A Does x affect the value of [a^2,(a^†)^2×e^2ikx]

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The discussion centers on the commutation relation between the squared lowering operator a^2 and the squared mode expansion involving e^2ikx in quantum field theory (QFT). The main challenge is addressing the positional dependence introduced by the e^ikx term while considering the linearity of integration. There is uncertainty about whether the exponential term can be treated as a scalar that can be factored out, particularly in relation to the behavior of ladder operators. The conversation also touches on the implications of using raising operators instead of lowering ones in this context. Overall, the participants seek clarity on how to properly handle these operators and their interactions within the framework of QFT.
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In terms of QFT commutators involving raising and lowering operators and the mode expansion, does [a^2,(a^†)^2×e^2ikx] get changed by the last positionally-dependent term?
What is the commutator between a^2 (lowering operator squared) and the squared mode expansion from QFT (the integral of a^2e^2ikx, the conjugate, and the cross term I don't feel like writing out)? My instinct is to try and divide the mode expansion into its two parts since integration is linear, such as with just [a^2,(a^†)^2×e^2ikx]. However, even if I was sure I could do that, I’m not sure how to go about taking care of the positional dependence. For example, if we just had [a^2,(a^†)^2], it would just be 2(1+(a^†)a), but I'm having trouble with the extra e^ikx term in the new commutator. My thought is that it's really just a number so it can be pulled out by linearity leaving just [a^2,(a^†)^2], but I'm unsure if the ladder operators have any impact on the e^whatever operator (such as switching modes), which would then change the commutator. Also, is it any different if the first lowering operator is instead a raising operator? Any insight into the math here would be appreciated!
 
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In the treatments I've seen the x and k are c-numbers i.e. parameters and not operators. All operators are expressed in terms of the creators and annihilators. Typically however the creators and annihilators are themselves indexed e.g. by momentum k. Note from the texts how e.g. the momentum operator is expressed.
\hat{p}= \int k a^\dagger(k)a(k) dk= \int k \hat{n}(k) dk
(suitably normalized.)
 
jambaugh said:
In the treatments I've seen the x and k are c-numbers i.e. parameters and not operators. All operators are expressed in terms of the creators and annihilators. Typically however the creators and annihilators are themselves indexed e.g. by momentum k. Note from the texts how e.g. the momentum operator is expressed.
\hat{p}= \int k a^\dagger(k)a(k) dk= \int k \hat{n}(k) dk
(suitably normalized.)
I know that in the quantum harmonic oscillator, you can have the ladder operators explicitly written in terms of x and k (vice versa). However, I'm not sure if I can use that explicit form since I'm working with a QFT system closer to a particle bath.
At any rate, I'm inclined to treat the e^ikx term as a scalar that's simply parameterized by the value of k and x if we can treat x as a parameter in the ladder operators rather than itself an operator. For example, if [(a^†)^2,a]=2a^†, we could just pull out our exponential to get [(a^†)^2,ae^ikx]=2(e^ikx)a^† rather than worrying about what implicit commutation the ladder operator might have with e^ikx. I'm still not sure, does this make sense?
 
For the quantum state ##|l,m\rangle= |2,0\rangle## the z-component of angular momentum is zero and ##|L^2|=6 \hbar^2##. According to uncertainty it is impossible to determine the values of ##L_x, L_y, L_z## simultaneously. However, we know that ##L_x## and ## L_y##, like ##L_z##, get the values ##(-2,-1,0,1,2) \hbar##. In other words, for the state ##|2,0\rangle## we have ##\vec{L}=(L_x, L_y,0)## with ##L_x## and ## L_y## one of the values ##(-2,-1,0,1,2) \hbar##. But none of these...

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