Klein-Gordon equation for electro-magnetic field?

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Discussion Overview

The discussion revolves around the application of the Klein-Gordon equation to the electromagnetic field in vacuum, exploring whether it can be treated as a massless particle. Participants examine the similarities and differences between the Klein-Gordon equation and the electromagnetic wave equation, as well as the implications of polarization and gauge choices.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the electromagnetic field can be viewed as a massless particle described by the Klein-Gordon equation, noting that both equations may be equivalent under certain conditions.
  • Others argue that the presence of two polarizations in the electromagnetic field is a consequence of its masslessness, which aligns with the properties of the Klein-Gordon equation.
  • A participant points out that longitudinal modes allowed by the Klein-Gordon equation are not observed in practice, suggesting the need for constraints in the solutions.
  • There is a discussion about the coupling of modes in the Klein-Gordon equation compared to the Dirac equation, with some participants asserting that the two modes in the electromagnetic field can propagate independently.
  • Several participants clarify the mathematical form of the Klein-Gordon equation, with some noting typographical errors in earlier posts and discussing different definitions of the D'Alembertian operator.
  • Questions arise regarding the relationship between relativistic quantum mechanics and the dynamics of photons, with some participants asserting that there are few coincidences in physics.
  • Concerns are raised about the implications of uniform probability density in quantum mechanics versus the energy distribution in electromagnetic waves.

Areas of Agreement / Disagreement

Participants express a mix of agreement and disagreement regarding the application of the Klein-Gordon equation to the electromagnetic field, the nature of polarization, and the implications of gauge choices. The discussion remains unresolved on several technical points and interpretations.

Contextual Notes

Participants reference various definitions and forms of the Klein-Gordon equation and the D'Alembertian operator, indicating that there may be inconsistencies in notation across different texts. The discussion also highlights the dependence on gauge choices in the treatment of the electromagnetic field.

Lojzek
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Can we imagine electro-magnetic field in vakuum as a massless particle that respects
Klein-Gordon equation (instead of Electromagnetic wave equation)?
It seems to me that both equations are the same, except that the electro-magnetic field can have 2 possible polarizations (then we count them as 2 different particles?).
 
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Yes. The EM wave equation for A^\mu is the KG equation of a massless particle.
Only having two polarizations is due to the masslessness.
 
However, note that because we do not observe longitudinal modes (which are allowed by the KG eqns) you have to include a constraint into the solution.
 
but the Klein-Gordon equation is a scalar equation. Are the two modes not coupled? They propagate independently each satisfying the (massless) K-G equation?

As a comparison, there is the Dirac equation. The 4 components each individually satisfy the K-G equation as well (for free particles, that is) but they are coupled by the Dirac equation and not independent.
 
pellman said:
but the Klein-Gordon equation is a scalar equation. Are the two modes not coupled? They propagate independently each satisfying the (massless) K-G equation?

As a comparison, there is the Dirac equation. The 4 components each individually satisfy the K-G equation as well (for free particles, that is) but they are coupled by the Dirac equation and not independent.

All good and true... but you can decouple the Dirac equation by finding it's eigenspinors. This is what you do, e.g., when you perform a mode expansion of the field.

Every free relativistic field will satisfy the KG equation, as it merely expresses p^2 = m^2. Note that \mathbf{E} and \mathbf{B} also obey the massless Klein Gordon equation. I think to get the KG equation for A you need to be in the Lorenz gauge.
 
Ok. I get it. The components of A are in general coupled by the Maxwell equations. It is just by selecting a special gauge they are de-coupled.
 
Lojzek said:
Can we imagine electro-magnetic field in vakuum as a massless particle that respects
Klein-Gordon equation (instead of Electromagnetic wave equation)?
It seems to me that both equations are the same, except that the electro-magnetic field can have 2 possible polarizations (then we count them as 2 different particles?).

Out from the dunce corner with my weekly dumb question. Looked up Klein-Gordon equations in wikipedia--nothing. Looked in my McGraw-Hill encyclopedia of Physics--nothing. Kindly generalize in words, no acronyms please, what those(or that) equation(s) is about.
 
klien gordon is kind of a relativistic Schrödinger equation. it uses energy squared is equal to the (momentum times the speed of light in vaccuum) squared plus the mass squared times the speed of light in vacuum to the fourth power, i think. and turns everything into waves and operators.

the electro magnetic equations can be found by comparing maxwells equations to each other. something like the laplacian of E equals the E double dot, where E is the electric field.

or something
 
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Normouse said:
Out from the dunce corner with my weekly dumb question. Looked up Klein-Gordon equations in wikipedia--nothing. Looked in my McGraw-Hill encyclopedia of Physics--nothing. Kindly generalize in words, no acronyms please, what those(or that) equation(s) is about.

