 ) parameters. The distinctive Skin ConductanceLevel (SCL) mo<strong>de</strong>l parameters are a constant level (c), and a gain (a) affecting a <strong>de</strong>cayingexponential, since the associated <strong>de</strong>cay parameter t d is also assumed to be the same of theSCR events.Using the complete mo<strong>de</strong>l in equation 4.24, the <strong>de</strong>tection and quantification of pairs ofoverlapping events is accomplished by means of an optimization process that fit the mo<strong>de</strong>lparameters to the observed data. The fragility of this mo<strong>de</strong>l is in the selection of the initialparameters for the optimization procedure. It has been shown to be very difficult to provi<strong>de</strong>a good initial approximation that guarantees the convergence of the optimization process[6]. The mo<strong>de</strong>l also lacks an extensive validation. While the base single event mo<strong>de</strong>l inequation 4.23 was tested in 60 SCR segments, the authors stated [146] that the completemo<strong>de</strong>l was only fitted to three double SCR responses.This proposal showed a method to solve the overlapping of SCR events, but the intrinsicproblems of the optimization task were not completely solved. Parameter initializationproved to be crucial to the success in obtaining a good fit of the mo<strong>de</strong>l, an issue notdiscussed in the work in [146].Bi-exponential Mo<strong>de</strong>l Also motivated by the short interstimulus-interval that provokesoverlapping skin conductance responses, Alexan<strong>de</strong>r et al. [6] proposed a bi-exponential

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