In one line
The wave function \(\psi\) is a mathematical function that describes the quantum state of a particle, and \(|\psi|^2\) gives the probability per unit length (or volume) of finding the particle at a location.
Explained simply
A weather forecast does not tell you exactly where the rain will fall; it gives a "chance of rain" map. The wave function works like that for an electron. You cannot say exactly where the electron is, but \(|\psi|^2\) tells you how likely you are to find it at each place. Where \(|\psi|^2\) is large, the electron is often found.
How it works
- For a particle, a wave function \(\Psi(x, t)\) is a solution of Schrödinger's equation. It is generally complex, so it cannot be measured directly.
- Max Born's interpretation: \(P(x) = |\Psi|^2 = \Psi^*\Psi\) is the probability density (\(\Psi^*\) is the complex conjugate).
- Probability of finding the particle between \(x\) and \(x + dx\) is \(|\Psi|^2dx\); in 3D, between volume \(dV\): \(|\Psi|^2dV\).
- Probability over a region \(a\) to \(b\): \(\int_a^b|\Psi|^2dx\).
- Since the particle must be somewhere, the total probability is 1: \(\int_{-\infty}^{\infty}|\Psi|^2dx = 1\). This is the normalisation condition.
- If a found \(\psi\) gives a total of \(N\) instead of 1, divide it by \(\sqrt{N}\) to normalise it.
Key formula
\(P = |\Psi|^2 = \Psi^*\Psi\); \(\int_{-\infty}^{\infty}|\Psi|^2dx = 1\). In one dimension \(|\Psi|^2\) has unit m−1; in 3D, m−3; the probability itself is dimensionless.
Quick example
For a particle in a box of length \(L\), \(\psi = A\sin(\pi x/L)\). Normalising: \(A^2\int_0^L\sin^2(\pi x/L)dx = A^2L/2 = 1\), so \(A = \sqrt{2/L}\). The probability density \(\frac{2}{L}\sin^2(\pi x/L)\) is maximum at \(x = L/2\), so the particle is most likely found at the centre and never at the walls.
Common mistakes
- Saying \(\psi\) itself is the probability; it is \(|\psi|^2\).
- Forgetting the complex conjugate when \(\psi\) is complex.
- Not normalising before calculating probabilities.
How MU asks it
Asked as "What is a wave function? State its physical significance" (3 marks) or "Explain probability density and normalisation" (3 to 5 marks). Define \(\psi\), give Born's interpretation \(|\psi|^2\), write the normalisation integral, and note that \(\psi\) itself has no direct physical meaning.