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5 Results

Our measured Stark FWHM ($W_{\rm m}$) and shift ($d_{\rm m}$) values at various electron temperatures (T) and densities (N) together with other authors data are given in Table 1.


  
Table 1: Measured Stark FWHM ($W_{\rm m}$) and shift ($d_{\rm m}$) values for the OIII spectral lines at observed electron temperatures (T) and densities (N). a, this work; b, Platisa et al. (1975); c, Puric et al. (1988a); d, Puric et al. (1988b) and e, Blagojevic et al. (2000). $W_{\rm m}/W_{\rm th}$represents the ratio between measured and our calculated (SCPF) values taken from Table 2
\begin{table}
\includegraphics[width=18cm,clip]{Table1.eps}\end{table}

Our calculated W and d data at 1023 m-3electron density are given in Table 2 for the mean wavelength $<\lambda >$ in the multiplet. The width and shift of each multiplet component can by easily evaluated if one takes into account that the W and d are proportional to $\lambda^2.$


  
Table 2: Electron Stark FWHM (W in pm) and shift (d in pm) calculated by using the semiclassical perturbation formalism (SCPF) (Eqs. (1)-(3)) at 1023 m-3 electron density and various electron temperatures (T in 104 K). $<\lambda >$ is the mean wavelength (in nm) in the multiplet. Negative shift is toward the blue
\begin{table}
\includegraphics[width=15cm,clip]{Table2.eps}\end{table}


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