Solving Problem 2.4 in Ballentine: Nonnegativeness Derivation

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Homework Help Overview

The discussion revolves around Problem 2.4 from Ballentine, which involves the derivation of nonnegativeness for a 2x2 state operator in quantum mechanics. Participants are exploring the properties of the operator, particularly focusing on trace normalization, self-adjointness, and the implications of these properties on the eigenvalues of the operator.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the representation of the state operator in a specific orthonormal basis and the implications of trace normalization and self-adjointness. There are attempts to derive conditions for nonnegativeness using eigenvalues and inequalities related to the trace. Some participants question how to further develop the reasoning based on the derived inequalities.

Discussion Status

The discussion is active, with participants providing insights into different approaches, such as working directly with eigenvalues. Some have offered partial reasoning and examples, while others are exploring the implications of their findings. There is recognition of the complexity involved, particularly in higher dimensions, and participants are engaging with the problem without reaching a consensus on a complete solution.

Contextual Notes

Participants note that the problem constraints include the self-adjointness of the state operator and the conditions on the trace. There is an acknowledgment of the challenges posed by higher-dimensional cases, where the presence of negative eigenvalues could violate the nonnegativeness condition.

EE18
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I am trying to solve Problem 2.4 in Ballentine:
Screen Shot 2023-03-07 at 10.41.08 AM.png

I note in my attempt below to what (2.6) and (2.7) refer.

My attempt thus far is as follows:
A ##2 \times 2## state operator can be represented in a particular orthonormal ##\beta = \{\phi_i\}## as below, where we have enforced trace normalization (2.6) and self-adjointness (2.7) (and have yet to enforce nonnegativeness),
$$[\rho]_{\beta} = \begin{bmatrix}
a & b \\
b^* & (1-a)
\end{bmatrix}$$
Now enforcing ##Tr{\rho^2}## and using the basis independence of the trace we obtain
$$Tr{\rho^2} = Tr{[\rho]_{\beta}^2} = Tr{ \begin{bmatrix}
a & b \\
b^* & (1-a)
\end{bmatrix}^2} = a^2 +2|b|^2+ (1-a)^2 \leq 1$$
with ##a \in \mathbb{R}##.

Now for an arbitrary ##u## in our space we may expand ##u = \sum_i c_i {\phi_i}## so we can immediately compute
$$(u,\rho u) = \begin{bmatrix}
c_1^* & c_2^*
\end{bmatrix}\begin{bmatrix}
a & b \\
b^* & (1-a)
\end{bmatrix}\begin{bmatrix}
c_1 \\ c_2
\end{bmatrix} = \begin{bmatrix}
c_1^* & c_2^*
\end{bmatrix}
\begin{bmatrix}
ac_1 + bc_2 \\ b^*c_1+(1-a)c_2 \end{bmatrix}$$
$$=c_1^*(ac_1 + bc_2)+ c_2^*(b^*c_1+(1-a)c_2) = |{c_1}|^2a +2\textrm{Re}(c_1^*c_2b) + (1-a)^2|{c_2}|^2$$
but I can't seem to see how to go further here. It seems like I have to use my aforementioned inequality but I can't see how. Any help would be greatly appreciated.
 
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For this type of problem, it's often more efficient to work with the eigenvalues directly, rather than a generic matrix. For this problem, we are given that:
$$Tr(\rho^2) ~\le 1 ~,~~~~ Tr(\rho) ~=~ 1 ~,~~~~ \rho = \rho^\dagger ~.$$For the 2D case, there are 2 eigenvalues, ##\rho_1## and ##\rho_2##, say, hence the eigenvalues of ##\rho^2## are the squares of these.

Self-adjointness of ##\rho## implies both the ##\rho_i## are real, hence ##\,\rho_i^2 \ge 0##.

The trace of a matrix is the sum of its eigenvalues, so we have 2 conditions:
$$\rho_1 + \rho_2 ~=~ 1 ~,~~~~ \rho^2_1 + \rho^2_2 ~\le~ 1 ~.$$Squaring the 1st equation gives $$\rho_1^2 + \rho_2^2 + 2 \rho_1 \rho_2 ~=~ 1 ~,$$and using this in conjunction with the 2nd equation implies... what?

I leave it to you to figure out the rest of the proof, including the follow-on of why it doesn't work for higher dimensional matrices. :oldbiggrin:
 
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strangerep said:
For this type of problem, it's often more efficient to work with the eigenvalues directly, rather than a generic matrix. For this problem, we are given that:
$$Tr(\rho^2) ~\le 1 ~,~~~~ Tr(\rho) ~=~ 1 ~,~~~~ \rho = \rho^\dagger ~.$$For the 2D case, there are 2 eigenvalues, ##\rho_1## and ##\rho_2##, say, hence the eigenvalues of ##\rho^2## are the squares of these.

Self-adjointness of ##\rho## implies both the ##\rho_i## are real, hence ##\,\rho_i^2 \ge 0##.

The trace of a matrix is the sum of its eigenvalues, so we have 2 conditions:
$$\rho_1 + \rho_2 ~=~ 1 ~,~~~~ \rho^2_1 + \rho^2_2 ~\le~ 1 ~.$$Squaring the 1st equation gives $$\rho_1^2 + \rho_2^2 + 2 \rho_1 \rho_2 ~=~ 1 ~,$$and using this in conjunction with the 2nd equation implies... what?

I leave it to you to figure out the rest of the proof, including the follow-on of why it doesn't work for higher dimensional matrices. :oldbiggrin:
Thank you so much for the detailed response. If possible, I came up with a demonstration of why it doesn't work for ##\dim V > 2## but it's really ugly:

In the case of 3 or more dimensions (for arbitrary dimension consider a state operator with 3 nonzero eigenvalues) we see that we can follow the proof up to the point ##Tr{\rho^2} = \rho_1^2+ \rho_2^2 + \rho_3^2 \leq 1 = \rho_1^2+ \rho_2^2 \rho_3^2 +2\rho_1 \rho_2 +2\rho_1 \rho_3 +2\rho_3 \rho_2## which implies ##\rho_1 \rho_2 +\rho_1 \rho_3 +\rho_3 \rho_2 \geq 0##. We can imagine obeying this constraint with one negative eigenvalue and two positive eigenvalues such that the positive eigenvalues "outweigh" the negative. Consider ##\rho_1 = \rho_2 -1/10 = 1/2## and ##\rho_3 = -1/10##. Then we have ##\rho_1 \rho_2 +\rho_1 \rho_3 +\rho_3 \rho_2 \geq 0## and ##Tr{\rho} = 1##. If we then take the eigenvector corresponding to that negative eigenvalue we see that the expectation value is negative.

Would you be able to suggest a nicer proof? Thank you again!
 
You only need to recognize that, for dim##V > 2,## there could be 1 or more negative eigenvalues while still satisfying the input constraints. That alone is enough to violate Ballentine's eq(2.12), i.e., that ##\rho_n \ge 0## for all ##n##.
 
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