Well, it was for quite a long time that indeed many writings on the Bohr Einstein debate judged that Bohr "won the debate". Only for some years people are more careful about it and appreciate Einstein's profound insights on the interpretation of quantum mechanics more, though you have a hard time as a follower of the statistical minimal interpretation (which I think indeed comes the closest to Einstein's point of view), as one sees in this forum.
The reason is a bit puzzling for me since I never understood the hype about Bohr's writings. To be honest, I'm not able to understand most of Bohr's writings very well, because they are pretty unclear, because they don't contain enough math to unambigously express what Bohr really wants to say. The same holds for Heisenberg.
For a long time the "Copenhagen doctrine" (though it never was a clearly defined concept, because there are many flavors of the Copenhagen interpretation with different meanings of only vaguely defined notions, particularly the "collapse of the state").
It think the change of mind came slowly with Bell's theoretical work on the question how to decide between Einstein's claim that quantum theory is incomplete and Bohr's claim that it is complete.
I think for Einstein QT is incomplete in the sense that there should be local hidden-variable theories to resolve the problem that on the one hand QT only describes the statistical behavior of measurements on ensembles of equally prepared quantum systems but that on the other hand the preparation in the quantum state has to refer to each single system within such an ensemble. There's no problem if you consider the quantum state (statistical operator) just as a way to mathematically describe the preparation of a single system, implying only the usual probabilistic meaning via Born's rule (in its general form for general as well mixed as pure states). Some people consider such an epistemic view as incomplete and want an ontological description, i.e., they want to say "an electron IS one-to-one mapped to some mathematical entity in the theory", as is the electromagnetic field in classical electrodynamics. I think that also explains, why Einstein tried to find a unified classical field theory for the about last 30 years of his life.
The breakthrough was that Bell, with deriving his famous inequalities valid for all local determinstic hidden-variable theories, found a physically testable prediction, i.e., he brought a rather vague philosophical question, which was not well defined to decide by experiments, to a sharply defined physical question, which can be (and today in fact is) answered by experiment.
At the time it was a risk to work on the foundations of QT and questioning the Copenhagen doctrine. A somewhat sad illustrative story related to this is the history of Everett's thesis (now known as the many-worlds interpretation). Fortunately courageous experimentalists like Aspect took up the challenge to experimentally realize the first Bell-test experiments, and the breakthrough was that indeed Bohr was right in the sense that there are at least no local deterministic hidden-variable theories that can explain the outcome of the Bell-test experiments, namely that Bell's inequality is violated and with an amazing significance precisely as predicted by quantum theory.
I'm aware that I should give references for this. I have only two books in mind, but there's for sure tons of papers on this historical subject out there, but I'm not a librarian. So here are my two references (though more in the popular-science end of the spectrum):
https://www.amazon.com/dp/1491531045/?tag=pfamazon01-20
https://www.hippiessavedphysics.com/