Determining the state from observation?

  • Context: Undergrad 
  • Thread starter Thread starter pellman
  • Start date Start date
  • Tags Tags
    Observation State
Click For Summary

Discussion Overview

The discussion revolves around how to determine the state of a quantum system from observations, particularly focusing on the spin of fermions and the implications of measurement on the relative phases of superposition states. Participants explore concepts related to quantum tomography, the relationship between different spin measurements, and the challenges of recovering wave functions from probability distributions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the state of a fermion can be expressed as a superposition of eigenstates, with coefficients a and b, and question how to determine the relative phase between these coefficients.
  • Others argue that while the probabilities |a|^2 and |b|^2 can be determined through measurements, the relative phase cannot be obtained from these probabilities alone.
  • A later reply suggests that measuring spin in arbitrary directions can provide the necessary information to determine the relative phase, referencing quantum tomography as a method.
  • Some participants discuss the need for measurements along three axes to fully determine the state, while others contend that only two equations are necessary to find the two unknowns in the spinor representation.
  • One participant raises a theoretical question about recovering a wave function from its probability distributions in position and momentum representations, suggesting this might be a known theorem.
  • Another participant notes that knowing the probabilities for different axes may be excessive and discusses the relationship between the probabilities and the angles in the spinor representation.
  • There is a mention of the overall phase being unobservable, which complicates the recovery of the wave function from its squared magnitudes.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of measurements along multiple axes and the sufficiency of equations to determine the state. The discussion remains unresolved regarding the best approach to determine the relative phase and the recovery of wave functions from probability distributions.

Contextual Notes

Limitations include the dependence on the definitions of observables and the unresolved mathematical steps in determining the relationships between probabilities and angles in the spinor representation.

Who May Find This Useful

This discussion may be of interest to those studying quantum mechanics, particularly in the areas of quantum measurement, spin systems, and the mathematical foundations of quantum theory.

pellman
Messages
683
Reaction score
6
How does one determine the state of a system from observations?

Let us look at a simple example: the spin of a fermion. Any state of the system is a superposition of up and down eigenstates. Denote the coefficients in this superposition by a and b. The question here amounts to determining a and b up to an overall phase.By performing spin measurements on many identically prepared systems we can determine the ratio |a|^2 / |b|^2. But how do we get the relative phase?
 
Physics news on Phys.org
If ##\left|\right.\uparrow\left.\right>## and ##\left|\right.\downarrow\left.\right>## are eigenstates of ##\hat{S}_z## and the state of the system is ##a\left|\right.\uparrow\left.\right> + b\left|\right.\downarrow\left.\right>##, the relative phases of ##a## and ##b## affect what the probabilities of different eigenvalues of ##\hat{S}_x## and ##\hat{S}_y## are.
 
pellman said:
How does one determine the state of a system from observations?

Let us look at a simple example: the spin of a fermion. Any state of the system is a superposition of up and down eigenstates. Denote the coefficients in this superposition by a and b. The question here amounts to determining a and b up to an overall phase.By performing spin measurements on many identically prepared systems we can determine the ratio |a|^2 / |b|^2. But how do we get the relative phase?
I don't think you can because the only observables |a|2, |b|2are independent of phase.

With light one can use tomography to get relative phase.

[Beaten by Hilbert2 with a better answer]
 
One can measure the spin in arbitrary directions, and this get information of the required form. In general, look up quantum tomography!
 
hilbert2 said:
If ##\left|\right.\uparrow\left.\right>## and ##\left|\right.\downarrow\left.\right>## are eigenstates of ##\hat{S}_z## and the state of the system is ##a\left|\right.\uparrow\left.\right> + b\left|\right.\downarrow\left.\right>##, the relative phases of ##a## and ##b## affect what the probabilities of different eigenvalues of ##\hat{S}_x## and ##\hat{S}_y## are.
But the probability is only one real parameter, and one needs to determine three. With one equation this is impossible.
 
Ok. Well the reason
hilbert2 said:
If ##\left|\right.\uparrow\left.\right>## and ##\left|\right.\downarrow\left.\right>## are eigenstates of ##\hat{S}_z## and the state of the system is ##a\left|\right.\uparrow\left.\right> + b\left|\right.\downarrow\left.\right>##, the relative phases of ##a## and ##b## affect what the probabilities of different eigenvalues of ##\hat{S}_x## and ##\hat{S}_y## are.

