OK, let’s be precise: the probability of the particle being observed in any interval is proportional to the length of that interval.
But all gases consist of moving particles. “Internal thermal equilibrium” simply means no heat flows between any two subsystems. If the temperature of two subsystems is unequal, then the entire system is still out of thermal equilibrium.
And, of course, a system at thermal equilibrium will experience microscopic fluctuations as usual. It is incorrect to say it is not at equilibrium; “equilibrium” does not mean “no motion”.
What is your reasoning that leads you to believe it does not? How exactly do you propose to define temperature of a system not at thermal equilibrium? Don’t say, “use a thermometer,” because one side might be hot and the other cold. And the microscopic definition assumes equilibrium as well.
Look, I honestly think you should carefully work through all the exercises on that web page (or any similar text). You can’t help but encounter all these definitions and concepts.