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Implication of energy measurement for wave function as a sum of stationary states 
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#1
Oct1712, 12:30 PM

P: 296

In Griffiths' page 36/37 he says "As we'll see in Chapter 3, what Cn^2 tells you is the probability that a measurement of the energy would yield the value En (a competent measurement will always return one of the "allowed" values  hence the name  and Cn^2 is the probability of getting the particular value En."
This statement comes at the end of the infinite square well section and it concerns any sum of stationary states. Wouldn't measuring one of the allowed energies "En", mean collapsing the wave function into the nth stationary state (and that state only!)? Doesn't that mean that the wave function has then assumed a single stationary state, thereby guaranteeing all subsequent energy measurements of the wave function to yield that particular En? This seems to disagree with my intuition about what happens to a wave function after measurement (that it would "delocalize" in energy space) and it disagrees with my professor's interpretation who literally takes issue with the statement that an energy measurement must yield one of the allowed values. He says that it can yield any value, and that a mix/sum of specific n states are responsible for returning a non"allowed" En. 


#2
Oct1712, 12:45 PM

P: 860




#3
Oct1712, 12:48 PM

P: 296

So just to be clear  once I measure the energy of my infinite square well wave function, I have set it into a stationary state corresponding to that allowed energy and it will remain there subsequently? All future measurements, for all time, of the energy of that wave function will be my first energy measurement? Doesn't that violate some version of the uncertainty principle? The delta E delta t one?
This very much disagrees with my professor so I want to make sure! And I understand your point about the expectation value but we were talking about an actual single measurement. 


#4
Oct1712, 01:26 PM

P: 860

Implication of energy measurement for wave function as a sum of stationary states
The idea is that (delta E)(delta T) ~ hbar, where (delta E) is the spread in energy and (delta T) is some measure of the characteristic time over which the system changes. If we reduce (delta E) to zero, then (delta T) must go to infinity; that is, it takes infinitely long for the system to undergo any changes; that is, the system never changes. Of course, this is why we call energy eigenstates "stationary states"! 


#5
Oct1712, 01:52 PM

P: 296

So all one needs to do to create a wave function that is exactly one stationary state is to create any wave function at all first (which is going to be a sum of stationary states), then measure its energy. Now you have a very simple single function of time and space rather than a sum of many. Can you give an example of an energy measurement in the real world which might be unperturbative enough to be a "pure" energy measurement?
What about measuring the wavelength of a photon emitted from an electron. If a specific allowed jump in energy of an electron caused this photon to be emitted, might not my measurement of that photon's wavelength be considered a "pure" energy measurement of the electron? Would that very measurement of the photon not put the electron in a stationary state? I am of course assuming that one could express the wave function of an electron as a sum of stationary states, which assumes that the time dependent Schrodinger equation of the electron (in some potential) would be separable, which is not necessarily true. 


#6
Oct1712, 10:01 PM

P: 860

To prepare a photon in a highly precise energy state you can use an optical cavity: http://en.wikipedia.org/wiki/Optical_cavity
An optical cavity consists of a pair of partially transparent mirrors separated by a certain distance. If you shoot a photon at it, it will only pass through if it has a wavelength (thus energy) in a very narrow range. You can think of this as an energy measurement measurement than detects whether the photon has a certain energy or not. A problem with thinking about stationary states of realworld electrons is that the only stationary state of an electron in an actual atom is the ground state. The excited states aren't pure energy eigenstates: they have a finite lifetime, after which they transition to the ground state + a photon, so they aren't stationary. 


#7
Oct1712, 10:23 PM

P: 446

You should make sure that you are not misunderstanding your prof. In any real world situation, the particle will not be perfectly isolated and there is no infinite well, so over time outside influences will cause the state to evolve from the stationary state. However, in the theoretical perfect world of the infinite square well, a perfect measurement will leave the particle in a fixed state.
Whenever real world situation come in, there will be many complications to this, but don't confuse those complications with the fundamental theory. There are more complicated situations when it comes to a measurement of the energy, but a measurement that gives you zero uncertainty for the energy of a single particle will necessarily be an eigenvalue of the state. 


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