A volume, V, of gas, weighs W = rho g V; where rho is the mass density, g is g.
The density of cold air is Rho > rho for the same gas when it's hot. That results because hot air molecules have more kinetic energy and zing about randomly over longer rms tracks. That is, hot air molecules are not packed in so tight as the cold molecules because they need more room to move around in.
So a given volume V of cold air weighs W = Rho g V > rho g V = w and clearly W > w in this case. The cold air is heavier than the hot air.
The hot air floats atop the cold air because it is indeed lighter than a comparable volume of cold air. Conversely, the cold air sinks below the hot air because it is heavier.
I'm puzzled by the leap from air to black holes. The physics and natural laws governing the two are totally different. And I think you need to study up on BH because you have some misconceptions.
First, BHs are not black because they are cold. In fact, the temperatures inside a massive BH can approach the trillions of degrees K that were once commonplace during the big bang. But they are black, from the outside, because all that radiant energy is trapped by the immense gravity and none escapes to be seen.
Second, as someone else has pointed out, there is no up or down for the typical natural BH. They are in deep space, where up and down have no meaning as there is no common reference point to use.
Sorry, your attempt to attribute the force of a gravity field to the degree of coldness will receive an icy reception in the physics domain I'm afraid.