What Is the Normalization Constant for a 2-Electron Antisymmetric Spin Function?

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Homework Statement


Given that the antisymmetric spin function for a 2 electron system is N[a1b2-a2b1], find the normalization constant N. (and by a and b I mean the alpha and beta spin states and by 1 and 2, I mean the labels on the two electrons...


Homework Equations


Normalization: 1=integral over all relevant space of (wavefunction*wavefunction)


The Attempt at a Solution


So I tried to square the spin function given, set it equal to 1, and solve for N. However, as the squared value of [a1b2-a2b1]... or what I THINK is the squared value of that, I kept on getting zero... what am I doing wrong in doing:

square of spin function=(N[a1b2-a2b1])^2
=(N^2)<a1b2-a2b1|a1b2-a2b1>
=(N^2)[<a1|a1><b2|b2>-<a1|a2><b2|b1>-<a2|a1><b1|b2>+<a2|a2><b1|b1>]

and because any sort of <a|a> is 1 and so is <b|b>, all those braket stuff are equal to 1, which overall makes the equation 0... I'm confused :(
 
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no, while <a1 b2|a1 b2> = 1, <a1 b2|a2 b1>=0
therefore you get
1= N^2 (1+0+0+1)
1= 2N^2
N = 1/sqrt(2) which is what one would expect naively.

note: the 2e- system has 4 states:
|a1 a2>,|a1 b2>,|a2 b1>,|a2 b2>
these are tensor products. eg. |a1 a2> = |a1>|a2>
 
how did you get (1+0+0+1)? I kept on getitng something like 1-1+1-1 or something that kept on cancelling all out to 0 :(
 
physgirl said:
square of spin function=(N[a1b2-a2b1])^2
=(N^2)<a1b2-a2b1|a1b2-a2b1>
=(N^2)[<a1|a1><b2|b2>-<a1|a2><b2|b1>-<a2|a1><b1|b2>+<a2|a2><b1|b1>]

and because any sort of <a|a> is 1 and so is <b|b>, all those braket stuff are equal to 1, which overall makes the equation 0... I'm confused :(

Your state

<br /> |\psi\rangle = N|\alpha_1\beta_2-\alpha_2\beta_1\rangle<br />

looks bad. Use this kind of notation instead:

<br /> |\psi\rangle = N\big(|\alpha_1\beta_2\rangle-|\alpha_2\beta_1\rangle\big)<br />

When you compute

<br /> \langle\psi|\psi\rangle<br />

don't start splitting states |\alpha_i\beta_j\rangle into sums of states |\alpha_i\rangle and |\beta_j\rangle, because that is wrong.
 
Ok, I got it now : ) but now my question is, I got to the point where N=sqrt(1/2). So can N be both positive AND negative of sqrt(1/2)?
 
physgirl said:
Ok, I got it now : ) but now my question is, I got to the point where N=sqrt(1/2). So can N be both positive AND negative of sqrt(1/2)?

In fact

<br /> N=e^{i\theta}\sqrt{1/2}<br />

are all valid normalization constants, where theta is some arbitrary constant, but the simplest \sqrt{1/2} is usually preferred.
 

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