We can do away with the notion of colliding atoms and think of the high energy experimental conditions as being conducive to the formation of small particles,
In the top most diagram, a small particle passes through a big particle with energy transitions −E1→n and En→2 occurring, on entering the big particle and on leaving the big particle. Both emission and absorption of energy occur in the same process. The overall change in energy state is,
ΔE1→2=En→2−E1→n
but −E1→n is energy emission and En→2 is energy absorption.
In the middle diagram, the small particle coalesce with the big particle and the lowest energy level attained is,
n=nlarge+n1
and the resulting bigger particle subsequently breaks into n−n2 and n2 particles where n2≠n1. This differ from the toppest case where n≠nlarge+n1 but simply n>n1. The small particle passing through the big particle retains its distinctiveness because of its high momentum. These two diagrams provide two scenarios as to what happened to the small particle inside the big particle. In both cases a subsequent departure follows coalescence.
The third diagram shows a simple coalescence without a subsequent separation. Only one singular energy emission occurs as n1→nlarge+1.
All three process occur simultaneously. Emissions form the colored background against which dark absorption lines show up in contrast.
Have a nice day.
Note: This discussion is of all n1, not just n1=1. The case of n1=1 generates an absorption series given the two processes involved; changing aψ and changing orbital energy level as according to Bohr model.