about @LHCbExperiment #pentaquark discovery
Once upon a time, there was a controversy in particle physics. There were some physicists who denied the existence of structures more elementary than hadrons, and searched for a self-consistent interpretation wherein all hadron states, stable or resonant, were equally elementary. Others, appalled by the teeming democracy of hadrons, insisted on the existence of a small number of fundamental constituents and a simple underlying force law. In terms of these more fundamental things, hadron spectroscopy should be qualitatively described and essentially understood just as are atomic and nuclear physics.(11)
The need of the partons
When we descrive the collisions between particles, we calculate the
cross section, the area of the distribution of the collisions' products. The mathematical object used to calculate the cross section are the
structure functions, that mathematically describes the inner structure of the particle. In 1969 studying the deep inelastic scattering
J. D. Bjorken(4, 18), in order to explain the experimental results, proposed a particular property for the hadronic structure function in the cross section called
scaling. In the same year
Richard Feynman(5, 18) suggested the necessity to adopt a new description of hadrons: they had to be made by smaller components, more elementary than the hadrons themselves. These components are called partons.
The Feynman's thesys was immediatly verified by Bjorken and
Paschos(6, 7, 18), in this way starting a great discussion about the parton models, described in the paper by
De Rújula,
Georgi and
Glashow quoted at the beginning of the post
(11) (an interesting review of the parton model and its story is in Greenberg
(18)).
Probably the most strong motivation to adopt the parton model to describe hadrons is the great production of particles in the ring particles accelerators
(5). So, theoretical physicists produced a lot of model, but the most succesfull is the quarks model, developed by
Murray Gell-Mann(1) and
Georg Zweig(2, 3), that introduced a new quantum number, the
flavor. The first formulation involved three type of quarks (and so three flavors): up, down and strange. To this first set of elementary particles in 1970 the quark charm was added by Glashow,
Iliopulos and
Maiani(8) and finally in 1973
Kobayashi and
Maskawa(9) completed the family with the two last quark, top and bottom, named by
Harari(10) in 1975.
Three quarks for Muster Mark!
Sure he has not got much of a bark
And sure any he has it's all beside the mark.
from Finnegan's Wake by James Joyce