- #1
ognik
- 643
- 2
The text states:
"Let us consider a wave packet whose Fourier inverse $\phi (\vec{k})$ is appreciably different from zero only in a limited range $\Delta \vec{k}$ near the mean wave vector $\hbar \vec{\bar{k}} $. In coordinate space, the wave packet $\psi(\vec{r}, t)$ must move approximately like a classical free particle with mean momentum $\hbar \vec{\bar{k}}$. To see this behavior we expand $\omega (\vec{k})$ about $\vec{\bar{k}}$:
$ \omega (\vec{k}) = \omega(\vec{\bar{k}}) + (\vec{k} - \vec{\bar{k}}) \cdot (\vec{\nabla_k} \omega)_{k= \vec{\bar{k}}} + ...$
$=\bar{\omega} + (\vec{k} - \vec{\bar{k}})\cdot \vec{\nabla_{\bar{k}}} \bar{\omega} +... $ with obvious abbreviations"
I'm afriad not much of the above is obvious to me ...please help me understand -
What is $ \omega (\vec{k})$?
What expansion are they using?
What are the abbreviations?
"Let us consider a wave packet whose Fourier inverse $\phi (\vec{k})$ is appreciably different from zero only in a limited range $\Delta \vec{k}$ near the mean wave vector $\hbar \vec{\bar{k}} $. In coordinate space, the wave packet $\psi(\vec{r}, t)$ must move approximately like a classical free particle with mean momentum $\hbar \vec{\bar{k}}$. To see this behavior we expand $\omega (\vec{k})$ about $\vec{\bar{k}}$:
$ \omega (\vec{k}) = \omega(\vec{\bar{k}}) + (\vec{k} - \vec{\bar{k}}) \cdot (\vec{\nabla_k} \omega)_{k= \vec{\bar{k}}} + ...$
$=\bar{\omega} + (\vec{k} - \vec{\bar{k}})\cdot \vec{\nabla_{\bar{k}}} \bar{\omega} +... $ with obvious abbreviations"
I'm afriad not much of the above is obvious to me ...please help me understand -
What is $ \omega (\vec{k})$?
What expansion are they using?
What are the abbreviations?