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Whenever flow enters an edge, this edge must lie on a currently shortest path towards the respective sink (w.r.t. \(c\)).
(we call such an edge \(vw\) active)
From now on: Only single-sink instances and all flow particles enter the network before time $\theta = 0$
The total volume of all flow particles with maximal distance at most $k$ to $t$ at time $\theta$
${\color{red}v} \in G\setminus T$ the closest node to $t$
and $b' \coloneqq b - 2\sum_{e \in \delta(v,T)}\tau_e \geq a$
Then $T \cup \Set{v}$ is sink-like for $[a,b']$
$\implies t$ has an inflow of $\geq \frac{1}{2}$ for every intervall $[a, a + 2\sum_{e \in E}\tau_e]$. Otherwise the flow terminates.
at least: | at most: | |
for acyclic graphs | $\tPmax + U$ | $\tPmax + U$ |
for general graphs | $\Omega(U \cdot \ln\tG)$ | $\Oc(U \cdot \tG)$ |