What is commutator of position and momentum operator?
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What is commutator of $ \hat{x} $ and $ \hat{p} $?
here our position and momentum are also operators and we need to find the $ [ \hat{x}, \hat{p} ] $.
so how will we find it??
as the name suggests they are operator and they operate on the functions (function of the Hilbert space).
for position operator we just multiply function by $x$ and for momentum operator we differentiate the function by $x$ and then multiple by $-i\hbar $. ( Note we are working only in 1 dimentions)
generally working with operators we use test function $\phi(x)$.
this $\phi(x)$ is arbitrary function.
so let's try to find
$ [ \hat{x}, \hat{p} ]\phi(x) $
by using defination of commutator we can write it as
$=[x(-i\hbar)\frac{d}{dx}-(-i\hbar)(\frac{d}{dx})x]\phi(x)$
$= [x(-i\hbar)\frac{d}{dx}\phi(x)-(-i\hbar)\frac{d}{dx}(x\phi(x)]$
$ = -i\hbar( x\frac{d\phi}{dx} - x\frac{d\phi}{dx}-\phi(x))$
$ = i\hbar\phi(x)$
now as $\phi(x)$ was arbitrary we'll Remove that and we get
$ [ \hat{x}, \hat{p} ] = i\hbar$
This equation is known as the cononical commutation relation. It's called canonical because position and momentum are related by Fourier transforms.
This is precisely the reason why minimum uncertainty in position and momentum is always great or equal to $\frac{\hbar}{2}$.
If for any 2 operators the commutator vanishes than uncertainty is zero that is you can measure both quantity simultaneously.( Basically $ \sigma_A\sigma_B = 0 $ ). Well if commutator is zero than they share simultaneous Eigen functions. But we'll discuss that into future posts.
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