How Does the Trace of a Matrix Relate to Its Components in Quantum Mechanics?

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SUMMARY

The discussion focuses on the relationship between the components of a 2x2 matrix X in quantum mechanics and its trace. The matrix is expressed as X = a_0 + σ · a, where σ represents the 2x2 Pauli matrices. The trace of the matrix is calculated as tr(X) = 2a_0, and the traces of the products with Pauli matrices yield tr(σ_kX) = 2a_k for k = 1, 2, 3. The participants clarify how to derive the components a_0 and a_k in terms of the matrix elements X_{ij}, leading to the expression a_k = 1/2[(σ_kX)_{11} + (σ_kX)_{22}] for k = 0, 1, 2, 3.

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  • Understanding of 2x2 matrices and their properties
  • Familiarity with Pauli matrices in quantum mechanics
  • Knowledge of matrix trace operations
  • Basic concepts of quantum state representations using kets
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Xyius
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Homework Statement


Suppose a 2x2 matrix X (not necessarily Hermitian, nor Unitary) is written as..
X=a_0+σ \cdot a
(In the book σ and a are both bold and are being dotted.)
Where a_0 and a_{1,2,3} are numbers.

a.)How are a_0 and a_k, (k=1,2,3) related to tr(X) and tr(σ_kX)?
b.)Obtain a_0 and a_k in terms of the matrix elements X_{ij}.


Homework Equations


tr(X)= The trace of X, meaning the sum of its diagonal components.
tr(X)=\sum_{a'}\left\langle a'|X|a' \right\rangle
Where the name a' represents base kets.

The Attempt at a Solution



I do not know where to start to be honest. My first question is how can a 2x2 matrix operator equal a number a_0 plus the dot product of two vectors? I know I must be misinterpreting this. Can anyone help?
 
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The σ's are the 2x2 Pauli matrices, so what the problem means is :

X = a0*(2x2 Identity matrix) + ax*(2x2 Pauli matrix σx) + ay*(2x2 Pauli matrix σy)+ az*(2x2 Pauli matrix σz)
 
phyzguy said:
The σ's are the 2x2 Pauli matrices, so what the problem means is :

X = a0*(2x2 Identity matrix) + ax*(2x2 Pauli matrix σx) + ay*(2x2 Pauli matrix σy)+ az*(2x2 Pauli matrix σz)

Ah that makes it MUCH more clear! So I basically plugged everything in and found the trace in each case and got..

tr(X)=2a_0
tr(σ_{1}X)=2a_1
tr(σ_{2}X)=2a_2
tr(σ_{3}X)=2a_3

Which I assume is what they are looking for for part A. Part B however is making me a bit confused. Do they want me to just solve the above expressions for a?
 
No, you have some matrix X where
$$X = \begin{pmatrix} X_{11} & X_{12} \\ X_{21} & X_{22} \end{pmatrix} = a_0 + \vec{a}\cdot\vec{\sigma}$$The problem wants you to solve for a0 and the ak's in terms of the Xij's. Start by writing down explicitly what ##a_0 + \vec{a}\cdot\vec{\sigma}## is equal to.
 
Ohh okay so would this be on the right track?

a_k=\frac{1}{2}\left[ (σ_kX)_{11}+(σ_kX)_{22} \right]
Where k=0,1,2,3

EDIT: I got this by looking at the expressions I posted for part A and finding a common equation that suits all of them. I now see that you said to start by writing the original expression. I will try this.
 

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