\partial^\mu \partial_\mu \psi + m \psi^2 == 0
 
  • #11
Genneth made a small typo - it should read

\partial^\mu \partial_\mu \psi + m^2 \psi == 0

or

(\square^2 + \mu^2)\psi = 0

[nrqed- you're too quick - I'm still editing - d*mn latex. It depends on your definition of \square]
 
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  • #12
Mentz114 said:
Genneth made a small typo - it should read

\partial^\mu \partial_\mu \psi + m^2 \psi == 0

or

(\Box^2 + \mu^2)\psi = 0

Mentz made a very minor typo: there is no exponent of two on \Box
:wink:
 
  • #13
nrqed - for me

\square^2 \equiv -\frac{d^2}{dt^2} + \nabla^2
 
  • #14
Mentz114 said:
nrqed - for me

\square^2 \equiv -\frac{d^2}{dt^2} + \nabla^2

Ok. It's just that I have never seen this definition used in any book so it's not the standard definition, as far as I know. But I may be wrond and if you know of any book using that notation I would be interested to know.

Regards
 
  • #15
nrqed,

it's true it is used differently in various texts. Itzykson&Zuber use your definition, but the Wiki page uses mine. I guess I&Z are more authoritative. Best to define just what one means by it, I guess.

M
 
  • #16
I think Gordan spelled his name that way, although Google votes 100-1 the other way.
 
  • #17
Mentz114 said:
nrqed - for me

\square^2 \equiv -\frac{d^2}{dt^2} + \nabla^2
Both signs are used in books.
The opposite sign
\square^2 \equiv +\frac{d^2}{dt^2} - \nabla^2
is winning out recently, because it corresponds to the metric (1,-1,-1,-1).
 
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  • #18
pam said:
I think Gordan spelled his name that way, although Google votes 100-1 the other way.

The Gordon in Klein-Gordon and the Gordan in Clebsch-Gordan are two different people.
 
  • #19
Here is a more direct question about this topic:

Is relativistic quantum mechanic also supposed to describe the dynamics of photons? Or are the similarities between equations concidental?
 
  • #20
pam said:
Both signs are used in books.
The opposite sign
\square^2 \equiv +\frac{d^2}{dt^2} - \nabla^2
is winning out recently, because it corresponds to the metric (1,-1,-1,-1).

Thanks for sending the details of that operator but I've been seeing such equations for years. Are there any physical/intuitive ideas associated with this one?
 
  • #21
Normouse,
the square is called the D'Alembertian operator. More info here -

en.wikipedia.org/wiki/D'Alembertian

It should strictly be written like this ( note the factor c^2)

\square^2 \equiv +\frac{1}{c^2}\frac{d^2}{dt^2} - \nabla^2

in which case, (as has been stated above)

(\frac{1}{c^2}\frac{d^2}{dt^2} - \nabla^2)\psi = 0 means that \psi is a field whose quanta travel at c.
 
  • #22
Normouse said:
Thanks for sending the details of that operator but I've been seeing such equations for years. Are there any physical/intuitive ideas associated with this one?

You might say so :smile:

The whole first part of my book is devoted to this equation...
for instance chapter 1:

http://physics-quest.org/Book_Chapter_EM_basic.pdf


Regards, Hans
 
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  • #23
lbrits said:
The Gordon in Klein-Gordon and the Gordan in Clebsch-Gordan are two different people.
Thank you. I now recall that I knew that once.
 
  • #24
Lojzek said:
Here is a more direct question about this topic:

Is relativistic quantum mechanic also supposed to describe the dynamics of photons? Or are the similarities between equations concidental?
RQM does describe the kinematics and dynamics of photons.
There are very few coincidences in physics.
 
  • #25
pam said:
RQM does describe the kinematics and dynamics of photons.
There are very few coincidences in physics.
This seems strange to me, since a straight wave in quantum mechanics implies uniform probability density and consequently uniform energy distribution (1 photon=h*f energy), while a straight electromagnetic wave implies energy distribution proportional to E^2, which oscilates.
 
  • #26
Good news

Mentz114 said:
Normouse,
the square is called the D'Alembertian operator. More info here -



It should strictly be written like this ( note the factor c^2)

\square^2 \equiv +\frac{1}{c^2}\frac{d^2}{dt^2} - \nabla^2

in which case, (as has been stated above)

(\frac{1}{c^2}\frac{d^2}{dt^2} - \nabla^2)\psi = 0 means that \psi is a field whose quanta travel at c.
Wow! A wonderfully clear and straight answer with actual intuition and physical feel. (VERY UNUSUAL for you physicists--careful your physicist card might be in jeopardy((just kidding))). Thanks Mentz114.
 
  • #27
Hans de Vries said:
You might say so :smile:

The whole first part of my book is devoted to this equation...
for instance chapter 1:




Regards, Hans

Books sure have improved since I was an undergraduate. I hope to "line by line" it soon. Thanks for that site(with your book on it). I wish I didn't have to work.
 

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