Comparing the results of OAWCF for field sizes of 15 × 15 and 10 × 10 cm2 (Figures 2 and 3) with CFf.s for a 15 × 15-cm2 field size (Figure 4) under 6-MV photon irradiation, it can be deduced that an OAWCF at a non-reference field size is approximated by multiplying the given correction factor at a reference field size by the corresponding correction factor at a non-reference field size.
By multiplying the compaction correction degree parameters in the map by the thicknesses in the depth domain, a plan map of compaction recovered thicknesses eventually can be obtained.
p values were corrected using Boneferroni's correction by multiplying the p values with the number of alleles tested for the locus.
Probabilities were calculated using Fisher's exact test and corrected for multiple comparisons using the Bonferroni correction, by multiplying the uncorrected p value by the number of alleles tested (12 for DRB1, 6 for DQA1, 5 for DQB1).
P-values were adjusted for multiple testing using Bonferroni correction by multiplying the nominal p-values with 12, which is the total amount of tests used in this study.
One solution to this is to apply the Bonferroni correction by multiplying the ' P' value by the number of comparisons.
As a SPECT, PET, CT or MRT scan allow the measurement of organ volumes and therefore masses, several studies have assumed uniform distribution of activity and applied a first-order correction by multiplying the activity concentration by the phantom organ weight, resulting in normalized time activity curves and residence times.
The simulated "non-normalized" data is generated by multiplying the given values after natural isotope correction by random factors.
To correct for multiple testing, Bonferroni correction was applied by multiplying the obtained p value from the Mann–Whitney U test by the numbers of comparisons (i.e. two) that were carried out.
For this process, the instrumental correction was performed by multiplying the amplitudes with a coefficient to approximate to synthetic waveforms.
