How Are Wigner D Functions Related to Nuclear Rotor Model Wave Functions?

patric44
Messages
308
Reaction score
40
Homework Statement
Φ = ((2l+1)/8pi^2) D^{j}_{MK}
Relevant Equations
why the nuclear rotor model wave function is written in terms of Wigner D functions?
hi guys
I am recently taking a Nuclear structure course, and have a lot of questions regarding the nuclear rotor model.
in most nuclear physics books the I have, the wave function associated with the rotor model of the nucleus is written in terms of the Wigner D functions , like the expression below
$$
\bra{\theta\;\phi\;\psi}\ket{JMK} = c(D^{J}_{MK}+(-1)^{J}D^{J}_{M-K})
$$
where c is a constant, I am a little bit familiar with the rotation matrix and its representation in the angular momentum basis , isn't the Wigner D functions is just the matrix elements of the rotation matrix in 3d ? , what is the relation between D functions and the eigen functions of the rotor model?
can anyone explain how the formula above is derived, or refer to a good book or a set of lecture notes in theoretical nuclear physics.
thanks in advance.
 
Physics news on Phys.org
can anyone explain what this expression mean
$$
\bra{\psi,\theta,\phi}\ket{IMK} = c D^{I}_{MK}
$$
isn't that the projection of the sate represented by IMK on the basis represented by psi,theta,phi?
why is that interpreted as the matrix elements of the rotation operator?
 
patric44 said:
I am recently taking a Nuclear structure course, and have a lot of questions regarding the nuclear rotor model.
in most nuclear physics books the I have, the wave function associated with the rotor model of the nucleus is written in terms of the Wigner D functions
Just curious, which textbooks are you referring to? ##: )##
 
##|\Psi|^2=\frac{1}{\sqrt{\pi b^2}}\exp(\frac{-(x-x_0)^2}{b^2}).## ##\braket{x}=\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dx\,x\exp(-\frac{(x-x_0)^2}{b^2}).## ##y=x-x_0 \quad x=y+x_0 \quad dy=dx.## The boundaries remain infinite, I believe. ##\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dy(y+x_0)\exp(\frac{-y^2}{b^2}).## ##\frac{2}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,y\exp(\frac{-y^2}{b^2})+\frac{2x_0}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,\exp(-\frac{y^2}{b^2}).## I then resolved the two...
It's given a gas of particles all identical which has T fixed and spin S. Let's ##g(\epsilon)## the density of orbital states and ##g(\epsilon) = g_0## for ##\forall \epsilon \in [\epsilon_0, \epsilon_1]##, zero otherwise. How to compute the number of accessible quantum states of one particle? This is my attempt, and I suspect that is not good. Let S=0 and then bosons in a system. Simply, if we have the density of orbitals we have to integrate ##g(\epsilon)## and we have...
Back
Top