Chem 3502 / 4502 Physical Chemistry II ( Quantum Mechanics ) 3 Credits Spring Semester 2006
نویسنده
چکیده
What is easier to notice is that, since the electron we are interested in is itself also delocalized (and not a point charge q), the total repulsion is a double integral, where we integrate over the space of the first electron the repulsion felt by the fractional charge at any point defined by the equation above that involves integrating over the space of the second electron. The result is just our old friend the Coulomb integral
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