5,849
edits
(→Proposed Solution: and -> an) |
|||
Line 22: | Line 22: | ||
{| class="wikitable" | {| class="wikitable" | ||
| '''1.''' The Arena ( | | '''1.''' The Arena (\( X, g_{\mu\nu}\)) | ||
| | | \(R_{\mu\nu} - \frac{1}{2} Rg_{\mu\nu} + \Lambda g_{\mu\nu} = \left( \dfrac{8 \pi G}{c^4} T_{\mu\nu}\right)\) | ||
| the Einstein field equations, which describe gravity in the theory of general relativity | | the Einstein field equations, which describe gravity in the theory of general relativity | ||
|- | |- | ||
| '''2.''' | | '''2.''' \(G\) (non abelian) | ||
\( SU(3) \times SU(2) \times U(1)\) | |||
| | | \(d_A^*F_A=J(\psi)\) | ||
| the Yang-Mills equation, which governs all other force fields in Yang-Mill-Maxwell theory | | the Yang-Mills equation, which governs all other force fields in Yang-Mill-Maxwell theory | ||
|- | |- | ||
| '''3.''' Matter | | '''3.''' Matter | ||
Antisymmetric, therefore light | Antisymmetric, therefore light | ||
| | | \((i \hbar \gamma^\mu \partial_\mu - m) \psi = 0\) | ||
| the Dirac equation, the equation of motion describing matter particles, or fermions | | the Dirac equation, the equation of motion describing matter particles, or fermions | ||
|} | |} |