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Gravitythe electromagnetic forceand the strong interaction all behave in the same way regardless of whether or not the universe is reflected in a mirror, and thus are said to conserve parity P-symmetry. Open-charm systems in cold nuclear matter - Lutz, M. G parity is a generalization of the C-parity. A meson is also a type of hadron, and it contains one quark and one antiquark.
D81 arXiv: Slightly more than three times as massive as the protonthis particle decayed slowly and didn't fit into the framework of mexon up, down, and strange quarks. According to the quark model[6] the properties of hadrons are primarily determined by their so-called valence quarks.
D mesic nuclei - Garcia-Recio, C.
Hadrons, baryons, mesons
Faddeev calculation of a K- p p quasi-bound state - Shevchenko, N. The symmetry which suppresses the electron havron is that of angular momentum, as described by Griffiths. Chiral perturbation theory - Pich, A. On the Fourier transformation of renormalization invariant coupling - Shirkov, D. Mesons are intermediate mass particles which are made up of a quark -antiquark pair.

Results and perspectives from the lattice - Bali, Gunnar S. This is an example of how hadron masses depend upon the dynamics inside the particle, and not just upon the quarks contained.
Low lying axial-vector mesons as dynamically generated resonances - Roca, L. Quarkonium at the Frontiers of High Energy Physics: Hidden local symmetry at loop: There were years of delays in the subatomic particle research during World War II —45with most physicists working in applied projects for wartime necessities.
Each type of meson has a corresponding antiparticle antimeson in which quarks are replaced by their corresponding antiquarks and vice versa.

Hideki Yukawa and the Pion Once quantum electrodyamics had produced the picture of the electromagnetic force as a process of exchanging photons, the question of whether or not the other forces were also exchange forces was a natural one. The predicted particle mass was about MeV. Baryons and mesons are included in the overall class known as hadronsthe particles which interact by the strong force.
The Role of the nucleon recoil in low-energy meson nucleus reactions - Baru, V.
Because the virtual quarks are not stable wave packets quantabut an irregular and transient phenomenon, it is not meaningful to ask which quark is real and which virtual; only the small excess is apparent from the outside in the form of a hadron.
D76 arXiv: There is more to life than the Higgs Boson!
News at work
Chiral unitary approach to meson meson and meson - baryon interactions and nuclear applications - Oller, J.
Baryonic resonances from baryon decuplet-meson octet interaction - Sarkar, Sourav et al.
D-meson decay constants and a check of factorization in non-leptonic B-decays - Becirevic, Meskn et al. D85 arXiv: Phi decay in nuclei - Oset, E. The pentaquark would be included in the classification of baryons, albeit an "exotic" one.
Heavy quark symmetry and chiral dynamics - Yan, Tung-Mow et al. A50 57 arXiv: The Spectral function of the rho meson in nuclear matter - Peters, W.
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