One possible approximation is as follows. When τ tends to infinity, the original equation is reduced to
d2dτ2A(τ)+(c+k28τ)A(τ)=0
and the corresponding analytical solution is
A(τ)=C1M(−ik216√c,12,2i√cτ)+C2W(−ik216√c,12,2i√cτ)
where M is the Whittaker M function and W is the Whittaker W function.
Making the change c=−a2 and a=−b we obtain
A(τ)=C1M(k216b,12,2bτ)+C2W(k216b,12,2bτ)
Then for k>0 and b>0, the solution
A(τ)=C1M(k216b,12,2bτ)
gives a exponentially growing solution; and
A(τ)=C2W(k216b,12,2bτ)
gives a exponential decaying solution.