I Confused about the spectrum of an observable

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The spectrum of an observable in quantum mechanics consists of eigenvalues, which represent the possible outcomes of measurements. These eigenvalues are distinct from probability amplitudes, which are derived from the inner product of states. The actual measurement outcome is determined by the system's state, while the eigenvalues are fixed by the potential of the system. The probability of measuring a specific eigenvalue is calculated using the inner product of the system's state vector and the corresponding eigenstate. Clarifications provided in the discussion helped resolve the confusion regarding the relationship between eigenvalues and probability amplitudes.
nomadreid
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Eigenvalues of an observable are probability amplitudes but also stated to be measurement values. What am I missing?
This is a very elementary question, from the beginnings of quantum mechanics.

For simplicity, I refer to a finite case with pure states.

If I understand correctly, the spectrum of an observable is the collection of eigenvalues formed by the inner product of states and hence equal to probability amplitudes; they are then associated to the possible values of a measurement.

Hence I am confused by statements such as the following

“Eigenvalues of observables are real and in fact are possible outcomes of measurements of a given observable.” (https://www.quantiki.org/wiki/observables-and-measurements, but not the only example.)

How can the square roots of probabilities, which are less than one, be values of measurements (which can be greater than one)?
 
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Eigenvalues are not the same as probability amplitudes. The wave function that gives the prob. amplitudes is one representation of the eigenstate, and it can be either a position or momentum representation.
 
nomadreid said:
Summary:: Eigenvalues of an observable are probability amplitudes but also stated to be measurement values. What am I missing?

If I understand correctly, the spectrum of an observable is the collection of eigenvalues formed by the inner product of states and hence equal to probability amplitudes
Only the green part of the sentence is required. The possible eigenvalues of the system are determined from the potential independent of the actual state of the system. This is the spectrum.
The result of any measurement will be determined by the actual state of the system. The measurement will yield an eigenvalue. The state vector of the system will predict the probability of that value being measured (i.e if you repeated the measurement on similarly prepared states blah blah) which is given by the inner product of the state vector of the system with the corresponding eigenstate.

.
 
Thank you very much, hutchphd and hilbert2. An explanation similar to the last two sentences of hutchphd's explanation apparently was picked up by me somewhere and morphed into the version I posted. This clears it up.
 
nomadreid said:
This clears it up.
Good.
May I congratulate you on your Gary Larson cartoon. Perhaps my all-time favorite, and that's a difficult choice.
 
For the quantum state ##|l,m\rangle= |2,0\rangle## the z-component of angular momentum is zero and ##|L^2|=6 \hbar^2##. According to uncertainty it is impossible to determine the values of ##L_x, L_y, L_z## simultaneously. However, we know that ##L_x## and ## L_y##, like ##L_z##, get the values ##(-2,-1,0,1,2) \hbar##. In other words, for the state ##|2,0\rangle## we have ##\vec{L}=(L_x, L_y,0)## with ##L_x## and ## L_y## one of the values ##(-2,-1,0,1,2) \hbar##. But none of these...

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