You may also approach this starting from an emitter follower configuration.
Ignoring small current to Q1’s base, all input current must go through Q2 and R1. This means voltage across R1 reflects input current. The base-emitter junction of Q2 offsets that by about +600 mV.
The right part, if seen as an emitter follower, outputs the same voltage, reduced by Q1’s base-emitter drop of -600 mV, on R2. If voltage on R2 is the same as on R1 and they’re the same value, by Ohm’s law the current on them must also be equal. And since that current on R2 is mostly drawn from Q2’s collector, Q2 pulls the same current as Q1 is fed.
This isn’t true, because components are mismatched. So they’re not going to be identical. However, an emitter follower configuration is highly resistant to variation in transitor’s amplification and base-emitter drop. Much, much more than the original configuration, which depends on both transistors having identical behavior. Since the emitter resistors can’t be too big, this is goign to be a very imperfect emitter follower, but in principle the benefits are still there.