Jump to content

Two-photon physics

From Wikipedia, the free encyclopedia

This is an old revision of this page, as edited by Kotika98 (talk | contribs) at 07:50, 3 May 2016 (Added explanation of the basic physics involved, removed irrelevant citation and replaced by a link to the "Schwinger limit".). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

A Feynman diagram (box diagram) for photon–photon scattering, one photon scatters from the transient vacuum charge fluctuations of the other

Two-photon physics, also called gamma–gamma physics, is a branch of particle physics that describes the interactions between two photons. Normally, beams of light pass through each other unperturbed. Inside an optical material, and if the intensity of the beams is high enough, the beams may affect each other through a variety on non-linear effects. In pure vacuum, some weak scattering of light by light will exist if the center-of-mass energy of the system of the two photons is large enough. Also, above some threshold of this center-of-mass energy of the system of the two photons, matter can be created.

Astronomy

Photon–photon scattering limits the spectrum of observed gammas to below 80 TeV. The other photon is one of the many photons of the cosmic microwave background. In the frame of reference where the invariant mass of the two photons is at rest, both photons are gammas with just enough energy to pair-produce an electron–positron pair.

Experiments

Two-photon physics can be studied with high-energy particle accelerators, where the accelerated particles are not the photons themselves but charged particles that will radiate photons. The most significant studies so far were performed at the Large Electron–Positron Collider (LEP) at CERN. If the transverse momentum transfer and thus the deflection is large, one or both electrons can be detected; this is called tagging. The other particles that are created in the interaction are tracked by large detectors to reconstruct the physics of the interaction.

Light-by-light scattering has not been directly observed so far. As of 2012, the best constraint on the elastic photon–photon scattering cross section belongs to PVLAS, which reports an upper limit far above the level predicted by the Standard Model.[1] Proposals have been made to measure elastic light-by-light scattering using the strong electromagnetic fields of the hadrons collided at the LHC.[2] Observation of a cross section larger than that predicted by the Standard Model could signify new physics such as axions, the search of which is the primary goal of PVLAS and several similar experiments.

Processes

From quantum electrodynamics it can be found that photons cannot couple directly to each other, since they carry no charge, but they can interact through higher-order processes[clarification needed]. Only in Topological Dipole Field Theory[3] photon-photon scattering is predicted. A photon can, within the bounds of the uncertainty principle, fluctuate into a charged fermion–antifermion pair, to either of which the other photon can couple. This fermion pair can be leptons or quarks. Thus, two-photon physics experiments can be used as ways to study the photon structure, or what is "inside" the photon.

The photon fluctuates into a fermion–antifermion pair.
Creation of a fermion–antifermion pair through the direct two-photon interaction. These drawings are Feynman diagrams.

We distinguish three interaction processes:

  • Direct or pointlike: The photon couples directly to a quark inside the target photon.[4] If a lepton–antilepton pair is created, this process involves only quantum electrodynamics (QED), but if a quark–antiquark pair is created, it involves both QED and perturbative quantum chromodynamics (QCD).[5][6] The intrinsic quark content of the photon is described by the photon structure function, experimentally analyzed in deep-inelastic electron–photon scattering.[7][8]
  • Single resolved: The quark pair of the target photon form a vector meson. The probing photon couples to a constituent of this meson.
  • Double resolved: Both target and probe photon have formed a vector meson. This results in an interaction between two hadrons.

For the latter two cases, the scale of the interaction is such as the strong coupling constant is large. This is called Vector Meson Dominance (VMD) and has to be modelled in non-perturbative QCD.

See also

References

  1. ^ G. Zavattini et al., "Measuring the magnetic birefringence of vacuum: the PVLAS experiment", Accepted for publication in the Proceedings of the QFEXT11 Benasque Conference, [1]
  2. ^ D. d'Enterria, G. G. da Silveira, "Observing Light-by-Light Scattering at the Large Hadron Collider", Phys. Rev. Lett., 111 (2013) 080405 [2]
  3. ^ Linker, P. (2015). "Topological Dipole Field Theory". The Winnower. 3: e144311.19292. doi:10.15200/winn.144311.19292.
  4. ^ T.F.Walsh and P.M.Zerwas, "Two photon processes in the parton model", Phys. Lett. B44 (1973) 195.
  5. ^ E.Witten, "Anomalous Cross-Section for Photon – Photon Scattering in Gauge Theories", Nucl. Phys. B120} (1977) 189.
  6. ^ W.A.Bardeen and A.J.Buras, "Higher Order Asymptotic Freedom Corrections to Photon–Photon Scattering", Phys. Rev. D20 (1979) 166, [Erratum-ibid. D21 (1980) 2041].
  7. ^ L3 Collaboration, Measurement of the photon structure function F2γ with the L3 detector at LEP, Phys. Lett. B 622, 249 (2005)
  8. ^ R. Nisius, The photon structure from deep inelastic electron photon scattering, Physics Report 332 (2000) 165
Retrieved from "https://en.wikipedia.org/w/index.php?title=Two-photon_physics&oldid=718395383"