First off, your system only depends on the combined value $p=\frac{\delta}{n}$.
Next, notice your control equation is about as simple as it gets: linear first order homogenous, doesn't even depend on $s$. Its solution is outright just
$$c(t)=c(0)e^{pt}$$
without trying.
To get the full solution, as a system of ODEs it's also extremely simple:
$$\underbrace{\begin{bmatrix}c\\s\end{bmatrix}^{'}}_{\vec{x}}=\underbrace{\begin{bmatrix}p&0\\-1&p\end{bmatrix}}_{A}\begin{bmatrix}c\\s\end{bmatrix}$$
with therefore
$$\vec{x}(t)=e^{At}\vec{x}(0)$$
where
$$e^{At}=\begin{bmatrix}e^{pt}&0\\-te^{pt}&e^{pt}\end{bmatrix}$$
from the matrix exponential.
Back to the phase diagram: you were looking at $\frac{dc}{dt}=0$, which is so simple you're just not believing the solution:
$$\frac{dc}{dt}=pc=0\quad\Rightarrow\quad c=0$$
Now you have your two special lines: along the line $c=0$ is vertical vectors (the horizontal component is zero), and $s=c/p$ has horizontal vectors.
You would also need to find stationary points (make both zero, that's the origin only), and any special lines that stay solutions (none, officially set $c=ms$ and solve $c'=ms'$ for some $m$).
Next, your two lines (in general, arbitrary curves) divide the space into 4 quadrants. In each quadrant (in general, arbitrary sectors of space), you get a particular combination of signs of derivatives, so $c>0,s<c/p$ means horizontally to the right and vertically downwards as an arrow.
Plotting the entire thing in Wolfram results in this graph (using $y\mapsto s,x\mapsto c,p=0.5$)