Sentence examples for Theoretical intensities from inspiring English sources
Theoretical intensities ( tilde{I}left( {lambda_{text{ul}} } right) ) are calculated for all the nine lines, which are termed as ( tilde{I}_{{{text{cal}}j}} ), using the obtained values of ( tilde{N}_{g} ) and ( tilde{N}_{m2} ) for larger grid points of ( tilde{N}_{e} ) and ( tilde{T}_{e} ).
where I hkl)E° and I(h ' k ' l ')T correspond to experimental and theoretical intensities of a given plane, and I hkl)E and I(h ' k ' l ')T correspond to experimental and theoretical intensities for those families of lattice planes which show a particular change.
After this, the theoretical intensities and accordingly the mismatch parameters with the experimental values are recalculated by repeating the same procedure as explained above while including the effect of opacity in the PEC's and diffusion of neutrals and metastable states to the wall.
Table 4 Theoretical and experimental intensities of the lines of YAB Ce 3+ corresponding to the 4 f → 5 d transitions Peak Ithe (a. u) Iexp (a. u) 1 1.4 1.4 2 0.36 0.38 4 0.46 0.78 6 1.28 1.36 7 1.3 1.3 Iexp, experimental intensity; Ithe, theoretical intensity.
Compared with the theoretical intensity ratio of 0.44 between peak (0 0 2) and (1 0 1) (calculated from JCPDS-34-1451 for a random orientation of the crystallites), these films demonstrate a strong preferred orientation along the c-axis with the (0 0 2) and (1 0 1) peak intensity ratio between 2 and 5, suggesting good crystalline quality of the films.
Open image in new window Fig. 2 Bottom Theoretical intensity distributions of azimuthally polarized A-TEM01* for the mode p = 0 (single-ring), A-TEM11* for the mode p = 1 (double-ring), A-TEM21* for the mode p = 2 (triple-ring).
The F value can be regarded as the theoretical intensity of a single molecule.
In some previous works, several coarse-grained models have been introduced to speed up calculations of theoretical intensity scattering patterns.
We refer to I and I t as the intensity of a peak and theoretical intensity, respectively, which match the corresponding ion from a simulated spectrum.
A nonlinear fit of experimental intensity to the theoretical intensity as a function EOM modulation (eqs 1 and 2) was performed for both polarized laser transmittance and horizontally polarized SHG.
The true FPKM was determined not from the theoretical intensity of the transcripts, but from the actual true number of reads that came from each transcript exonic reads only.
