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How to visualize the quantum wave nature of matter?
- The wavelength measures the spatial period of the sine wave, i.e. the distance between repeating wave forms.
- The frequency measures the how often a sine wave repeats itself per second.
- The amplitude measures the height of the wave crest over the zero line.
- The Phase determines the position of a reference point on the wave to a second point in space, in units of the wavelength.
Macroscopic wave phenomena can be easily visualized.
Wave 1 | Wave 2 | ||
Amplitude | \(A\) | ||
Wavelength | \(\lambda\) | ||
Phaseshift | \(\Delta \varphi\) |
Interference
In order to measure very small distances it often useful to employ wave interference. When two wave fields are superposed their wave crests may add up (constructive interference) while the encounter of a crest and a trough tends to cancel the wave (destructive interference). The pattern of constructive and destructive interference in space allows to determine the wavelength.
It is a particular trait of quantum physics that wave functions may be associated not only with dense ensembles of particles but even with an ensemble that has been diluted to a single particle in the machine at any instant. The wave function seemingly still describes the individual quantum object. This is why one often says that ‘each particle interferes with itself’.
Quantum theory can only predict probabilities for a certain outcome. Which of the many possibilities is finally assumed in a measurement on an initial superposition of options and states is entirely random. Only many measurements under identical conditions reveal the strictly deterministic distribution of probabilities which is also obtained from solving Schrödinger’s equation
\( i\hbar\frac{\partial}{\partial t}\psi(\mathbf{r},t) \;=\; \left(- \frac{\hbar^2}{2m}\Delta + V(\mathbf{r},t)\right)\psi(\mathbf{r},t) \)
All experiments so far have confirmed Born’s rule: the squared modulus \(|\psi|^2\) of the state function \(psi\) represents the probability to find a quantum object at time \(t\) at position \(r\) with all other parameters contained in \(psi\).