This is it. I worked it out on paper. The relative phase in the S_z representation can be expressed in terms of the absolute values of the coefficients in all three representations. But you need measurements with respect to all three axes. Thanks!
 
Last edited:
This question came to me because I often see statements like, given a system in state ψ, what is the probability of observing the system to be in state ϕ? And I finally wondered, what does it mean to "observe the system to be in state ϕ" when observations can only return limited information?

So, just for fun, how about the next simple example?
Determining the (time-independent) position wave function for a single particle in one dimension

In principle, from observations we can get the probability distributions in both the position representation and in the momentum representations. The wave functions in each representation are related by a Fourier transform.

So the theoretical question amounts to: if we know | f(x) |^2 and |F(k)|^2 for two complex-valued functions f(x) and F(k) which are Fourier transforms, can we recover f(x)?

This is probably a theorem out there somewhere. Anyone know?
 
Last edited:
Knowing probabilities for three different axes is overkill.

Write a two-component spinor this way: ##|\psi\rangle = e^{i\chi} \left( \begin{array} \\ cos(\frac{\theta}{2}) e^{-i \frac{\phi}{2}} \\ sin(\frac{\theta}{2}) e^{+i \frac{\phi}{2}} \end{array} \right)##. The overall phase ##\chi## is unobservable. So there are two unknowns: ##\theta## and ##\phi##. So you shouldn't need more than 2 equations to determine them.

Let's let ##P_x, P_y, P_z## be the probabilities for measuring the particle to be spin-up in the three directions. Then, if I did the calculation correctly,

##P_x = \frac{1}{2} (1+sin(\theta) cos(\phi))##
##P_y = \frac{1}{2} (1+sin(\theta) sin(\phi))## (I might have made a sign error---it might be ##-sin(\theta) sin(\phi)##)
##P_z = \frac{1}{2} (1+cos(\theta))##

This implies a relationship between the three probabilities:

##\sum_j (2 P_j - 1)^2 = 1##
 
stevendaryl said:
##P_x = \frac{1}{2} (1+sin(\theta) cos(\phi))##
##P_y = \frac{1}{2} (1+sin(\theta) sin(\phi))## (I might have made a sign error---it might be ##-sin(\theta) sin(\phi)##)
##P_z = \frac{1}{2} (1+cos(\theta))##

Right. But knowing ##cos(\phi)## alone is not enough because there are two values of ##\phi## with that value of ##cos(\phi)##. You need both ##cos(\phi)## and ##sin(\phi)##
 
  • #10
pellman said:
So the theoretical question amounts to: if we know | f(x) |^2 and |F(k)|^2 for two complex-valued functions f(x) and F(k) which are Fourier transforms, can we recover f(x)?

This is probably a theorem out there somewhere. Anyone know?
This is a question you should ask at MathOverflow, where there are many professional mathematicians. You can then feed back the best answer from there to the present thread.
 
  • #11
pellman said:
So the theoretical question amounts to: if we know | f(x) |^2 and |F(k)|^2 for two complex-valued functions f(x) and F(k) which are Fourier transforms, can we recover f(x)?

This is probably a theorem out there somewhere. Anyone know?

I need to modify this statement since it is easily shown that for a given f the function ## g = e^{i \phi} f## for constant ##\phi## has both ##|g(x)|^2 = |f(x)|^2 ## and ##|G(k)|^2 = |F(k)|^2##. Which is fine from a quantum measurement standpoint. The overall phase is not observable.

So if we know | f(x) |^2 and |F(k)|^2 for two complex-valued functions f(x) and F(k) which are Fourier transforms, can we recover f(x) up to a constant factor of the form ## e^{i \phi} ##?
 
  • #12
A. Neumaier said:
This is a question you should ask at MathOverflow, where there are many professional mathematicians. You can then feed back the best answer from there to the present thread.
Thanks. I will try that.
 

Similar threads

  • · Replies 124 ·
5
Replies
124
Views
9K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 0 ·
Replies
0
Views
1K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 18 ·
Replies
18
Views
2K
  • · Replies 15 ·
Replies
15
Views
1K
  • · Replies 8 ·
Replies
8
Views
1K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 29 ·
Replies
29
Views
4K