Landau Energy Spectrum in the non-relativistic limit

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In the non-relativistic limit, the relationship between mass (m), momentum (p), and energy (E) is explored, highlighting that m is significantly greater than both p and the angular frequency (w). By factoring out m^2 from the square root, the energy expression simplifies to E = m + w(n + 1/2). However, this leads to a discrepancy with the expected form E = p^2/2m + w(n + 1/2). The discussion emphasizes the importance of not setting p to zero prematurely, as it obscures the dependency on momentum. Understanding these transformations is crucial for accurately deriving energy expressions in quantum mechanics.
desperate_student
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Homework Statement
In the relativistic landau energy spectrum for a particle in a magnetic field, how does the m^2 term simplify down to p^2/2m in the non-relativistic limit?
Relevant Equations
Non-Relativistic: E=p^2/2m +w(n+1/2), n=0,1,2....
Relativistic: E= sqrt(p^2 +m^2+2mw(n+1/2)) n=0,1,2....
At non-relativistic limit, m>>p so let p=0
At non-relativistic limit m>>w,
So factorise out m^2 from the square root to get:
m*sqrt(1+2w(n+1/2)/m)
Taylor expansion identity for sqrt(1+x) for small x gives:
E=m+w(n+1/2) but it should equal E=p^2/2m +w(n+1/2), so how does m transform into p^2/2m?
 
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desperate_student said:
At non-relativistic limit, m>>p so let p=0
If you set p=0, it should be obvious that you will not get an equation that depends on p. So try it again without doing that.
 
I want to find the solution to the integral ##\theta = \int_0^{\theta}\frac{du}{\sqrt{(c-u^2 +2u^3)}}## I can see that ##\frac{d^2u}{d\theta^2} = A +Bu+Cu^2## is a Weierstrass elliptic function, which can be generated from ##\Large(\normalsize\frac{du}{d\theta}\Large)\normalsize^2 = c-u^2 +2u^3## (A = 0, B=-1, C=3) So does this make my integral an elliptic integral? I haven't been able to find a table of integrals anywhere which contains an integral of this form so I'm a bit stuck. TerryW

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