- #1
riclambo
- 7
- 0
Hello Forum,
This is my first post. There is some preamble, but the problem itself is straightforward enough, even though I cannot solve it.
I'm trying to calculate the spin orbit matrix for an alkali metal atom at the centre of a complex of 12 noble gas atoms which form a tetradecahedron. The basis set consists of the metal atom excited state p orbitals plus the excited state rare gas (n + 1) p orbitals. The metal atom p orbitals (of [tex]t_{1u}[/tex] symmetry in [tex]O_h[/tex]) mix with the [tex]t_{1u}[/tex] rare gas cage atom group orbitals. The cage group orbitals are then:
[tex]t^{1}_{1u}(x): x_{2}+x_{3}+x_{6}+x_{8}[/tex]
[tex]t^{1}_{1u}(y): y_{1}+y_{3}+y_{5}+y_{7}[/tex]
[tex]t^{1}_{1u}(z): z_{9}+z_{10}+z_{11}+z_{12}[/tex]
[tex]t^{2}_{1u}(x): -(x_{1}+x_{3}+x_{5}+x_{7}+x_{9}+x_{10} +x_{11}+x_{12})[/tex]
[tex]t^{2}_{1u}(y): -(y_{2}+y_{4}+y_{6}+y_{8}+y_{9}+y_{10}+y_{11}+y_{12})[/tex]
[tex]t^{2}_{1u}(z): -(z_{1}+z_{2}+z_{3}+z_{4}+z_{5}+z_{6}+z_{7}+z_{8})[/tex]
[tex]t^{3}_{1u}(x): z_{1}-z_{3}-z_{5}+z_{7}+y_{9}-y_{10}+y_{11}-y_{12}[/tex]
[tex]t^{3}_{1u}(y): -z_{2}+z_{4}+z_{6}-z_{8}+x_{9}-x_{10}+x_{11}-x_{12}[/tex]
[tex]t^{3}_{1u}(z): x_{1}-x_{3}-x_{5}+x_{7}-y_{2}+y_{4}+y_{6}-y_{8}[/tex]
The LCAO-MOs are then:
[tex]\varphi(x) = c_{1}p^{M}_{x}+c_{2}t^{1}_{1u}(x)+c_{3}t^{2}_{1u}(x)+c_{4}t^{3}_{1u}(x) [/tex]
[tex]\varphi(y) = c_{1}p^{M}_{y}+c_{2}t^{1}_{1u}(y)+c_{3}t^{2}_{1u}(y)+c_{4}t^{3}_{1u}(y) [/tex]
[tex]\varphi(z) = c_{1}p^{M}_{z}+c_{2}t^{1}_{1u}(z)+c_{3}t^{2}_{1u}(z)+c_{4}t^{3}_{1u}(z) [/tex]
Here the superscripts M, I, 2, and 3 refer to the metal and different rare gas group orbitals, respectively. The elements of the spin-orbit matrix have the form:
[tex]\left\langle \varphi(i)\eta \left|H_{SO}\right| \varphi(j)\eta'\right\rangle [/tex]
where
[tex]\eta[/tex] and [tex] \eta'[/tex] are the spin functions.
[tex]H_{SO} = \zeta_{M}l_{M}.s + \zeta_{X}\sum l_{k}.s[/tex]
where
[tex]\zeta_{M}[/tex]
and
[tex]\zeta_{X}[/tex]
are the metal and rare gas SO coupling constants. The sum is over all rare gas atom centers and makes use of the standard angular momentum operator relations. The final results looks like:
A*(Matrix of 1s and 0s)
where
[tex]A = h^{2}(c^{2}_1\zeta_{M} - 4c_1c_2\zeta_{X}S_1 -4c_1c_2\zeta_{X}S_{\pi}+ 4c_1c_3\zeta_{X}S_1 - 4c_1c_4\zeta_{X}S_2+4c_1c_2\zeta_{M}S_{\pi}+8c_1c_3\zeta_{M}S_1+8c_1c_3\zeta_{M}S_2)/8{\pi}[/tex]
[tex]S_1 = \left\langle p^{M}_{z}\left|-z_1 \right\rangle[/tex]
[tex]S_2 = \left\langle p^{M}_{z}\left|y_4 \right\rangle[/tex]
[tex]S_{\pi} = \left\langle p^{M}_{z}\left|z_9 \right\rangle[/tex]
The article I have attached gives more details and the result on page 3, which looks like a fairly simple expression. I have seen this kind of problem for tetrahedral and octahedral complexes but never for a tetradecahedral complex. Although I can derive some of its terms, I cannot arrive at the final form. If there are any physical chemists or chemical physicists out there, could you please give this 30 minutes of your time, even if it is just to point me to a more helpful reference.
