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| | [No title] (Site not responding. Last check: 2007-10-22) |
 | | The form of \ the function is", FontSize->14], "\n ", StyleBox["V(x) = D (", FontSize->14], Cell[BoxData[ \(TraditionalForm\`e\^\(\(-2\) \[Alpha]\ \((x - x\_0)\)\)\)], FontSize->14], StyleBox[" - 2", FontSize->14], Cell[BoxData[ \(TraditionalForm\`e\^\(\(-\[Alpha]\)\ \((x - x\_0)\)\)\)], FontSize->14], StyleBox[ ")\nwhere x is the distance between the two atoms. |
 | | At long range, as x\[RightArrow]\ \[Infinity], the potential energy becomes a constant (since the interaction \ between the atoms becomes negligible) which is chosen to be the zero of the \ energy scale. |
 | | The goal of this exercise is \ to study the quantum mechanical wavefunctions for a diatomic molecule \ described by a Morse potential, first the scattering wavefunctions (or \ continuum states) corresponding to E > 0, and then the bound state \ vibrational wave functions corresponding to E |
| www-theory.chem.washington.edu /~hannes/Chem465in00/Lab3cMorse.nb (1192 words) |
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