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Parton (particle physics)

physical science Maturity 9-11 Next article →

In particle physics, the parton model provides a way to understand the internal structure of hadrons. Hadrons are particles like protons and neutrons that make up the core of atoms. The model describes hadrons as being composed of several point-like constituents called partons. This framework is essential for interpreting the results of high-energy particle collisions. It helps scientists understand the complex radiation patterns produced during these events.

Parton scattering
Parton scattering

By using this model, researchers can better analyze how particles behave when they interact at extreme speeds.

The mechanism of the parton model relies on the energy or "resolution scale" used to look at a particle. At low energies, a probe only sees the most basic components, known as valence partons. For example, a baryon like a proton contains three valence quarks. A meson contains two valence partons, which are a quark and an antiquark. However, as the energy increases, the resolution scale improves. At these higher energies, the probe detects additional particles called sea partons. This means the number of partons actually increases as the momentum transfer grows.

CTEQ6 parton distribution functions
CTEQ6 parton distribution functions

Partons behave differently depending on the physical scale being observed. A single quark parton at one scale might appear as a single particle. At a smaller length scale, that same quark might resolve into a superposition of a quark and a gluon. Similarly, a gluon parton can resolve into a state containing a gluon, a quark, and an antiquark. This happens because the resolution is tied to the momentum transfer of the probe. This relationship is a consequence of Heisenberg's uncertainty principle. The higher the energy and momentum of the probe, the smaller the length scale it can see.

The history of the parton model is tied to several major breakthroughs in physics. Richard Feynman proposed the model in 1969 to analyze high-energy hadron collisions. Shortly after, James Bjorken and Emmanuel Anthony Paschos applied the model to electron-proton deep inelastic scattering. Over time, experimental observations such as Bjorken scaling helped validate the theory. The discovery of asymptotic freedom in quantum chromodynamics (QCD) also played a key role. These discoveries allowed scientists to finally match partons to the specific particles known as quarks and gluons. Interestingly, physicist Murray Gell-Mann once preferred the term "put-ons" for these constituents.

One of the most dynamic processes in this field is the parton shower. When partons are accelerated, they emit radiation. In the theory of quantum chromodynamics, this radiation takes the form of gluons. This is similar to how accelerated electric charges emit photons in quantum electrodynamics (QED). However, there is a major difference between these two types of radiation. Unlike photons, gluons carry color charges. Because they carry charge, gluons can emit further radiation themselves. This creates a cascading effect known as a parton shower.

Parton scattering
Parton scattering

To study these complex showers, scientists use sophisticated computer simulations. These are often called Monte Carlo event generators. These programs help researchers calibrate and interpret data from massive experiments like those at the Large Hadron Collider (LHC). Two common choices for these simulations are PYTHIA and HERWIG. These tools are vital for studying particle phenomenology. They allow scientists to model how partons eventually turn into the larger particles seen in detectors. Without these simulations, understanding the chaotic environment of a collider would be nearly impossible.

Modern research has expanded the model into even more detailed territory. Scientists now use Generalized Parton Distributions (GPDs) to gain a deeper understanding of hadron structure. While ordinary parton distribution functions (PDFs) provide probability densities, GPDs include more variables. These include the spin and the transverse momentum of the partons. GPDs can even be used to create a full three-dimensional image of the partons inside a hadron. This advanced approach helps researchers study the spin structure of the proton. It connects the movement of quarks and gluons to the overall angular momentum of the particle.

CTEQ6 parton distribution functions
CTEQ6 parton distribution functions
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