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Consequently, the value c (V, V 1, V 2) is computed correctly.
We argue that the maximum weight of an orientation of (T w v, P w v ) orienting the edges on path T (v, w) towards w equals (4) A (v, w ) + ∑ i = 1 ℓ max S (u i, w ), S (v, u i ) - A (v, w ), and, hence, S v, w) is computed correctly.
For the correctness, we argue that for v, w ∈ V with v ≺ w and for a coloring c w ∈ C w that is feasible for case (1), the maximum weight of an orientation of (T w v, P w v ) consistent with c w that orients the edges on path T (v, w) from v to w is A (v, w ) + W LCA (w, c w ) + ∑ i = 1 ℓ M (u i, v, w, c w ), and, hence, S v, w, c w) is computed correctly.
Similar(57)
The gain factors can consequently not be computed correctly from and.
Otherwise, the gain factors cannot be computed correctly (cf. Protocol B1).
Especially, it is discussed how first and second order derivatives can be computed correctly using cubic or trigonometric splines by a double filtering approach giving filters of length 7.
If this is not suitable, the cardinalities can also be computed correctly by flagging to the PPCF application that submissions of all c k splits should be treated as one submission.
However, connections made with distant neighbors are penalized by an attenuation factor α, which should strictly be less than the inverse largest eigenvalue of the adjacency matrix in order for the Katz centrality to be computed correctly.
In the previous section, we have seen that the gain factors can only be computed correctly from channel estimates obtained with protocols B1 or B2 if the relays are phase synchronous.
(2) Need for global phase reference: it turns out that for two of the protocols, the gain factors can only be computed correctly if the relays possess a global phase reference. .
Finally, the crosshead was weighed between each experiment so the corresponding energy and force values would be computed correctly.
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