Chapter 3: The Gaussian Wavepacket
The center of the Gaussian satisfies the classical equations of motion, however the width first, spreads and then contracts periodically in time, twice per period.
where
is the angular frequency of the oscillator) and hence the Gaussian moves without spreading.
The center of the Gaussian satisfies the classical equations of motion. Now the width first contracts and then spreads, twice per period.
Gaussian wavepacket. in a harmonic potential. The envelope is the absolute value and the oscillatory curve in the interior is the imaginary part of the wavepacket. The zero-point, phase
has been removed for clarity. Note that the average position and momentum change according to the classical equations of motion, i.e. the average momentum vanishes at the classical turning points and is maximum at the potential minimum.
has been removed for clarity. Note that the average position and momentum change according to the classical equations of motion, i.e. the average momentum vanishes at the classical turning points and is maximum at the potential minimum.