Finding the Density Matrix of a 4x4 System at Thermal Equilibrium

In summary, the density matrix of a system at thermal equilibrium can be obtained by using the formula \rho = \frac{e^{-\beta H}}{Z}, where \beta = \frac{1}{kT} and Z = tr (e^{-\beta H}). To find e^{-\beta H}, the Hamiltonian can be written in the form of XDX^{-1} where X is the matrix formed by the eigenvectors of H and D is a diagonal matrix with elements equal to the eigenvalues of H. By taking the exponential of the diagonal elements of -\beta D, the matrix e^{-\beta H} can be obtained. However, it is important to note that the final answer should be multiplied
  • #1
yukawa
13
0
How to obtain the density matrix of the following system at thermal equilibrium?

Given:

Hamiltonian H :(in 4x4 matrix form)
Hij = the i-th row and j-th column element of H
H11 = (1+c)/2
H22 = -(1+c)/2
H23 = 1-c
H32 = 1-c
H33 = -(1+c)/2
H44 = (1+c)/2
where c is a parameter and all other elements are zero
 
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  • #2
Hi yukawa! :smile:

Show us what you've tried, and where you're stuck, and then we'll know how to help! :smile:
 
  • #3
I tried to find it by using this formula:

[tex]\rho = \frac{e^{-\beta H}}{Z} [/tex]

where [tex]\beta = \frac{1}{kT}[/tex] and [tex]\ Z = tr (e^{-\beta H}) [/tex]

I was stuck at finding [tex]\ e^{-\beta H} [/tex].

The following is what i tried in order to find [tex]\ e^{-\beta H} [/tex].

i) finding the eigenvectors and eigenvalues of H and write H in form of XDX-1 (where X is the matrix formed by the eigenvectors of H and D is a diagoanl matrix with elements equal to the eigenvalues of H) :

explicitly,
X11 = X44= 1
X22 = X23 = X33 = [tex]1/\sqrt{2}[/tex]
X32 = -[tex]1/\sqrt{2}[/tex]
all other elements are zero.
and
D11 = D44 = (1+c)/2
D22 = (-3+c)/2
D33 = (1-3c)/2
all other elements are zero.
(by the way, how can i input a matrix in the post?)

ii) then i calculate [tex]\ e^{-\beta H} [/tex] by:
[tex]\ e^{-\beta H} = X e^{-\beta D} X^{-1} [/tex] and [tex]\ e^{-\beta D}[/tex] is just taking the exponential of the digonal elements of [tex] -\beta D[/tex].

Is this approch correct? I can't get the answer as shown in my notes.
 
  • #4
LaTeX

yukawa said:
(by the way, how can i input a matrix in the post?)

Is this approch correct? I can't get the answer as shown in my notes.

Hi yukawa! :smile:

I've just woken up … :zzz: not in functioning mode yet … :confused:

For the LaTeX for matrices tables and long equations, see http://www.physics.udel.edu/~dubois/lshort2e/node56.html#SECTION00850000000000000000

And if you know the answer, always tell us!

it makes it much quicker for us to spot where you've gone wrong. :wink:
 
Last edited by a moderator:
  • #5
the eigenvectors(left) and eigenvalues(right) of the Hamiltonian are:

[tex]\left|\uparrow\uparrow\right\rangle : (1+c)/2[/tex]

[tex]\left|\downarrow\downarrow\right\rangle : (1+c)/2
[/tex]

[tex]\frac{1}{\sqrt{2}}(\left|\uparrow\downarrow\right\rangle - \left|\downarrow\uparrow\right\rangle ) : (-3+c)/2[/tex]

[tex]\frac{1}{\sqrt{2}}(\left|\uparrow\downarrow\right\rangle + \left|\downarrow\uparrow\right\rangle ) : (1-3c)/2[/tex]

Write H = XDX-1,
[tex]\begin{displaymath}
\mathbf{H} =
\left(\begin{array}{cccc}
1 & 0 & 0 & 0 \\
0 & \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} & 0 \\
0 & -\frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} & 0 \\
0 & 0 & 0 & 1 \\
\end{array}\right)

\left(\begin{array}{cccc}
\frac{1+c}{2} & 0 & 0 & 0 \\
0 & \frac{-3+c}{2} & 0 & 0 \\
0 & 0 & \frac{1-3c}{2} & 0 \\
0 & 0 & 0 & \frac{1+c}{2} \\
\end{array}\right)

