Difference between revisions of "Uemoto Testpage"
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| − | + | ==This is test page of MediaWiki== | |
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| + | === Time Dependent Kohn-Sham Equation === | ||
<math> | <math> | ||
i \hbar | i \hbar | ||
| − | \frac{\partial | + | \frac{\partial}{\partial t} |
| + | u_{n, k} | ||
= | = | ||
| − | \ | + | \left[ |
| − | \ | + | \frac{1}{2m} \left( |
| + | {p}^2 | ||
| + | + | ||
| + | \frac{e}{c}{{A}} | ||
| + | \right) | ||
| + | + | ||
| + | V_\mathrm{H} | ||
| + | + | ||
| + | V_\mathrm{XC} | ||
| + | + | ||
| + | V_\mathrm{nucl} | ||
| + | \right] | ||
| + | u_{n,k} | ||
</math> | </math> | ||
| + | |||
| + | - <math> u_nk </math> is the Kohn-Sham orbital. | ||
| + | |||
| + | - <math> A </math> is the vector potential. | ||
Latest revision as of 18:55, 7 June 2017
This is test page of MediaWiki
- The first line
- Second line
- Third line
Time Dependent Kohn-Sham Equation
[math] i \hbar \frac{\partial}{\partial t} u_{n, k} = \left[ \frac{1}{2m} \left( {p}^2 + \frac{e}{c}{{A}} \right) + V_\mathrm{H} + V_\mathrm{XC} + V_\mathrm{nucl} \right] u_{n,k} [/math]
- [math] u_nk [/math] is the Kohn-Sham orbital.
- [math] A [/math] is the vector potential.
