"Einstein field equation"의 두 판 사이의 차이

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2번째 줄: 2번째 줄:
  
 
* prerequiste : Riemann tensor, the Ricci tensor, and the Ricci scalar
 
* prerequiste : Riemann tensor, the Ricci tensor, and the Ricci scalar
 +
*  relativistic matter field equation<br><math>R_{\mu \nu} - {1 \over 2}g_{\mu \nu}\,R + g_{\mu \nu} \Lambda = {8 \pi G \over c^4} T_{\mu \nu}</math><br> where R_{\mu \nu}\, is the Ricci curvature tensor, R\, the scalar curvature,,  <math>\Lambda</math> is the [[cosmological constant]]<br>
  
 
 
 
 
 
 
 
 
relativistic matter field equation
 
 
<math>R_{\mu \nu} - {1 \over 2}g_{\mu \nu}\,R + g_{\mu \nu} \Lambda = {8 \pi G \over c^4} T_{\mu \nu}</math>
 
 
where R_{\mu \nu}\, is the Ricci curvature tensor, R\, the scalar curvature,,  <math>\Lambda</math> is the [[cosmological constant]]
 
  
 
 
 
 
29번째 줄: 22번째 줄:
 
<h5 style="line-height: 2em; margin: 0px;">equation of motion</h5>
 
<h5 style="line-height: 2em; margin: 0px;">equation of motion</h5>
  
 
+
* http://en.wikipedia.org/wiki/Einstein%E2%80%93Hilbert_action#Derivation_of_Einstein.27s_field_equations<br>
 
 
 
 
 
 
 
 
  
 
 
 
 
52번째 줄: 41번째 줄:
 
* [[differential geometry and topology]]
 
* [[differential geometry and topology]]
 
* [[Yang-Mills Theory(Non-Abelian gauge theory)]]
 
* [[Yang-Mills Theory(Non-Abelian gauge theory)]]
 +
* [[string theory and Einstein equations]]
  
 
 
 
 

2011년 9월 22일 (목) 08:00 판

introduction
  • prerequiste : Riemann tensor, the Ricci tensor, and the Ricci scalar
  • relativistic matter field equation
    \(R_{\mu \nu} - {1 \over 2}g_{\mu \nu}\,R + g_{\mu \nu} \Lambda = {8 \pi G \over c^4} T_{\mu \nu}\)
    where R_{\mu \nu}\, is the Ricci curvature tensor, R\, the scalar curvature,,  \(\Lambda\) is the cosmological constant

 

 

 

Einstein-Hilbert action

\(S= - {1 \over 2\kappa}\int R \sqrt{-g} \, d^4x \\)

\(\kappa = {8 \pi G \over c^4} \)

 

 

equation of motion

 

 

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