zonde said:
Haven't you changed signature of spacetime from (-,+,+,+) to (+,+,+,+) in your transformation?
The problem is that if you use the (-,+,+,+) spacetime signature to determine the distance of a null interval, you get zero.
There is a bit more discussion in Mentz114's
earlier copy of the proof, in Post #52 of this thread.
You will see somewhere in the first couple of paragraphs a mention of a constant of proportionality k, relating Δx and ΔL and \sqrt{\Delta x^2 + \Delta t ^2}.
If you use the (+,+,+,+) spacetime signature to determine the distance of a null interval you get an observer dependent quantity which is
proportional to the spatial distance, Δx, between the two events.
So he has defined ΔL to be a quantity which is
proportional to the spatial distance, rather than
exactly the spatial distance.
Since in the end, we are simply looking for whether or not ΔL/λ is an invariant, the extra constant factor does not make a difference, so long as that factor is also invariant. Since that factor is only a function of c, which is invariant, it does indeed work.
Now referring back to Mentz114's earlier proof, you will see he mentions a parameter k. Feel free to check my math, but I believe it can be calculated as follows. (And if something doesn't make sense, ask for more explicit definitions of the variables!)
\begin{align*}<br />
\Delta x &= \Delta L \\ <br />
\Delta t &= \frac{\Delta L}{ c}\\ <br />
\Delta x^2+\Delta t^2 &=\left ( 1+\frac{1}{c^2} \right )\Delta L^2\\<br />
k \left ( \Delta x^2+\Delta t^2 \right )&=\Delta L^2\\<br />
\therefore k&=\frac{c^2}{c^2+1}<br />
\end{align*}
In Mentz114's later proof, he changes the definition of ΔL, so it is no longer equal to Δx, but just proportional to it, although I'm not sure he makes this entirely clear.