Two-photon physics: Difference between revisions
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* ''Double resolved'': Both target and probe photon have formed a vector meson. This results in an interaction between two hadrons. |
* ''Double resolved'': Both target and probe photon have formed a vector meson. This results in an interaction between two hadrons. |
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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. |
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. |
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== See also == |
== See also == |
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Revision as of 21:02, 24 March 2012
Two-photon physics, also called gamma-gamma physics, is a branch of particle physics for the interactions between two photons. If the energy in the center of mass system of the two photons is large enough, matter can be created.[1]
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 is large, one or both electrons can be deflected enough to 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.
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. 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.
We distinguish three interaction processes:
- Direct or pointlike: The photon couples directly to a quark inside the target photon[citation needed]. 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).
- 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
- Channelling radiation has been considered as a method to generate polarized high energy photon beams for gamma-gamma colliders.
- Matter creation
- Pair production
References
- ^ Moffat JW (1993). "Superluminary Universe: A Possible Solution to the Initial Value Problem in Cosmology". Intl J Mod Phys D. 2 (3): 351–65. arXiv:gr-qc/9211020. Bibcode:1993IJMPD...2..351M. doi:10.1142/S0218271893000246.
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- L3 Collaboration, Measurement of the photon structure function F2γ with the L3 detector at LEP, Phys. Lett. B 622, 249 (2005).