Homework Statement
Derive a microscopic version of the continuity equation given
\rho(\vec{r},t) = \sum_{i=1}^N \delta(\vec{r}-\vec{q}_i(t))
and \rho is dynamic variablesHomework Equations
I wonder if someone can point out the difference (in general) between the macroscopic and microscopic...
Hi,
Thank for your help. I agree.
So I tried
\int_0^{2\pi}\int_0^{\pi} e^{-\beta \mu \epsilon \cos\Phi}sin\Theta d\Theta d\Phi
but still gets the Bessel function.
Is my limit of integration wrong?
Should it be
\int_0^{2\pi}\int_0^{\pi}\int_0^\infty e^{-\beta \mu \epsilon \cos\Phi} r^2...
Hi,
So my attempt was to compute q = \int_0^{2\pi} e^{-\beta U} d\Theta
But this gives me the Bessel function, so I am not sure if I am on the right track.
Homework Statement
Given the perfect gas molecules with permanent electrical dipole moment u in the field \epsilon.
The potential energy is U = -u\epsilon\cos\Theta
Derive the additional effect of \epsilon on the heat capacity.
I need some hints, please help. Thanks.
Homework Statement
So the question is I have to use some trial function of the form \sum c_if_i to approximate the energy of hydrogen atom where f_i=e^{-ar} for some number a (positive real number). Note that r is in atomic unit.
Homework Equations
Because r is in atomic unit, I think I should...
So all I try to do was to show that the coherent state has minimum uncertainty equally distributed between x and p. And the hint given was to show that \Delta x |\alpha> = x\Delta p |\alpha>, and thus it makes me think that I should treat \Delta x and \Delta p as operators rather than numbers.
Oh my question was how can you come up with such transformation; that is finding a U that satisfies U\sigma^3U^{-1}=\sigma_1 instead of a U that satisfies U\sigma^3=\sigma_1
Thanks,
Hi,
How can I write \Delta x and \Delta p as operators? I want to show that \Delta x|\alpha> = c\Delta p|\alpha> where |\alpha> is coherent state.
I feel like I have to write x and p in terms of annihilation operators, but I always think that \Delta x and \Delta p are numbers, not operators...
Thank you,
Ya I am out of my misery. A tiny bit of problem was you wrote [a, a^\dagger]=\hbar
which should be 1. But generally I get what you are talking about. Thanks.
Yes I think I get that from the previous post.
So the coherent state |\alpha> = ce^{\alpha a^\dagger} |0> .
Now I want to show that the normalized constant c is e^{-\frac{\alpha^2}{2}}
So I do the dot product
<\alpha|\alpha> = c^2 e^{a \bar{\alpha}}e^{\alpha a^\dagger}
We consider
e^{a...
Thank you for helping. I was careless when typing my last post. I read through wiki about BCH but only the last part of the page mentioned about annihilation operators, but then the explanation is not quite clear. So in short, is there a formula to find <\alpha| if knowing that |\alpha> =...