Are Pauli Matrices Unitary and Do Their Complex Conjugates Match?

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Discussion Overview

The discussion revolves around the properties of Pauli matrices, specifically their unitarity and the relationship between their complex conjugates and transposes. Participants explore definitions and characteristics of these matrices, including their hermitian nature and connections to higher-dimensional representations.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether the first Pauli matrix is unitary based on its transpose.
  • Another participant provides definitions for unitary and hermitian matrices, demonstrating that all Pauli matrices are both hermitian and unitary.
  • A different participant notes that the diagonal elements of hermitian matrices must be real and discusses the traceless property of Pauli matrices, suggesting they form a basis for complex 2×2 traceless hermitian matrices.
  • Another participant mentions that adding the identity matrix creates a basis for all 2×2 hermitian matrices, not just traceless ones.
  • A participant seeks clarification on the transpose and complex conjugate of the second Pauli matrix, leading to a detailed explanation of the relationships between these operations.
  • One participant introduces a question about the relationship between spin-1 matrices and Pauli matrices, suggesting a connection but noting that the properties differ for the 3×3 matrices.

Areas of Agreement / Disagreement

Participants generally agree on the properties of the Pauli matrices being hermitian and unitary. However, there is some disagreement regarding the relationship between spin-1 matrices and Pauli matrices, with at least one participant asserting that they are not the same.

Contextual Notes

The discussion includes various mathematical properties and assumptions about matrix operations, which may not be fully resolved or universally accepted among participants.

shounakbhatta
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Hello,

I am new to this:

Taking the first Pauli Matrix:

σ1=[0 1
1 0]

Doing the transpose it becomes:

[0 1
1 0]

So is it a unitary matrix?

Similarly
σ2= [0 -i
i 0]

Doing a transpose

=[0 i
[-i 0]

Does it mean the complex conjugates are the same?

-- Shounak
 
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A matrix M is unitary iff

[tex]M^\dagger M = MM^\dagger = 1[/tex]

A matrix M is hermitian iff

[tex]M^\dagger = M[/tex]

with

[tex]M^\dagger = {M^\ast}^t[/tex]

So for the Pauli matrix σ² you have

[tex]M = \begin{pmatrix} 0 & -i \\ i & 0 \end{pmatrix}[/tex]

[tex]M^\dagger = {\begin{pmatrix} 0 & -i \\ i & 0 \end{pmatrix}^\ast}^t = {\begin{pmatrix} 0 & i \\ -i & 0 \end{pmatrix}}^t = {\begin{pmatrix} 0 & -i \\ i & 0 \end{pmatrix}} = M[/tex]

[tex]MM^\dagger = M^2 = 1[/tex]

The same applies to other Pauli matrices, so every a Pauli matrix σi is both hermitian and unitary
 
Since Tom answered the question, I'll just make a comment about something that I find useful to know.

Note that the diagonal elements of a hermitian matrix must be real. The Pauli matrices are also traceless, i.e the sum of the diagonal elements is 0. Every complex 2×2 traceless hermitian matrix can be written in the form
$$\begin{pmatrix} x_3 & x_1-ix_2\\ x_1+ix_2 & -x_3\end{pmatrix},$$ where the ##x_i## are real numbers, and this can clearly can also be written as ##\sum_i x_i\sigma_i##. So the Pauli matrices are basis vectors for the vector space of complex 2×2 traceless hermitian matrices. If you can remember this, it's pretty easy to remember what they look like.
 
Last edited:
If you add the 2*2 identity matrix you get a basis for 2*2 hermitean matrices (no longer traceless)

These matrices are related to 4-dim. Minkowski space in SR which you see immediately by calculating the determinant
 
Thanks for the help.

Just a small question to Tom"

(0 -i
i 0) when transposed becomes (0 i
i 0) but why again= (0 -i
i 0)?

Thank you.

-- Shounak
 
shounakbhatta said:
(0 -i
i 0) when transposed becomes (0 i
i 0) but why again= (0 -i
i 0)?
I don't quite understand what you're asking, but maybe this will clear it up:
$$\begin{align}
\sigma_2 &=\begin{pmatrix}0 & -i\\ i & 0\end{pmatrix}\\
\sigma_2^T &=\begin{pmatrix}0 & i\\ -i & 0\end{pmatrix}\\
\sigma_2^\dagger &= \begin{pmatrix}0^* & i^*\\ (-i)^* & 0^*\end{pmatrix} =\begin{pmatrix}0 & -i\\ i & 0\end{pmatrix}=\sigma_2
\end{align}$$
 
Thank you. Yes, it clears up.

I have one more question:

For a spin 1 for Pauli matrix it follows:

Jx=hbar/√2 (0 1 0
1 0 1
0 1 0)


Now the above, does it follows from below?

σ1=σx= (0 1
1 0)

But Jz=hbar( 1 0 0
0 0 0
0 i 0)

whereas σ3=σz= (1 0
0 -1)

is it somehow related to each other?
 
the 3*3 matrices for spin 1 have partially different properties and are NOT Pauli matrices!
 

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