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In addition, there exists an important discrepancy between the projected and non-projected states.
Indeed, the overlap between the projected and non-projected wavefunctions is of the order of 0.22 for the even-even systems and 0.19 for the odd ones.
Indeed, the overlap between the projected and non-projected wavefunctions is of the order of 0.22 for the even even systems and of 0.19 for the odd ones.
We reported in Table9 (respectively Table10) the values of the relative discrepancy δ E between the projected and non-projected energies, as a function of (N-Z), for Z = 6 and Z = 8 when G np = 0.75 G pp (respectively when G np = 1.5 G pp ) in order to illustrate the region G np < (G np ) c (respectively G np > (G np ) c ).
We reported in Table 9 (respectively, Table 10) the values of the relative discrepancy δE between the projected and non-projected energies, as a function of (N − Z), for Z = 6 and Z = 8 when G np = 0.75 G pp (respectively, when G np = 1.5 G pp ) to illustrate the region G n p < G n p c (respectively, G n p > G n p c ).
In the second approach, we directly optimise the null space projection matrix by minimising the difference between the projected and the desired vector of the secondary task increment.
The results show excellent agreement between the projected and measured values.
We investigated relationships between the projected shelf seas changes across the ensemble and changes in the large-scale climate forcing.
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