Proper time between two events in a timelike separation i just began to study special relavity, and i'd like to know if i made some mistake in one of the questions of the book i solved. the question is:

If we have to events A and B with timelike separation, show that the proper time
$${\Delta}{\tau}=\int_{A}^{B}d{\tau}$$ is maximum when calculated along a straight line

Here's what i did: first, consider a reference frame where the moving particle is at rest spatially and put the point A at the origin and B at some point B=(t,0,0,0). I know that ${\tau}=t/\gamma$. therefore, by integrating i got that $${\Delta}{\tau}=\frac{{\Delta}t}{\gamma}$$ but $\gamma \geq 1 $ therefore ${\Delta}t \geq {\Delta}{\tau}$. So i concluded that ${\Delta}{\tau}$ is maximum when it's equal to ${\Delta}{t}$ which is, $\gamma=1$. Formally, ${\Delta}t/\gamma$ is a straight line with inclination $1/\gamma$. Is my approach correct? sorry if it's kinda trivial once it's well a known fact in SR. thanks in advance for your help
 A: Here is what i read in classical field theory by Landau, i quote:
The time interval read by a clock is equal to the integral
$\frac{1}{c}\int_{a}^{b}ds$
taken along the world line of the clock. If the clock is at rest then its world line is clearly a line parallel to the $t$ axis; if the clock carries out a nonuniform motion in a closed path and returns to its starting point, then its world line will be a curve passing through the two points, on the straight world line of a clock at rest, corresponding to the beginning and end of the motion. On the other hand, we saw that the clock at rest always indicates a greater time interval than the moving one. Thus we arrive at the result that the integral
$\int_{a}^{b}ds$
taken between a given pair of world points, has its maximum value if it is taken along the
straight world line joining these two points.
A: No, your approach doesn't make sense. Given A is at the origin and B is on the $t$ axis, the straight-line distance between them is $Δτ = Δt$. There's no gamma factor. If you computed straight-line distance in an arbitrary reference frame then you would have $Δτ = Δt'/γ$. But this is simply because $Δt' = γΔt$. You're just computing the same thing (straight-line distance) in different coordinates.
To show that the straight-line distance is maximal over all paths, you need to integrate over all paths. Define a path as a differentiable function $\mathbf x(t)$ with $|\mathbf x'(t)| < c$. Then calculate the length of that path using the spacetime metric, and show that it's maximized when $\mathbf x'(t)$ is constant. You can use any coordinate system since they're equivalent, but it'll be easiest to use the coordinates where A is at the origin and B is on the $t$ axis (in which $\mathbf x'(t)$ is identically zero if it's constant).
