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				<datestamp>2025-12-31T07:17:19Z</datestamp>
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	<dc:title xml:lang="en-US">Unified formulae for augmented near orthonormalized STO-kG (1s, …, 4f) basis sets via atomic orbital energy fit with graphical representations to use in molecular structure calculations</dc:title>
	<dc:creator>Kristyan, Sandor</dc:creator>
	<dc:subject xml:lang="en-US">Ab initio calculations</dc:subject>
	<dc:subject xml:lang="en-US">Computational chemistry</dc:subject>
	<dc:subject xml:lang="en-US">Unified STO-kG basis sets</dc:subject>
	<dc:subject xml:lang="en-US">Molecular structure calculations</dc:subject>
	<dc:subject xml:lang="en-US">STO-kG(3d and 4f) basis functions</dc:subject>
	<dc:subject xml:lang="en-US">Recursive formulae for overlap molecular integrals</dc:subject>
	<dc:description xml:lang="en-US">STO-kG type (linear combination of k Gaussians) basis functions for 1s to 4f Hydrogen-like orbitals by ‘energy fit’ are reported as simple functions of the atomic number Z and quantum numbers to utilize in molecular electronic structure calculations. We analyze how they reproduce the one-electron atomic wave function shapes and energy values (-Z2/(2n2)) as an obvious primary claim along with reproducing the nodes exactly. The literature STO-kG yields a huge number of tables for different atoms in the periodic table; in contrast, our sets contain Z as a parameter yielding a compact list. A ‘variation-like’ property is also discussed for excited states (2s and up). The optimizations have been done by using least squares fits via the Lagrange multiplier method for energy with a constraint for normalization. All these STO-kG basis functions are normalized exactly to one in our tables. The general problem of STO-kG(3 and 4du^2) and STO-kG(4fu^3 and 4fuv^2) basis functions among the six technical 3duv as well as the ten technical 4f used in practice is commented on. In relation and comparison, the Gaussian package STO-kG basis set is commented on.</dc:description>
	<dc:publisher xml:lang="en-US">Atlanta Publishing House LLC</dc:publisher>
	<dc:date>2025-12-31</dc:date>
	<dc:type>info:eu-repo/semantics/article</dc:type>
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	<dc:identifier>https://www.eurjchem.com/index.php/eurjchem/article/view/2711</dc:identifier>
	<dc:identifier>10.5155/eurjchem.16.4.382-394.2711</dc:identifier>
	<dc:source xml:lang="en-US">European Journal of Chemistry; Vol. 16 No. 4 (2025): December 2025; 382-394</dc:source>
	<dc:source>2153-2257</dc:source>
	<dc:source>2153-2249</dc:source>
	<dc:language>eng</dc:language>
	<dc:relation>https://www.eurjchem.com/index.php/eurjchem/article/view/2711/2985</dc:relation>
	<dc:rights xml:lang="en-US">Copyright (c) 2025 Sandor Kristyan</dc:rights>
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