\left(\begin{array}{cccc}
1 & 0 & 0 & 0 \\
0 & \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} & 0 \\
0 & \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} & 0 \\
0 & 0 & 0 & 1 \\
\end{array}\right)

\end{displaymath}

[/tex]

Therefore, take k = 1,
[tex]\begin{displaymath}
\mathbf{e^{-\beta H}} =
\left(\begin{array}{cccc}
1 & 0 & 0 & 0 \\
0 & \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} & 0 \\
0 & -\frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} & 0 \\
0 & 0 & 0 & 1 \\
\end{array}\right)

\left(\begin{array}{cccc}
e^{-\frac{1+c}{2T}} & 0 & 0 & 0 \\
0 & e^{-\frac{-3+c}{2T}} & 0 & 0 \\
0 & 0 & e^{-\frac{1-3c}{2T} }& 0 \\
0 & 0 & 0 & e^{-\frac{1+c}{2T}} \\
\end{array}\right)

\left(\begin{array}{cccc}
1 & 0 & 0 & 0 \\
0 & \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} & 0 \\
0 & \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} & 0 \\
0 & 0 & 0 & 1 \\
\end{array}\right) =

\left(\begin{array}{cccc}
e^{-\frac{1+c}{2T}} & 0 & 0 & 0 \\
0 & \frac{1}{2}(e^{-\frac{-3+c}{2T}}+e^{-\frac{1-3c}{2T}}) & \frac{1}{2}(-e^{-\frac{-3+c}{2T}}+e^{-\frac{1-3c}{2T}}) & 0 \\
0 & \frac{1}{2}(e^{-\frac{-3+c}{2T}}+e^{-\frac{1-3c}{2T}}) & \frac{1}{2}(e^{-\frac{-3+c}{2T}}+e^{-\frac{1-3c}{2T}}) & 0 \\
0 & 0 & 0 & e^{-\frac{1+c}{2T}} \\
\end{array}\right)



\end{displaymath}

[/tex]

However, the ans. in the notes is:

[tex]\begin{displaymath}
\mathbf{e^{-\beta H}} =
\left(\begin{array}{cccc}
e^{-\frac{1+c}{T}} & 0 & 0 & 0 \\
0 & cosh\frac{1-c}{T} & -sinh\frac{1-c}{T} & 0 \\
0 & -sinh\frac{1-c}{T} & cosh\frac{1-c}{T} & 0 \\
0 & 0 & 0 & e^{-\frac{1+c}{T}} \\
\end{array}\right)
\end{displaymath}

[/tex]
 
  • #6
Hi yukawa! :smile:

Best ever LaTeX! :biggrin:

Now I know the answer, it's easy to see where you've gone wrong …

you haven't!

you're just out by a factor of e-(1+c)/2T! :wink:
 
Last edited:
  • #7
Oh! yes!
I got it.
Thank you very much.:smile:
 

1. What is a density matrix?

A density matrix is a mathematical representation of a quantum mechanical system that describes the state of the system in terms of probabilities. It is used to describe the behavior of a system that is in a superposition of multiple states.

2. How is the density matrix of a 4x4 system at thermal equilibrium calculated?

The density matrix of a 4x4 system at thermal equilibrium can be calculated by taking the tensor product of the density matrix for each individual subsystem and then applying the Boltzmann distribution to account for thermal equilibrium. This results in a 16x16 matrix with non-zero elements only on the diagonal.

3. What does the diagonal of the density matrix represent?

The diagonal elements of the density matrix represent the probabilities of the system being in each possible state. The sum of all diagonal elements must equal 1, representing the fact that the system must be in one of its possible states.

4. How does the density matrix change over time?

The density matrix of a system can change over time due to interactions with its environment or external forces. This change is described by the Schrödinger equation, which takes into account the Hamiltonian of the system and the density matrix at a given time.

5. What is the significance of finding the density matrix of a 4x4 system at thermal equilibrium?

Finding the density matrix of a 4x4 system at thermal equilibrium allows us to understand the statistical behavior of the system and make predictions about its future states. It is an important tool in quantum mechanics and is used in a variety of applications, such as quantum computing and materials science.

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