H atom electron in combined spin/position state

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Homework Statement


An electron in a H atom occupies the combined spin and position state: R21{(sqrt(1/3)Y10χ+) + (sqrt(2/3)Y11χ-)} If you measured both the z component of spin and the distance from the origin, what is the probability density for finding the particle with spin up and at radius r?


Homework Equations





The Attempt at a Solution



The answer should just be |R21|^2*(1/3)*|Y10|^2*|χ+|^2 = (r^2)/(96πa^5) * exp(-r/a) * (cosθ)^2, right? Or do I need to do an integral? The theta dependence of my answer is bugging me, but I'm not entirely sure if I need to integrate over theta and phi to just get an r dependent answer? Could somebody please help me think through this? Thanks very much.
 
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If the question just asks for "radius r", then, yes, you do have to integrate out the theta and phi dependence.
 
Sorta makes sense, but if the probability density is not isotropic in theta, it still seems wrong to me to integrate that dependence away.
 
If you don't integrate over the angles, the expression you have doesn't give the probability density that the electron is at a distance r; it's the probability density that the electron is at a distance r, angle θ, and angle φ.
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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