- #1
earthling75
- 3
- 0
- Homework Statement
- Calculate the probability of finding a particle with spin = 1 in a given state to have an eigenvalue of ##\hbar$ in $S_y## basis.
- Relevant Equations
- $$S_{\pm}|s,m\rangle = \hbar \sqrt{s(s+1)-m(m\pm 1)}|s,(m\pm 1)\rangle$$
Probability ##=|\langle \chi |\chi_+^y \rangle|^2##
I know how to construct Sy for spin = 1 case from the raising and lowering operators.
I get
$$
S_y=\frac{i\hbar}{\sqrt{2}}\begin{pmatrix}
0 & -1 & 0 \\ 1 & 0 & -1 \\ 0 & 1 & 0 \\
\end{pmatrix}
$$
From what I have seen, the eigenspinor for $\hbar$ is found by solving
$$
\frac{i\hbar}{\sqrt{2}}\begin{pmatrix}
0 & -1 & 0 \\ 1 & 0 & -1 \\ 0 & 1 & 0 \\
\end{pmatrix}
\cdot
\begin{pmatrix}
\alpha \\ \beta \\ \gamma
\end{pmatrix} =
\hbar \begin{pmatrix}
\alpha \\ \beta \\ \gamma
\end{pmatrix}
$$
That leaves me with three equations
$$
-\frac{i}{\sqrt{2}} \beta = \alpha$$
$$
\frac{i}{\sqrt{2}} \alpha - \frac{i}{\sqrt{2}}\gamma = \beta$$
$$
\frac{i}{\sqrt{2}} \beta = \gamma$$
I think I know how to construct the eigenspinor from these values. Is it simply
$$
\chi_{+}^y=\frac{1}{\sqrt{2}}\begin{pmatrix}
-\frac{i}{\sqrt{2}} \\ 1 \\ \frac{i}{\sqrt{2}}
\end{pmatrix}
$$?
The actual particle I'm trying to measure is in the state
$$
\chi = \frac{1}{2}
\begin{pmatrix} 1\\ i\sqrt{2}\\ -1
\end{pmatrix}
$$
but when I do the calculation, I get
$$
|\langle \chi_{+}^y|\chi\rangle|=\frac{1}{\sqrt{2}}\begin{pmatrix}
\frac{i}{\sqrt{2}}& 1& -\frac{i}{\sqrt{2}}
\end{pmatrix}\cdot \frac{1}{2}\begin{pmatrix}1\\ i\sqrt{2}\\-1
\end{pmatrix} =1
$$
What am I doing wrong?
I get
$$
S_y=\frac{i\hbar}{\sqrt{2}}\begin{pmatrix}
0 & -1 & 0 \\ 1 & 0 & -1 \\ 0 & 1 & 0 \\
\end{pmatrix}
$$
From what I have seen, the eigenspinor for $\hbar$ is found by solving
$$
\frac{i\hbar}{\sqrt{2}}\begin{pmatrix}
0 & -1 & 0 \\ 1 & 0 & -1 \\ 0 & 1 & 0 \\
\end{pmatrix}
\cdot
\begin{pmatrix}
\alpha \\ \beta \\ \gamma
\end{pmatrix} =
\hbar \begin{pmatrix}
\alpha \\ \beta \\ \gamma
\end{pmatrix}
$$
That leaves me with three equations
$$
-\frac{i}{\sqrt{2}} \beta = \alpha$$
$$
\frac{i}{\sqrt{2}} \alpha - \frac{i}{\sqrt{2}}\gamma = \beta$$
$$
\frac{i}{\sqrt{2}} \beta = \gamma$$
I think I know how to construct the eigenspinor from these values. Is it simply
$$
\chi_{+}^y=\frac{1}{\sqrt{2}}\begin{pmatrix}
-\frac{i}{\sqrt{2}} \\ 1 \\ \frac{i}{\sqrt{2}}
\end{pmatrix}
$$?
The actual particle I'm trying to measure is in the state
$$
\chi = \frac{1}{2}
\begin{pmatrix} 1\\ i\sqrt{2}\\ -1
\end{pmatrix}
$$
but when I do the calculation, I get
$$
|\langle \chi_{+}^y|\chi\rangle|=\frac{1}{\sqrt{2}}\begin{pmatrix}
\frac{i}{\sqrt{2}}& 1& -\frac{i}{\sqrt{2}}
\end{pmatrix}\cdot \frac{1}{2}\begin{pmatrix}1\\ i\sqrt{2}\\-1
\end{pmatrix} =1
$$
What am I doing wrong?
Last edited: