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Thus the positive solution ( u, v ) of (4.1) is stable.
In fact, every solution ( u, v ) of ( P ¯ ) satisfies ≤ ( u, v ) ≤ on [ 0, 1 ].
In this section, we analyze the stability of positive steady states ( u , v of (1.2).
So the weak solution ( u, v ) of (1.1 - 1.4 1.1 - 1.4rmly bounded.
Then, the solution (u, v) of (1.1) blows up in finite time.
If (C_0=0), then the solution ((u,, v)) of system (1.1) blows-up in finite time.
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This means that kernel CCA finds the directions a and b that maximize the correlation E [ u v ] of corresponding projections subject to E [ u 2 ] = 1 and E [ v 2 ] = 1.
For a preliminary core C with den(C) < T d, the edge clustering coefficient ECC u, v) <span class="lh">of each edge (u, v) connecting the seed vertex v and a rest vertex u is calculated.
For every unordered pair { u, v} of adjacent nodes u and v, we set the distance variable x uvk to 1 if k is less than or equal to the Manhattan distance of u and v.
If (pq<1), then there exists exactly one solution ((u,v)) of (1.6) such that u and v are positive. .
If (pq<1), then there exists exactly one solution ((u,v)) of (1.6) such that u and v are positive.
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