Two-photon physics

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 of non-linear effects. In pure vacuum, some weak scattering of light by light exists as well. Also, above some threshold of this center-of-mass energy of the system of the two photons, matter can be created.

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

Astronomy

Photon–photon scattering limits the spectrum of observed gammas to a photon energy below 80 TeV, that is, a wavelength of more than ~ 1.5×10−20 m. 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.

Frequently, photon-photon interactions will be studied via ultraperipheral collisions (UPCs) of heavy ions, such as gold or lead. These are collisions in which the colliding nuclei do not touch each other; i.e., the impact parameter is larger than the sum of the radii of the nuclei. The strong interaction between the quarks composing the nuclei is thus greatly suppressed, making the weaker electromagnetic interaction much more visible. In UPCs, because the ions are heavily charged, it is possible to have two independent interactions between a single ion pair, such as production of two electron-positron pairs. UPCs are studied with the STARlight simulation code.

Light-by-light scattering can be studied using the strong electromagnetic fields of the hadrons collided at the LHC,[1][2] it has first been seen in 2016 by the ATLAS collaboration[3][4] and was then confirmed by the CMS collaboration.[5] The best previous constraint on the elastic photon–photon scattering cross section was set by PVLAS, which reported an upper limit far above the level predicted by the Standard Model.[6] 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 and a fermionic field, since they carry no charge and no 2 fermion + 2 boson vertex exists due to requirements of renormalizability, but they can interact through higher-order processes or couple directly to each other in a vertex with an additional two W bosons: a photon can, within the bounds of the uncertainty principle, fluctuate into a virtual 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, somewhat metaphorically, 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.

There are three interaction processes:

  • Direct or pointlike: The photon couples directly to a quark inside the target photon.[7] 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).[8][9][10]

The intrinsic quark content of the photon is described by the photon structure function, experimentally analyzed in deep-inelastic electron–photon scattering.[11][12]

  • 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. d’Enterria, David; da Silveira, Gustavo G. (22 August 2013). "Observing Light-by-Light Scattering at the Large Hadron Collider". Physical Review Letters. American Physical Society (APS). 111 (8): 080405. arXiv:1305.7142. doi:10.1103/physrevlett.111.080405. ISSN 0031-9007. PMID 24010419. S2CID 43797550.
  2. Michael Schirber (22 Aug 2013). "Synopsis: Spotlight on Photon-Photon Scattering". Physical Review Letters. 111 (8): 080405. arXiv:1305.7142. doi:10.1103/PhysRevLett.111.080405. PMID 24010419. S2CID 43797550.
  3. "ATLAS spots light-by-light scattering". CERN Courier. 11 Nov 2016. Retrieved 27 May 2019.
  4. ATLAS Collaboration: Light-by-light scattering in ultra-peripheral Pb+Pb collisions at √sNN=5.02 TeV with the ATLAS detector at the LHC
  5. Collaboration, CMS (2019). "Evidence for light-by-light scattering and searches for axion-like particles in ultraperipheral PbPb collisions at $\SQRT{s_\mathrm{NN}} =$ 5.02 TeV". Phys. Lett. B. 797: 134826. arXiv:1810.04602. doi:10.1016/j.physletb.2019.134826. S2CID 201698459.
  6. Zavattini, G.; Gastaldi, U.; Pengo, R.; Ruoso, G.; Valle, F. Della; Milotti, E. (20 June 2012). "Measuring the magnetic birefringence of vacuum: the PVLAS experiment". International Journal of Modern Physics A. World Scientific Pub Co Pte Lt. 27 (15): 1260017. arXiv:1201.2309. Bibcode:2012IJMPA..2760017Z. doi:10.1142/s0217751x12600172. ISSN 0217-751X. S2CID 119248772.
  7. Walsh, T.F.; Zerwas, P. (1973). "Two-photon processes in the parton model". Physics Letters B. Elsevier BV. 44 (2): 195–198. Bibcode:1973PhLB...44..195W. doi:10.1016/0370-2693(73)90520-0. ISSN 0370-2693.
  8. Witten, Edward (1977). "Anomalous cross section for photon-photon scattering in gauge theories". Nuclear Physics B. Elsevier BV. 120 (2): 189–202. Bibcode:1977NuPhB.120..189W. doi:10.1016/0550-3213(77)90038-4. ISSN 0550-3213.
  9. Bardeen, William A.; Buras, Andrzej J. (1 June 1979). "Higher-order asymptotic-freedom corrections to photon-photon scattering". Physical Review D. American Physical Society (APS). 20 (1): 166–178. Bibcode:1979PhRvD..20..166B. doi:10.1103/physrevd.20.166. ISSN 0556-2821.
  10. Bardeen, William A.; Buras, Andrzej J. (1 March 1980). "Erratum: Higher-order asymptotic-freedom corrections to photon-photon scattering". Physical Review D. American Physical Society (APS). 21 (7): 2041. Bibcode:1980PhRvD..21.2041B. doi:10.1103/physrevd.21.2041. ISSN 0556-2821.
  11. Achard, P.; et al. (L3 collaboration) (2005). "Measurement of the photon structure function F2γ with the L3 detector at LEP". Physics Letters B. 622 (3–4): 249–264. arXiv:hep-ex/0507042. doi:10.1016/j.physletb.2005.07.028. ISSN 0370-2693.
  12. Nisius, Richard (2000). "The photon structure from deep inelastic electron–photon scattering". Physics Reports. 332 (4–6): 165–317. arXiv:hep-ex/9912049. Bibcode:2000PhR...332..165N. doi:10.1016/s0370-1573(99)00115-5. ISSN 0370-1573. S2CID 119437227.
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