Quantum Mechanics - Two spin 1/2 particles

[Tangent87]

How do we show that the state |\chi>=\frac{1}{\sqrt{2}}(|\uparrow>|\downarrow>-|\downarrow>|\uparrow>) has total spin zero? Does it involve acting some combination of the spin operators on it?

I know that the total spin operator \underline{S^2}=S_x^2+S_y^2+S_z^2=\frac{3\hbar^2}{4}I where I is the 2x2 identity matrix but I don't see how that helps.

 

[arkajad]

For two particles you should use

S_{12}=S_1\otimes S_2

For each spin component. So, for S_z it will be easy. For S^2_x+S^2_y you play with S_x+iS_y[/tex] and its conjugate, their commutations with S_z, or you can play with the explicit form of states and matrices.

 

[Dickfore]

Act on it with the operator:

<br /> \hat{S}^{2} = \hat{S}^{2}_{1} + \hat{S}^{2}_{2} + 2 (\hat{\mathbf{S}}_{1} \cdot \hat{\mathbf{S}}_{2})<br />

and express the dot product with the ladder operators:

<br /> (\hat{\mathbf{S}}_{1} \cdot \hat{\mathbf{S}}_{2}) = \hat{S}_{1 x} \hat{S}_{2 x} + \hat{S}_{1 y} \hat{S}_{2 y} + \hat{S}_{1 z} \hat{S}_{2 z}<br />
<br /> = \frac{1}{4} \left[\left(\hat{S}_{1 +} + \hat{S}_{1 -}\right) \left(\hat{S}_{2 +} + \hat{S}_{2 -}\right) - \left(\hat{S}_{1 +} - \hat{S}_{1 -}\right) \left(\hat{S}_{2 +} - \hat{S}_{2 -}\right)\right] + \hat{S}_{1 z} \hat{S}_{2 z}<br />
<br /> = \frac{1}{2} \left(\hat{S}_{1 +} \hat{S}_{2 -} + \hat{S}_{1 -} \hat{S}_{2 +}\right) + \hat{S}_{1 z} \hat{S}_{2 z}<br />

You should get:

<br /> \hat{S}^{2} |\chi\rangle = S (S + 1) |\chi\rangle<br />

What value for S do you get?

 

[Tangent87]

Thank you for your help, I get \hat{S}^{2} |\chi\rangle = 0, I take it that's correct as it's supposed to be a state of total spin 0? Is there no easier way to do it though as it took quite a bit of work and I see the result stated in so many textbooks as if it's obvious?

 

[Dickfore]

There is, through the use of Young tableaux.