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Further insights into the emission properties of TCQR may be found by performing state filling experiments.

It is known that the noise subspace can be found by performing eigen-decomposition on ({hat {mathbf {R}}_{text {x}}}); nevertheless, the multiplicity of the noise eigenvalues cannot be accessed.

In addition, the location of extreme, if it is an anomaly, can be found by performing RTM-calculations with the centers of the sampling circles at the nodes of a grid.

This way, the transition probabilities pi,j in (13) for (itilde {R}{le } j{le } itilde {R}) can be found by performing the following operation: The left-hand-side vector in includes all transition probabilities from system state i to states in between (i tilde {R}) and (i tilde {R}).

If the values (gamma _{kpi}^{j}) are known for all frequency and bandwidth configurations, then the (vec {x^{mathrm { opt)}}}) can be found by performing an exhaustive search on the set of samples (left (vec {x}^{j},gamma _{kpi}^{j}right)).

The vertical dimension of can be found by performing autocorrelation over an entire symbol (vertical correlation), where it is assumed that the orientation of subcarriers versus symbols is as depicted in Figure 2. Without taking the effects of delays and CFOs into consideration, we define the absolute value of the vertical correlation as.

Confirmation was found by performing high temperature fretting tests.

The critical value is found by performing a linear stability analysis of the basic reaction regime.

Optimal position of the gun focusing solenoid for low emittance beam generation is found by performing particle tracking simulations.

Selected system parameters, which are found by performing analytical modeling, are tested and analyzed with RELAP5 code and compared with the analytical results.

Once the measurements performed, the fitting parameters (of type JC = f(B, T)) of each strand have been found, by performing regression analysis.