Is Heisenberg principle applicable to a photon?

fluidistic
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I wonder if Heisenberg principle (both \Delta p \Delta x \geq \frac{\hbar }{2} and \Delta E \Delta t \geq \frac{\hbar }{2}) can be applied to photons.
Say I have a laser emitting a flash. I know very well the wavelength of the photon, therefore its momentum. Also, I know well where it might be: it travels at c and must lie somewhere inside the cross section area of the laser beam situated at a distance ct from the laser, if I consider a time t after emission. Which seems to contradict that if I know well the momentum of the laser, I shouldn't know well where it is.
The same doubt arises with the relation between \Delta E and \Delta t. I know very well the energy of a laser photon since I know very well its wavelength. And I do so at any time...
Unless E\neq \frac{hc}{\lambda}...
So I don't understand if I'm missing something or if Heisenberg's principle cannot be applied to photons.
 
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It applies to lasers. You don't know the wavelength as well as you think. Common notion is that a laser is monochromatic, and compared to natural light, "it is", but there is a uncertainty to the wavelength that prevents it to be perfectly monochromatic.
 
Dr Lots-o'watts said:
It applies to lasers. You don't know the wavelength as well as you think. Common notion is that a laser is monochromatic, and compared to natural light, "it is", but there is a uncertainty to the wavelength that prevents it to be perfectly monochromatic.

That explains everything... thanks a lot.
 
I think you will find the discussion in Landau, vol 4, section 1, "The uncertainty principle in the relativistic case" to be very illuminating.

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