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Notably, this implies that the frequently observed inter-study variability of the AIF during the early (bolus passage) phase has essentially no influence since it does not contribute much to the integral up to T (see Figure 1).
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For higher field integrals up to J= 1Tm this homogeneity is not sufficient and additional correction elements that realise certain radial current distributions in the beam cross section are required.
The systemic approach uses a transfer model that is based on computing the convolution integral of up to several signals, e.g., efficient rainfall, pumping, to simulate flow rates and groundwater levels in both the karst conduit and the carbonate matrix at the aquifer outlet and in several parts of the catchment area.
Analysis of Gaussian likelihood functions indicates that 25 active points is sufficient to compute the evidence integral in up to 30 dimensions.
A more straightforward method is to use the Gaussian approximation that depends only on integrals involving up to two eigenvalue densities.
The Cauchy Fantappié integrals constructed up to that point may however lack the basic requirement of producing holomorphic functions, whatever the given data is.
This gap at temperature 0 K is further enhanced to d 2 = 0.181 for the same critical Coulomb energy u c = 1.7 and for hopping integrals taken up to third nearest neighbours.
Grid verification study shows mostly monotonic convergence with averaged grid uncertainty <5% for integral quantities and up to 10% for local variables.
Integral yields of up to 177.3 MBq/μAh and 81.6 MBq/μAh for natEu d,x 147,149Gd reactions and up to 43.3 MBq/μAh and 61.8 MBq/μAh for natEu p,x 147,149Gd reactions, respectively, were calculated.
As in the work reported in ref (37), we define the w(r) to be zero in the bulk (i.e., at rM = 4.90 nm), such that the constant C in the equation above can be expressed as Substituting eqs 2 and 3 into eq 1, we derive the following equation: where the integral is extended up to the maximum distance rD allowed for dimeric states.
Integrals of products up to the fifth order are derived in a unified manner for the three fundamental shapes in terms of the position vectors of vertices.
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