Theoretical study of the Compton effect with correlated three-photon emission: From the differential cross section to high-energy triple-photon entanglement
Abstract:The three-photon Compton effect is studied. An incoming photon undergoes triple scattering off a free electron, which leads to the emission of three entangled photons. We investigate the properties of both the total cross section, assuming a low-energy cutoff for the detected photons, and the differential cross section. Particular emphasis is laid on evaluating polarization-resolved cross sections. The entanglement of the final three-photon state is analyzed.
“…The discrepancy for higher energies is quite expected due to inapplicability of the soft-photon approximation for the parameter ω 0 = ω 1 50 = s−m 2 e 100me chosen in ref. [28].…”
Using modern multiloop calculation methods, we derive the analytical expressions for the total cross sections of the processes e−γ →$$ {e}^{-}X\overline{X} $$
e
−
X
X
¯
with X = μ, γ or e at arbitrary energies. For the first two processes our results are expressed via classical polylogarithms. The cross section of e−γ → e−e−e+ is represented as a one-fold integral of complete elliptic integral K and logarithms. Using our results, we calculate the threshold and high-energy asymptotics and compare them with available results.
“…The discrepancy for higher energies is quite expected due to inapplicability of the soft-photon approximation for the parameter ω 0 = ω 1 50 = s−m 2 e 100me chosen in ref. [28].…”
Using modern multiloop calculation methods, we derive the analytical expressions for the total cross sections of the processes e−γ →$$ {e}^{-}X\overline{X} $$
e
−
X
X
¯
with X = μ, γ or e at arbitrary energies. For the first two processes our results are expressed via classical polylogarithms. The cross section of e−γ → e−e−e+ is represented as a one-fold integral of complete elliptic integral K and logarithms. Using our results, we calculate the threshold and high-energy asymptotics and compare them with available results.
“…The discrepancy for higher energies is quite expected due to inapplicability of the softphoton approximation for the parameter ω 0 = ω 1 50 = s−m 2 e 100me chosen in Ref. [26].…”
Using modern multiloop calculation methods, we derive the analytical expressions for the total cross sections of the processes e − γ → e − X X with X = µ, γ or e at arbitrary energies. For the first two processes our results are expressed via classical polylogarithms. The cross section of e − γ → e − e − e + is represented as a one-fold integral of complete elliptic integral K and logarithms. Using our results, we calculate the threshold and high-energy asymptotics and compare them with available results.
“…* Multiple Thomson scattering has been previously discussed in, for instance, Refs. [19][20][21]. One would naively expect that the cross section for n-photon emission would scale as σ n ∼ α n−1 σ Thomson ; while this is true in the high-energy regime (E γ m e ), up to logarithmic corrections [22,23], in the nonrelativistic regime the cross section has the form [21,24]…”
The discovery of neutrino oscillations invites many fundamental physics questions that have yet to be answered. Two of these questions are simple, easy to state, and essential: What are the values of the neutrino masses? Are neutrinos Majorana fermions? The reason we don't know the answer to those questions is that it is difficult to measure neutrino properties outside of the ultrarelativistic regime. We discuss the physics of eγ → eνν near threshold, where one has access to nonrelativistic neutrinos and only nonrelativistic neutrinos. Near threshold, eγ → eνν is a rich phenomenon and its cross section is sensitive to the individual values of the neutrino masses and the nature of the neutrinos. We show that if one could scan the threshold region, it would be simple to identify the mass of the lightest neutrino, the neutrino mass ordering, and whether the neutrinos are Majorana fermions. In practice, however, event rates are tiny and backgrounds are huge; the observation of eγ → eνν in the sub-eV regime appears to be utterly inaccessible in the laboratory. Our results, nonetheless, effectively illustrate the discriminatory power of nonrelativistic neutrino observables.
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