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Showing posts with the label fact

Translation operator. Central potentials

PROFESSOR: The fact is that angular momentum is an observable, and as such it deserves attention. There is an active way of thinking of observables, and we have not developed it that much in this course. But for example, with a momentum operator you've learned that the momentum operator can give you the differential operator. It's a derivative, and derivatives tell you how to move, how a function varies. So with the momentum operator, for example, you have the momentum operator p hat, which is h bar over i d dx. And you could ask the question of, OK, so the momentum operator moves or takes a derivative, does the momentum operator move a function? Does it generate a translation? And the answer is, yes. That's another way of thinking of the momentum operator as a generator of translations. But how does it do it? This is a Hermitian operator, and it takes a derivative. It doesn't translate the function. But there is a universal trick that if you exponentiate ...

Lec 27 MIT 18.03 Differential Equations, Spring 2006

As a matter of fact, it plots them very accurately. But it is something you also need to learn to do yourself, as you will see when we study nonlinear equations. It is a skill. And since a couple of important mathematical ideas are involved in it, I think it is a very good thing to spend just a little time on, one lecture in fact, plus a little more on the problem set that I will give out. The last problem set that I will give out on Friday. I thought it might be a little more fun to, again, have a simple-minded model. No romance this time. We are going to have a little model of war, but I have made it sort of sublimated war. Let's take as the system, I am going to let two of those be parameters, you know, be variable, in other words. And the other two I will keep fixed, so that you can concentrate on them better. I will take a and d to be negative 1 and negative 3. And the other ones we will leave open, so let's call this one b times y, and this other one will be...