Understanding LCAO Matrix Solutions for Molecules

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The discussion focuses on using Linear Combination of Atomic Orbitals (LCAO) to construct matrices for solving molecular orbitals in small molecules and delocalized pi-systems. The user seeks to expand upon Huckel theory, which is limited to conjugated pi-systems in hydrocarbons, to encompass a broader range of small molecules such as H3, HF2-, H2O, and CH4, as well as larger molecules with delocalized pi-systems, including linear and cyclic hydrocarbons and crown ethers. The challenge lies in generalizing these concepts while maintaining accuracy. Suggestions for further reading include extended Huckel theory and resources like a specific paper by Roald Hoffmann and the free software program Yaehmop, which can aid in this exploration.
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I would like to understand how LCAO may be used to construct the matrix to be solved for the molecular orbitals of two cases of molecules:

1) small molecules like H3 (or H3+, HF2-, H2O, CH4, etc.
2) groups or parts of molecules with delocalized pi-systems (including linear and cyclic hydrocarbons, crown ethers, carboxylate ions, etc.)

Huckel theory instruction is readily available, but it is only supposed to apply to the case of conjugated pi-systems in hydrocarbons, i.e. a special case of part 2 of what I'm looking for.

I wish to generalize this, to all very small molecules like the ones I listed, and also to delocalized pi-systems (within the framework of arbitrary larger molecules, which I presume need not be considered to affect that system much).

Can anyone suggest where I should read or look (Internet sources are welcome too) to find this explanation laid out?
 
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