Since y and z aren't involved, let's simplify to just talk about x and t.
Then a Lorentz transformation transforms a pair (x,t) into another pair, (x',t'). We're assuming that ##x' = Ax + Bt## and ##t' = Dx + Et##. Maybe it's clearer if we write them as functions:
##F_{x'}(x,t) = Ax + Bt##
##F_{t'}(x,t) = Dx + Et##
Then we have the assumptions:
Assumption 1: When ##x'=0##, ##x=vt##.
This means that the function ##F_{x'}(x,t)## satisfies ##F_{x'}(vt, t) = 0##. This implies that ##B = -vA##.
Assumption 2: When ##x=0##, ##x'=-vt'##.
This means that the functions ##F_{x'}(x,t)## and ##F_{t'}(x,t)## satisfy:
##F_{x'}(0, t) = -v F_{t'}(0, t)##.
So this implies that ##A\cdot 0 + B t = -v (D \cdot 0 + E t)##. So ##B = -vE##.
So you can conclude that ##E = A## and ##B = -vA##. But you can't conclude that ##D = 0##. To get ##D##, you need another assumption. That's usually the invariance of the speed of light:
Assumption 3: When ##x=ct##, then ##x' = c t'##.
In terms of functions,
##F_{x'}(ct, t) = c F_{t'}(ct, t)##