Difference between revisions of "Electric QuadrupoleMoment Forest NuclPhys I"
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As in the dipole calculation we assume that the object is in a state such that its maximum total angular momentum is along the z-axis. | As in the dipole calculation we assume that the object is in a state such that its maximum total angular momentum is along the z-axis. | ||
− | or <math>\psi</math> | + | or <math>\Psi_{jm} = \Psi_{jj}</math> |
+ | |||
+ | |||
+ | then | ||
+ | |||
+ | <math>Q = < \Psi_{jj} |3z^2 - r^2|\Psi_{jj}></math> | ||
+ | |||
+ | From definition of quadrupole moment for a single charged object/particle. | ||
+ | |||
+ | The origin of this comes from electron-statics. | ||
+ | |||
+ | You expand the electric potential in terms of spherical harmonics. | ||
+ | |||
+ | <math>\Phi(\vec{r}) = {\Sigma_{l=0}}^{\infty} {\Sigma_{m=-l}}^{l} \frac{4\pi}{2l + 1} q_{lm} \frac{Y_{lm}(\theta \psi)}{r^{l+1}}</math> | ||
+ | |||
+ | because | ||
+ | |||
[[Forest_NucPhys_I]] | [[Forest_NucPhys_I]] |
Revision as of 04:36, 7 April 2009
Electric Quadrupole Moment of a Nucleus
Pages 104-111
As in the dipole calculation we assume that the object is in a state such that its maximum total angular momentum is along the z-axis.
or
then
From definition of quadrupole moment for a single charged object/particle.
The origin of this comes from electron-statics.
You expand the electric potential in terms of spherical harmonics.
because