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X-ray diffraction pattern of the basic sample Ni0.65Zn0.35Fe2O4 is shown in Fig. 1a.
➢The τ 2/τ b ratio diminishes during doping of the basic sample, which indicates different nature of volume defects.
The characteristic d-spacings of the basic sample are in good agreement with values reported in standard JCPDS cards.
The experimentally observed lattice constant (8.3738 Å) of the basic sample is in agreement with the reported value (8.382 Å) of the same composition [15].
The saturation magnetization (74.1 emu/g) and Curie temperature (382 °C) of the basic sample are well in agreement with the reported values [17].
Other socio-demographic details of the basic sample, including those participants who had not completed the questionnaire, have been reported elsewhere [ 23].
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On the basis of the taken measurements of positron lifetimes, τ 1 and τ 2 are slightly different, within the margin of errors, for the basic samples and for the doped samples.
In order to validate the previously attained results of the basic samples more complex parts for accurately defined applications have to be investigated.
The said delay is considered as a fraction of the basic sampling period and it is modeled by including a discrete time version of a unit-amplitude pure phase shift network in one of the arms of the tan-lock phase detector (PD).
We defined a population of approximately 1000 individuals as the basic sample unit (BSU) and a total of 108 BSU were included.
The coverage rate was 62.3%, resulting in the basic sample of N = 2,473 participants.
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