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Correction for simulated temperatures.
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We explored the phase diagram for a range of simulated temperatures and global fields, studying the competition between the antiferromagnetic couplings and the polarizing field.
The experimental results are summarized as follows: the diagonal elements of the density matrix corresponding to the CETS are determined by measuring the set of diagonal Pauli operators (equation (5)) for a range of simulated temperatures and external fields.
Figure 5 shows the results of simulated temperatures and temperature excess values (the difference of simulated temperatures and the normal subsurface temperatures) along a vertical profile at the middle part of the simulated region for the same model as in Figure 4 (M55; Table 2).
This estimation is performed for Sn 10% Pb alloy in the metallic mold, using conjugate gradient method (CGM), based on the noisy simulated temperatures for the constant and temperature-dependent thermo-physical properties.
The projected temperature changes are always presented as simulated changes relative to the simulated temperatures of the individual models for the baseline period 1961 1990.
These results are consistent with those recently simulated by Verma and Gómez-Arias (2013b) for the LHGF and LPGF. Figure 6 Simulated temperatures at three locations (L1, L2, and L3).
The simulated temperatures agreed well with the experimental data.
Simulated temperatures at all depths successfully approximated the measured data.
For example, a drop in the thermal conductivity of sediments with increasing temperature could result in greater simulated temperatures at depth.
Simulated temperatures.
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