Modern 2:Measurements and Eigenstates

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'''NB''':  that is not <math>\hbar</math>
 
'''NB''':  that is not <math>\hbar</math>
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===examples of precisely determined measurements===
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[http://en.wikipedia.org/wiki/Spectral_line spectral lines]

Revision as of 03:09, 27 February 2006

measurements uncertainty

We have seen that in general if N copies of a system are prepared in identical states, then the result of any measurement will have a statistical spread of values. Further, there is a fundamental connection between the uncertainty of an observable and that of its Fourier transform pair. E.g.,

\Delta x \Delta p_x \geq \hbar /2 

It would be nice if we could expect something like

\Delta E \Delta t \geq \hbar/2

to be true, but it's not obvious.

John Baez on the time/energy uncertainty relation

One of the reasons it's not obvious is that there while there is an energy operator in QM (the Hamiltonian), there is no time operator in QM!

It turns out that from the Fourier transform ideas we've talked about you can show that:

\Delta \omega \Delta t \geq 2 \pi

which then gives (using Einstein's relation)

 \Delta E \Delta t \geq h   

NB: that is not \hbar


examples of precisely determined measurements

spectral lines

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