Random Phase Approximation (Why they call it so?)

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SUMMARY

The term "Random Phase Approximation" (RPA) in many-body physics refers to the method of calculating correlation functions in quantum field theory, particularly through the work of Bohm and Pines in their 1951 paper. RPA distinguishes between two types of electron responses to a wave: one that is in phase and contributes to organized behavior, and another that has a phase difference dependent on particle position, which averages out to zero in large systems. This averaging process is the essence of the "random" aspect of the approximation.

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  • Study the original paper by Bohm and Pines, "Phys. Rev. 82, 625, (1951)" for foundational insights on RPA
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  • Learn about the mathematical formulation of Green's functions in quantum mechanics
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"Random Phase Approximation" (Why they call it so?)

Hi,

I'm wondering that why the scientists call this phenomena in many body physics "Random Phase Approximation". (Why Random? Why Phase?) It seems that when we want calculate a correlation function in quantum field theory, it leads to calculation of 4-particle or 6-particle green's function and we use mean field theory to calculate it and nothing more. so why we should call it random phase approximation (Why Random? Why Phase?) .

Thank you.
 
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From the original paper on RPA by Bohm and Pines, Phys. Rev. 82, 625, (1951):
Bohm and Pines said:
We distinguish between two kinds of response of the electrons to a wave. One of these is in phase with the wave, so that the phase difference between the particle response and the wave producing it is independent of the position of the particle. This is the response which contributes to the organized behavior of the system. The other response has a phase difference with the wave producing it which depends on the position of the particle. Because of the general random location of the particles, this second response tends to average out to zero when we consider a large number of electrons, and we shall neglect the contributions arising from this. This procedure we call the random phase approximation.”
 
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