"Klein-Gordon equation"의 두 판 사이의 차이

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<h5>introduction</h5>
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* [[클라인-고든_방정식]]
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==introduction==
  
* free massive scalar field which describes the spin-0 particles
 
 
* in condensed matter physics it describes long wavelength optical phonons
 
* in condensed matter physics it describes long wavelength optical phonons
* formulated as a relativistic generalization of Schrodinger equation
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*  there are real KG equation and complex KG equation
*  there are real KG equation and complex KG equation<br>
 
 
** real case describes electrically neutral particles
 
** real case describes electrically neutral particles
** complex case describes charged particles
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** complex case describes charged particles
 
* <math>(\Box + m^2) \psi = 0</math> i.e. <math>(\Box + m^2) \psi =\psi_{tt}-\psi_{xx}-\psi_{yy}-\psi_{zz}+m^2\psi=0</math>
 
* <math>(\Box + m^2) \psi = 0</math> i.e. <math>(\Box + m^2) \psi =\psi_{tt}-\psi_{xx}-\psi_{yy}-\psi_{zz}+m^2\psi=0</math>
*  people found 2 problems of KG equations<br>
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*  correct interpretations of <math>\phi</math> requires the idea of quantum field rather than the particle wavefunction
** negative energy states
 
** negative probability density
 
*  correct interpretations of <math>\phi</math> requires the idea of quantum field rather than the particle wavefunction<br>
 
 
** negative probability density -> charge density
 
** negative probability density -> charge density
*  Dirac suggested Dirac sea by invoking the exclusion principle and then KG equation only applicable to spinless particles<br>
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*  Dirac suggested Dirac sea by invoking the exclusion principle and then KG equation only applicable to spinless particles
** for example, <math>\pi</math>-meson
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** for example, <math>\pi</math>-meson
* Thus the Dirac equation comes in to deal with spin-<math>1/2</math> particles.
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* Thus the Dirac equation comes in to deal with spin-<math>1/2</math> particles.
 
 
 
 
 
 
 
 
 
 
<h5>plane wave solutions</h5>
 
 
 
* <math>u(x,t)=Ae^{i(kx-\omega t)}</math>
 
 
 
 
 
 
 
 
 
 
 
<h5>Lorentz invariant commutation relation</h5>
 
  
 
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<h5>history</h5>
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==Lorentz invariant commutation relation==
  
* http://www.google.com/search?hl=en&tbs=tl:1&q=
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<h5>related items</h5>
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==related items==
  
 
* [[special and general relativity]]
 
* [[special and general relativity]]
 
* [[sine-Gordon equation]]
 
* [[sine-Gordon equation]]
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[[분류:physics]]
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[[분류:math and physics]]
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[[분류:QFT]]
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[[분류:migrate]]

2020년 12월 28일 (월) 04:16 기준 최신판



introduction

  • in condensed matter physics it describes long wavelength optical phonons
  • there are real KG equation and complex KG equation
    • real case describes electrically neutral particles
    • complex case describes charged particles
  • \((\Box + m^2) \psi = 0\) i.e. \((\Box + m^2) \psi =\psi_{tt}-\psi_{xx}-\psi_{yy}-\psi_{zz}+m^2\psi=0\)
  • correct interpretations of \(\phi\) requires the idea of quantum field rather than the particle wavefunction
    • negative probability density -> charge density
  • Dirac suggested Dirac sea by invoking the exclusion principle and then KG equation only applicable to spinless particles
    • for example, \(\pi\)-meson
  • Thus the Dirac equation comes in to deal with spin-\(1/2\) particles.



Lorentz invariant commutation relation

related items