1.16: The Commutator
- Page ID
- 50117
One must be careful to observe the correct order of operators. For example,
\[ \hat{x}\hat{k} \neq \hat{k}\hat{x} \nonumber \]
but
\[ \hat{x}\hat{\omega} = \hat{\omega}\hat{x} \nonumber \]
In quantum mechanics we define the commutator:
\[ [\hat{q},\hat{r}]=\hat{q}\hat{r}-\hat{r}\hat{q} \nonumber \]
We find that the operators \(\hat{r}\) and \(\hat{\omega}\) commute because \([\hat{x},\hat{\omega}]=0\).
Considering the operators \(\hat{x}\) and \(\hat{k}\):
\[ [\hat{x},\hat{k}]=-ix\frac{d}{dx}+i\frac{d}{dx}x \nonumber \]
To simplify this further we need to operate on some function, f(x):
\[\begin{align*} [\hat{x},\hat{k}]f(x) &=-ix\frac{df}{dx}+i\frac{d}{dx}(xf) \\[4pt] &= -ix\frac{df}{dx}+if\frac{dx}{dx}+ix\frac{df}{dx} \\[4pt] &=if \end{align*} \nonumber \]
Thus, the operators \(\hat{x}\) and \(\hat{k}\) do not commute, i.e.
\[ [\hat{x},\hat{k}] = i \nonumber \]
Although we used Fourier transforms, Equation (1.10.13) can also be derived from the relation (1.16.5) for the non-commuting operators operators \(\hat{x}\) and \(\hat{k}\). It follows that all operators that do not commute are subject to a similar limit on the product of their uncertainties. We shall see in the next section that this limit is known as "the uncertainty principle‟.
\(^{†}\)We have applied Parseval's theorem; see the Problem Sets.