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thanks for everyone who can give an answer

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thanks for everyone who can give an answer

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vanesch

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If you solve for classical fields, you see that their solution space is build up from different modes (this is sometimes called "separation of variables" and you separate the spatial variables from the time variable), so you write your general field solution, satisfying boundary (but not initial) conditions:Kruger said:We describe classical fields with electromagnetic WAVES. Why can quantum theory describe the electromagnetic field with harmonic oscillations? An electromagnetic wave has a certain direction where it moves with a certain velocity. And an oscillation just oscillates up and down. So, what are the analogies of these two things?

E(r,t) = a1(t) E1(r) + a2(t) E2(r) +...

and it turns out that the solutions for a1(t)... are of the form A sin(w1.t) + B cos(w1.t).

Each term in this sum is called a field mode.

These constants (A and B) for each a(t) are fixed by the initial conditions and give you your solution E(r,t) that satisfies boundary and initial conditions.

So when looking at the dynamics in time, it is as if the final E-field is just a composition of different harmonic oscillators, described by a1(t), a2(t) ...

The field is then just seen as a kind of book keeping device that helps us keep track of all these different oscillators, but just specifying A and B of each of them is equivalent to this description.

So there is a 1-1 relationship between a set of oscillators of frequencies w1, w2, ... and a field solution E(r,t).

cheers,

Patrick.

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scroll down to the https://www.physicsforums.com/journal.php?s=&action=view&journalid=13790&perpage=10&page=7 [Broken] -entry

regards

marlon

regards

marlon

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marlon

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reilly

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That being said, the topic is discussed in excruciating detail in almost any book that covers basic QFT and canonical quantization. (I think the discussion in Mandel and Wolf's book on Quantum Optics is the best, but check out Google. You'll hit lots of paydirt.)

Regards,

Reilly Atkinson

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Kruger said:

thanks for everyone who can give an answer

A classical wave can also be described like a collection of harmonic oscillators, an infinite one.

At each point of the transversal wave you have harmonic motion, site there a harmonic oscillator and ready!

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An EM-wave is just a fluctuation of the EM field. The dynamics is described in terms of the constituent harmonic oscillators. Just think of this : you jump on a trampoline with a very big surface. Once you have jumped, the trampoline surface will vibrate up and down and this vibration will propagate over the surface : that is the wave or the excitation of the trampoline.Kruger said:

Now, in QFT, the transition from a flat trampoline to an oscillating one demands some energy dE. Via E=mc², energy is the same as mass. So through this excitation, you have created a mass : ie a particle. That is what we mean when we say particles are excitations of fields in QFT

regards

marlon

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reilly

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Regards,

Reilly Atkinson

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Is there any book you could recommand on this topic?

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Anthony Zee's QFT in a Nutshell.

But beware : only read the first few chapters. :)

marlon

But beware : only read the first few chapters. :)

marlon

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Consider two parallel walls. Between this walls there can only be certain electromagnetic waves. The electric and magnetic field vanishes at the wall. On electromagnetic wave just forms one electromagnetic oscillation between the walls.

If we want to use this for free space we just say the distance of the two walls is "infiniti". Thus we can apply the same prinziple. Only difference is that the harmonic oscillations can have any wave numbers k.

Is that right? Can we just imagine this as a reason why the em-quantum field is described by a collection of independant harmonic oscillations?

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