Register to reply 
3 easy QFT questionsby Sterj
Tags: None 
Share this thread: 
#1
Apr1305, 02:35 PM

P: n/a

I have three questions about QFT. I know you can answer this questions, sure you can.
 How does a standing wave look like in 3 dimensions (x,y,z). I mean an electro magnetic oscillation between two walls or in free space. I can't really imagine that thing and looked for pictures (google) but coudn't find what I searched for.  Let's say we have an electromagnetic oscillation with quantum number n=3. Then this has energy of 7/2*w*h(bar) and contains 3 particles (photons). Here we say this particles make the field oscillating. And thus the oscillation of this particles can go from earth to moon. But if we describe this 3 photons as wave packets they don't have such an influence (from moon to earth). Something has to be false, but what?  Consider two plates. Between that plates there is a harmonic oscillation with energy 7/2*w*h(bar). How can we describe this oscillation with formulas. I tried to solve this with 2 wave functions. One comes from left and one from the right side and they interfer. But my wave functions don't involve the energy, arghhhhh. Can someone give me a guess? Thanks for any help. 


#2
Apr1305, 02:53 PM

P: 4,006

or google for standing wave animation These phonons do not make any field oscillate, they are the actual result of the oscillations of a massless spin 1 field. Well, actually they arise as the oscillations of a massive spin 1 field (with certain energy value that corresponds to the given energy), and then the mass is taken to be ZERO. marlon 


#3
Apr1305, 03:42 PM

P: n/a

thanks marlon



#4
Apr1305, 05:31 PM

P: 4,006

3 easy QFT questions
marlon 


#5
Apr1405, 06:41 AM

Sci Advisor
HW Helper
PF Gold
P: 2,015

QFT is usually described in perturbation theory usiing Feynman diagrams.
In this case, the created photons are plane (or spherical) wave trains. They don't really propagate in space, because having a defiinite momentum, the wave train is infinite and exists thoughout all space. They are best seen in the momentum representation. A physical photon with a finite extent in space would be a linear combination of these photon states forming wave packet, just as a classical EM wave packet is formed. So photon wave packets can be wave packets in QED, formed in the same way wave packets are formed in EM. 


#6
Apr1405, 08:17 AM

P: 4,006

We need to make a clear distinction between real and virtual photons here
Again this can lead to a discussion on semantics Though it is really important to realize that photons arise as the actual vibrations of the spin 1field (you can call this the actual wave indeed). But it needs to be said that when the field 'goes' from one vibrationmode to another, the change in energy corresponds to the actual photon. Not the wave itself... That is the big difference between QM and QFT marlon 


#7
Apr1405, 08:25 AM

P: n/a

thanks you both.
I tried to calculate a harmonic oscillation in free space. I did this by letting one wave come from the right side and one from the left (superposition between these two waves gives me an oscillation): psi(x,t)=cos(xt)+sin(x+t) That's the expression with no energy. For the expression with energy I did this: p(x,t)=exp[i(kxwt)] u(x,t)=exp[i(kx+wt)] now k=p/h(bar) (1) and E=hf p=hf/c thus: p=E/c and with (1) and the definition m=E/(c*h(bar)) the wavefunction p(x,t) goes into: p(x,t)=exp[i(mxwt)] And if I take the superposition of these two waves I get the oscillation: psi(x,t)=p(x,t)+u(x,t) And if the oscillation is in the ground state the factor m transforms because E=h(bar)w/2 And the w in the wavefunction is the same w as the w in the energy expression for the ground state. Is this right? 


Register to reply 
Related Discussions  
6 Easy Questions  Introductory Physics Homework  4  
Guys, I have 4 easy questions. (probably easy to you)  Introductory Physics Homework  32  
Two easy questions!  Academic Guidance  9  
Easy questions.  Introductory Physics Homework  15  
Easy Questions  Plz Help  Introductory Physics Homework  3 