Infrared said:
By "increase/decrease without bound" do you mean ##\lim_{x\to\infty}|f(x)|=\infty## or just ##\lim\sup_{x\to\infty}|f(x)|=\infty##? What does "oscillate" mean?
Okay, well I mean the first, that ##\lim_{x\to\infty} |f(x)| = \infty##. From the way ##f_n## is constructed, we see that its convergence depends on the behavior of ##f## at infinity, and that ##g(x)## is precisely asymptotic form of ##f## at infinity.
So what I meant is, that if we have no limit, that means that either limit is in positive/negative infinity(that's what I meant by increase/decrease without bound), or the number of accumulation points is not equal to one(there's no unique pointt to which the sequence converges for fixed ##x##, violating pointwise convergence, and hence uniform convergence as well).
Infrared said:
I agree with this (and probably you also mean to allow functions which are eventually periodic).
I indeed do allow that case(in which a function eventually turns to behaving periodic), I commented on it later in the answer, when I obtain the general form of ##f##.
Infrared said:
I can't figure out what mathematical claim you are making here. Can you make this precise?
What I mean is that behavior of ##f_n##, the way its limit approaches as ##n\to\infty##, is the same way ##f## behaves as ##x\to\infty##, unless we make the sequence independent of ##n##. This is a consequence of how we constructed ##f_n## as just being a translation along ##x##-axis. So we choose that either ##f## has a finite limit, hence the sequence also has a finite limit, which makes it uniformly converge to a constant(which I addressed in the first answer), or ##f## can be periodic with a specific period that would make ##f_n## independent of ##n##. This is the case of periodic function with period ##\frac{1}{k}##. Now, this doesn't exhaust the possible behaviors of ##f##, but it does exhaust possible behaviors of ##f_n## and hence ##g##.
If we, for example, allow ##f## to be periodic with a different period from the form we mentioned, that would make ##f_n## limit undefined, since it would produce more than one accumulation point(which I addressed when I talked about general rational and irrational periods). Even if ##f## is aperiodic, it must be of such behavior that at infinity it becomes a periodic function of period ##\frac{1}{k}##, otherwise ##f_n## wouldn't converge even pointwise.
So that's what I meant, these two cases are two possibilities of how ##f_n## would converge, and from there I give the general form of ##g## which is ##aP(x) + b##. Every ##g## can be written in this general form, since ##P## is a completely general function of period ##\frac{1}{k}##, it just has to be continuous. So I considered specific cases on how ##f_n## converges and then combined them in general way.
From there, I find that then ##f## must be of general form ##s(x)P(x)+t(x)##, where ##s## and ##t## converge towards ##a## and ##b## we find in ##g##, and ##P## is just a periodic function of period ##\frac{1}{k}##, so it doesn't interrupt the convergence of ##f_n##.
All other cases can be broken down to these possibilities, the main thing is that we essentially want ##f_n## to have a well defined limit, and then we take all possible combinations of functions that give that. I think it is precise enough now, unless I missed something that is of essential importance. Also when I mention accumulation points, it is an abuse of words, since in terms of uniform convergence those 'points' are functions, while in terms of pointwise converges they are actually points. But it should be clear from the context what I mean in every particular case.