Klein-gordon Equation

The Klein-Gordon equation (Klein-Fock-Gordon equation or sometimes Klein-Gordon-Fock equation) is a relativistic version (describing scalar (or pseudoscalar) spinless particles) of the Schrdinger equation. The Schrdinger equation for a free particle is
\frac{\hat{\vec{p}}^2}{2m} \psi = i \frac{\partial}{\partial t}\psi where \hat{\vec{p}} = -i\nabla is the momentum operator, using natural units where \hbar=c=1. The Schrdinger equation suffers from not being relativistically covariant, meaning it does not take into account Einstein's special theory of relativity. It is natural to try to use the identity from special relativity
E = \sqrt{p^2 + m^2} for the energy; then, just inserting the quantum mechanical momentum operator, yields the equation
\sqrt{(-i\nabla)^2 + m^2} \psi= i \frac{\partial}{\partial t}\psi This, however, is a cumbersome expression to work with because of the square root. Cumbersomeness, however, doesn't really count as an objection. But this equation, as it stands, is nonlocal. Klein and Gordon instead worked with the square of this equation (the Klein-Gordon equation for a free particle), which in covariant notation reads
(\partial^2 + m^2) \psi = 0. The Klein-Gordon equation was actually first found by Schrdinger, before he made the discovery of the equation that now bears his name. He rejected it because he couldn't make it fit data (the equation doesn't take into account the spin of the electron); the way he found his equation was by making simplifications in the Klein-Gordon equation. The Klein-Gordon equation may also be derived out of purely information-theoretic considerations. See extreme physical information. In 1926, soon after the Schrdinger equation was introduced, Fock wrote an article about its generalization for the case of magnetic fields, where forces were dependent on velocity, and independently derived this equation. Both Klein and Fock used Kaluza and Klein's method. Fock also determined the gauge theory for the wave equation. The Klein-Gordon equation for a free particle has a simple plane wave solution.

External links

 

<< PreviousWord BrowserNext >>
the knack
qed project
dbase
nim li punit
pride's purge
coalsack nebula
the assassin
rump parliament
enewetak
19th century philosophy
sam (spynet)
pendleton
atomic age
brampton arts council
theatre brampton
samuel french playwrights competition
a year in the death of eddie jester
elizabeth macleod
a chinese ghost story part ii
phoumi vongvichit
tv tome
jenniferjohn and britneybob
tail man
jarmo pohjaniemi
heather christensen
deputy
early history of laos
margaret matson
sibley monroe checklist 1
star of david
thai yuan
sibley monroe checklist 2
arthur erickson
list of u.s. televangelists
kong le
brooke family
charles sibley
goldfinger (band)
vladimir vapnik
ouane rattikone
25 pounder short mark 1
harriette chick
khamphoui
kouprasith abhay