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equations:klein-gordon_equation [2017/10/21 15:23]
jakobadmin [Student]
equations:klein-gordon_equation [2021/03/31 18:22] (current)
edi [Concrete]
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-====== Klein-Gordon Equation ======+<WRAP lag>​$ ​ ( \partial _{\mu} \partial ^{\mu}+m^2)\Phi ​0 $</​WRAP>​
-<tabbox Why is it interesting?> ​+====== Klein-Gordon Equation ​  ​======
-<note tip>​It'​s the correct equation of motion that describes free [[basic_notions:​spin|spin]] $1$ particles. +<tabbox Intuitive
-<tabbox Layman> ​+The Klein-Gordon equation describes how the state of a relativistic (= fast moving) quantum system without spin changes in time. 
 +The analogous equation for systems with half-integer spin is the [[equations:​dirac_equation|]]. 
 +If the system only moves slowly, the Klein-Gordon equation becomes the [[equations:​schroedinger_equation]]. ​
-<note tip> 
-Explanations in this section should contain no formulas, but instead colloquial things like you would hear them during a coffee break or at a cocktail party. 
   ​   ​
-<​tabbox ​Student+<​tabbox ​Concrete 
 +The Klein-Gordon equation can be derived from the Lagrangian 
 +\begin{equation} \mathscr{L}= \frac{1}{2}( \partial _{\mu} \Phi \partial ^{\mu} \Phi -m^2 \Phi^2) \end{equation} 
 +using the [[equations:​euler_lagrange_equations|Euler-Lagrange equations]]. 
 +The most general solution of the Klein-Gordon equation is\begin{equation}\label{KGsol} \Phi(x)= \int \mathrm{d }k^3 \frac{1}{(2\pi)^3 2\omega_k} \left( a(k){\mathrm{e }}^{ -i(k x)} + a^\dagger(k) {\mathrm{e }}^{ i(kx)}\right) .\end{equation} 
 +  * A nice discussion can be found in [[http://​​website_Chap03.pdf |chapter 3 of Klauber'​s Student Friendly QFT book]] 
 +  * For an elementary derivation of the Klein-Gordon equation see Physics from Symmetry by Schwichtenberg 
 +**Graphical Summary** 
 +The diagram below shows the Klein-Gordon equation and its Lagrangian in various forms. For a more detailed explanation see [[https://​​|Fun with Symmetry]]. ​
-  *   * For an elementary derivation of the Klein-Gordon equation see Physics from Symmetry by Schwichtenberg+{{:​equations:​klein_gordon.jpg?​nolink}}
-<​tabbox ​Researcher+<​tabbox ​Abstract
 <note tip> <note tip>
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 </​note>​ </​note>​
---Common Question 1#+<tabbox Why is it interesting?​
-  +The Klein-Gordon equation is the correct equation of motion that describes free [[basic_notions:​spin|spin]] $0$ particles. For a spin-1 generalization see the Duffin-Kemmer-Petiau equation.
---> Common Question 2# 
   ​   ​
-<​tabbox ​Examples+<​tabbox ​Definitions
---> Example1# 
-  +  * $\partial _{\mu} $ denotes the partial derivative and $\partial _{\mu} \partial ^{\mu}$ stands for a sum using the Einstein sum convention, i.e. $\partial _{\mu} \partial ^{\mu} =  \partial _0 \partial^0 - \partial _1 \partial^1 -\partial _2 \partial^2 -\partial _3 \partial^3$,​ 
-<--+  * $m$ denotes the mass of the particle, 
 +  * $\Phi$ describes the spin $0$ field if we work in a field theory.  
 +  * Note: $\Phi$ cannot be interpreted as a wavefunction because it is a real valued field; it is its own anti-particle like the Majorana fermion. Only in the case that it is the U(1)-charged (requires 2 independent real Klein Gordon fields that are symmetry transform into each other) is a naive wavefunction interpretation possible. Basically, you get a relativistic scalar superfluid field. Nevertheless,​ there are single particle wavefunctions lurking in the single real Klein-Gordon theory. But you need to use the coherent state representation to see the 1st quantized operators from the complex annihilation and creation operators. Essentially undoing the second quantization. ​
---> Example2:# 
-  ​ 
-<tabbox History> ​ 
 </​tabbox>​ </​tabbox>​
equations/klein-gordon_equation.1508592190.txt.gz · Last modified: 2017/12/04 08:01 (external edit)