In the ATK Reference (
http://quantumwise.com/documents/manuals/latest/ReferenceManual/index.html/chap.atkse.html#sect1.atkse.intro) the shape of the orbitals used within the Hückel-Method is given as
Therein n, l and m are the principal, angular and magnetic qunatum numbers, respectivley:
1s : n=1, l=0, m=0
2s : n=2, l=0, m=0
2p : n=2, l=1, m=-1,0,1
3s : n=3, l=0, m=0
3p : n=3, l=1, m=-1,0,1
3d : n=3, l=2, m=-2,-1,0,1,2
...
The radial part R_nl(r) is given as a superposition of two (double zeta) Slater type orbitals (STOs):
The constants C1, C2, eta1, eta2 are the orbital weights and slater coefficients fitted by different authors and tabulated within the ATK-manual.
My question is now: why does the radial part depend on the angular momentum? In literature I often see STOs (here only single zeta for simplicity) of the form:
R_n(r) = N*r^(n-1)*exp(-eta*r)
with
N={ ( [2eta]^[2n+1] ) / (2n)! }^(1/2) .
The difference is the missing
r^-l and a square root on some prefactors (
N={...}^(1/2)).
By using the Cerda carbon graphite parameters of the 2p orbitals as an example (as given in a paper of Cerda and also in the ATK reference), I calculated the integral over
Conjugate[phi]*phi (
phi being the whole orbital, including the spherical harmonics) and found out, that only by dropping the angular dependency and including the mentioned square roots, the orbitals are normalized.
Any comments would be highly recommended, as I want to plot the orbitals I'm using and I want to be sure that everything is OK.
Thanks.