- #1
Master J
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After a fruitless search for a good undergraduate resource for Green's Functions (Economou's book is far too advanced for an intro course) , I hope someone here can clear this up.
So I have the Greens Functions (gf) for the time independent Schrodinger equation:
SUM |a><a| / (E - e(k)) where |a> form an orthonormal basis, e(k) is the particle energy. First off, for a free particle, E and e(k) are the same thing are they not? h^2.k^2/2m , so is the denominator not just zero, or is there a subtle meaning here?
Now, the more interesting part. Ok, so I have found some notes, but unfortunately they don't explain what is going on:
It takes the adove gf and adds an imaginary part to the denominator, and takes the limit that this imaginary parts goes to zero...then we get:
P ( 1 / E - e(k) ) + i(pi) DELTA( E - e(k))
where delta is the Dirac Delta function. What is this P? And how is this so? Is it just a mathematical relation??
And finally, I see that the density of states follows from this, but how is it motivated?? The result is just stated.
So I have the Greens Functions (gf) for the time independent Schrodinger equation:
SUM |a><a| / (E - e(k)) where |a> form an orthonormal basis, e(k) is the particle energy. First off, for a free particle, E and e(k) are the same thing are they not? h^2.k^2/2m , so is the denominator not just zero, or is there a subtle meaning here?
Now, the more interesting part. Ok, so I have found some notes, but unfortunately they don't explain what is going on:
It takes the adove gf and adds an imaginary part to the denominator, and takes the limit that this imaginary parts goes to zero...then we get:
P ( 1 / E - e(k) ) + i(pi) DELTA( E - e(k))
where delta is the Dirac Delta function. What is this P? And how is this so? Is it just a mathematical relation??
And finally, I see that the density of states follows from this, but how is it motivated?? The result is just stated.