Why should the quantum number m be less than equal to l.

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SUMMARY

The discussion centers on the convergence of the series derived from the recursion formula for Legendre polynomials in quantum mechanics, specifically regarding the quantum number m in relation to l. The recursion formula is given as b_{n-2} = - \frac{n^2 - m^2}{l(l+1) - (n-1)(n-2)}b_{n}, where l represents the maximum value of n for which b_n is non-zero. It is established that for the series to converge, the condition |m| ≤ l must be satisfied, ensuring that the series terminates and does not diverge. This termination is crucial as it prevents the coefficients from growing indefinitely, which would otherwise lead to divergence.

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sanalsprasad
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I was reading the following article regarding solution of wavefunction of hydrogen :
http://skisickness.com/2009/11/22/

To solve the angular part they gave the substitution of y = \sin \theta and then assumed that Y is a polynomial i.e. Y(y) = \sum b_n x^n and then arrived at the recursion formula :
b_{n-2} = - \frac{n^2 - m^2}{l(l+1) - (n-1)(n-2) }b_{n} , where l is maximum value of n for which b_n is non-zero.

Then they say that :
" There must be a minimum value of n; otherwise, the series will diverge at y=0. Given l, for the series to converge, it is necessary that |m|=l-2k, with k greater than or equal to zero and less than or equal to l/2. For even or odd l, this series gives l+1 solutions. This solution gives the eigenfunctions with both odd or both even m and l. "

I did not understand why the series converges only for this particular condition. Is it something to do with starting with b_l and then finding b_{l-2} and then b_{l-4} and so on in terms of b_l.
Thanks for help!
 
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I don't care to post the mathematical reasoning because the physical reason is easy to understand.

How can a projection of a vector on any arbitrary axis (angular momentum in the case) be larger than the magnitude of the vector?
 
sanalsprasad said:
I did not understand why the series converges only for this particular condition.

When you use that recursive formula to generate polynomials (so called Legendre polynomials), every term in the resulting polynomial has coefficient larger than 1, and the coefficients only grow when going to higher-power terms. There's no way how that kind of a series could converge unless it terminates at some point. And the series terminates only if m ≤ l (with that condition, all coefficients are zero after some term).
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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