Solving Klein Gordon’s equation

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SUMMARY

The discussion focuses on solving the Klein-Gordon equation using separation of variables, specifically through the assumption that the solution can be expressed as a product of functions, \(\phi(x, t) = F(x) A(t)\). The resulting equations lead to the general solution \(\phi(t,x) = (c_1 e^{kt} + c_2 e^{-kt})(c_3 e^{kx} + c_4 e^{-kx})\). Boundary conditions (BC) and initial conditions (IC) are applied to determine constants, resulting in the specific solution \(\phi(t,x) = \frac{1}{4} e^{k(t-x)} - \frac{1}{4} e^{-k(t-x)}\). The discussion concludes with a request for validation of the steps taken and guidance on determining the value of \(k\).

PREREQUISITES
  • Understanding of the Klein-Gordon equation and its significance in quantum field theory.
  • Familiarity with separation of variables as a mathematical technique.
  • Knowledge of boundary conditions (BC) and initial conditions (IC) in differential equations.
  • Proficiency in manipulating exponential functions and their derivatives.
NEXT STEPS
  • Research methods for determining the constant \(k\) in solutions of the Klein-Gordon equation.
  • Explore the implications of boundary and initial conditions on the solutions of partial differential equations.
  • Study the derivation and applications of the Klein-Gordon equation in quantum mechanics.
  • Learn about numerical methods for solving differential equations, particularly in the context of wave equations.
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Physicists, mathematicians, and students studying quantum mechanics or field theory, particularly those interested in solving differential equations related to wave phenomena.

Safinaz
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Homework Statement
I try to solve Klein Gordon’s equation for specific boundary and initial conditions
Relevant Equations
The Klein Gordon’s equation for a masses scalar is given by :
## \left( \frac{\partial^2}{\partial t^2} - \frac{\partial^2}{\partial x^2} \right) \phi (x, t) = 0 ##………(1)
My solution:

Let ## \phi (x, t) = F(x) A(t) ##, then Eq. (1) becomes

##
\frac{1}{A(t)} \frac{\partial^2}{\partial t^2} - \frac{1}{F(x)} \frac{\partial^2}{\partial x^2} = 0
##

So that : ## \frac{\partial^2}{\partial t^2} = k^2 ~A (t)##, and ## \frac{\partial^2}{\partial x^2} = k^2 ~F (x)##.

Leads to :
##
\phi(t,x) = ( c_1 e^{kt} + c_2 e^{-kt} ) ( c_3 e^{kx} + c_4 e^{-kx} )
##

Assuming BC and IC :

##
bc={\phi[t,0]==1,(D[\phi[t,x],x]/.x->Pi)==0}
##
##
ic={\phi[0,x]==0,(D[\phi[t,x],t]/.t->0)==1}
##

BC leads to ##c_3 = c_4= 1/2 ## and the IC leads to to ##c_1=- c_2= 1/2 ##.

Ending up by :
##
\phi(t,x) = \frac{1}{4} e^{k(t-x)} - \frac{1}{4} e^{-k(t-x)}……… (2)
##

So any help are these steps correct till Eq. (2) ? And how to determine ##k##?
 
Last edited:
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You just wrote down the scalar wave equation, not the Klein-Gordon equation.
 

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