Regards,
Ricardo
This is my first post. There is some preamble, but the problem itself is straightforward enough, even though I cannot solve it.
I'm trying to calculate the spin orbit matrix for an alkali metal atom at the centre of a complex of 12 noble gas atoms which form a tetradecahedron. The basis set consists of the metal atom excited state p orbitals plus the excited state rare gas (n + 1) p orbitals. The metal atom p orbitals (of [tex]t_{1u}[/tex] symmetry in [tex]O_h[/tex]) mix with the [tex]t_{1u}[/tex] rare gas cage atom group orbitals. The cage group orbitals are then:
[tex]t^{1}_{1u}(x): x_{2}+x_{3}+x_{6}+x_{8}[/tex]
[tex]t^{1}_{1u}(y): y_{1}+y_{3}+y_{5}+y_{7}[/tex]
[tex]t^{1}_{1u}(z): z_{9}+z_{10}+z_{11}+z_{12}[/tex]
[tex]t^{2}_{1u}(x): -(x_{1}+x_{3}+x_{5}+x_{7}+x_{9}+x_{10} +x_{11}+x_{12})[/tex]
[tex]t^{2}_{1u}(y): -(y_{2}+y_{4}+y_{6}+y_{8}+y_{9}+y_{10}+y_{11}+y_{12})[/tex]
[tex]t^{2}_{1u}(z): -(z_{1}+z_{2}+z_{3}+z_{4}+z_{5}+z_{6}+z_{7}+z_{8})[/tex]
[tex]t^{3}_{1u}(x): z_{1}-z_{3}-z_{5}+z_{7}+y_{9}-y_{10}+y_{11}-y_{12}[/tex]
[tex]t^{3}_{1u}(y): -z_{2}+z_{4}+z_{6}-z_{8}+x_{9}-x_{10}+x_{11}-x_{12}[/tex]
[tex]t^{3}_{1u}(z): x_{1}-x_{3}-x_{5}+x_{7}-y_{2}+y_{4}+y_{6}-y_{8}[/tex]
The LCAO-MOs are then:
[tex]\varphi(x) = c_{1}p^{M}_{x}+c_{2}t^{1}_{1u}(x)+c_{3}t^{2}_{1u}(x)+c_{4}t^{3}_{1u}(x) [/tex]
[tex]\varphi(y) = c_{1}p^{M}_{y}+c_{2}t^{1}_{1u}(y)+c_{3}t^{2}_{1u}(y)+c_{4}t^{3}_{1u}(y) [/tex]
[tex]\varphi(z) = c_{1}p^{M}_{z}+c_{2}t^{1}_{1u}(z)+c_{3}t^{2}_{1u}(z)+c_{4}t^{3}_{1u}(z) [/tex]
Here the superscripts M, I, 2, and 3 refer to the metal and different rare gas group orbitals, respectively. The elements of the spin-orbit matrix have the form:
[tex]\left\langle \varphi(i)\eta \left|H_{SO}\right| \varphi(j)\eta'\right\rangle [/tex]
where
[tex]\eta[/tex] and [tex] \eta'[/tex] are the spin functions.
[tex]H_{SO} = \zeta_{M}l_{M}.s + \zeta_{X}\sum l_{k}.s[/tex]
where
[tex]\zeta_{M}[/tex]
and
[tex]\zeta_{X}[/tex]
are the metal and rare gas SO coupling constants. The sum is over all rare gas atom centers and makes use of the standard angular momentum operator relations. The final results looks like:
A*(Matrix of 1s and 0s)
where
[tex]A = h^{2}(c^{2}_1\zeta_{M} - 4c_1c_2\zeta_{X}S_1 -4c_1c_2\zeta_{X}S_{\pi}+ 4c_1c_3\zeta_{X}S_1 - 4c_1c_4\zeta_{X}S_2+4c_1c_2\zeta_{M}S_{\pi}+8c_1c_3\zeta_{M}S_1+8c_1c_3\zeta_{M}S_2)/8{\pi}[/tex]
[tex]S_1 = \left\langle p^{M}_{z}\left|-z_1 \right\rangle[/tex]
[tex]S_2 = \left\langle p^{M}_{z}\left|y_4 \right\rangle[/tex]
[tex]S_{\pi} = \left\langle p^{M}_{z}\left|z_9 \right\rangle[/tex]
The article I have attached gives more details and the result on page 3, which looks like a fairly simple expression. I have seen this kind of problem for tetrahedral and octahedral complexes but never for a tetradecahedral complex. Although I can derive some of its terms, I cannot arrive at the final form. If there are any physical chemists or chemical physicists out there, could you please give this 30 minutes of your time, even if it is just to point me to a more helpful reference.
Regards,
Ricardo