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J/psi meson

physical science Maturity 11-13 Next article →

The J/psi meson is a unique subatomic particle. It is a flavor-neutral meson. This means it is made of a charm quark and a charm antiquark. When a charm quark and a charm anti-quark form a bound state, scientists call them charmonium. The J/psi is the most common form of charmonium. This is because it has a spin of 1 and a low rest mass. Its rest mass is 3.1 GeV. This is just slightly higher than the mass of a D meson. Understanding this particle helps scientists study the fundamental building blocks of our universe.

This particle behaves in a very surprising way. It has a mean lifetime of about 10^-18 seconds. This lifetime was about a thousand times longer than scientists expected. This happens because of the OZI rule. This rule strongly suppresses hadronic decay modes. A decay mode is a specific way a particle breaks apart. Because hadronic decays are suppressed, electromagnetic decays can compete with them. This allows the J/psi to have a significant branching fraction to leptons. Leptons are fundamental particles like electrons or muons. The particle can decay into several different things, such as three gluons or a pair of leptons.

There are different states of charmonium. The J/psi is the most common one. There are also excited states. The first excited state is called the psi(2S). The next excited state is called the psi(3770). These names indicate their specific quantum states or their mass in GeV. Other vector charm-anticharm states are named using the psi symbol and their quantum state or mass. These different states show how quarks can bind together in various ways. Scientists use these states to map out the rules of the strong interaction.

In the 1960s, the first quark models were proposed. These models suggested that protons and neutrons were made of quarks. At that time, scientists only knew about three flavors of quarks: up, down, and strange. Many people thought quarks were just mathematical fiction. They were seen as tools for calculation rather than real physical objects. However, experiments at the Stanford Linear Accelerator Center (SLAC) in 1969 showed evidence of particles inside protons. This helped prove that quarks were likely real. Later, the model expanded to include six quarks: charm, top, bottom, up, down, and strange.

The discovery of the J/psi happened in 1974. Two different research groups found it at almost the same time. One group was at the Stanford Linear Accelerator Center, led by Burton Richter. The other group was at the Brookhaven National Laboratory, led by Samuel Ting. Ting's group saw a peak at 3.1 GeV in production rate plots. They announced their findings on 11 November 1974. This moment was so impactful that it is called the "November Revolution." It caused rapid changes in high-energy physics. Richter and Ting were awarded the 1976 Nobel Prize in Physics for this work.

The name of the particle is also quite special. It is the only particle with a two-letter name. Richter wanted a Greek name. He chose "psi" after consulting with a friend. Ting wanted a Roman name. He chose "J" because stable particles often used Roman characters. To be fair to both groups, the scientific community combined them into "J/psi." This name honors both the Stanford and Brookhaven discoveries. It is a rare example of a name that represents a joint victory in science.

Scientists also study how the J/psi behaves in extreme heat. In a hot QCD medium, the particle can melt. This happens when the temperature rises well beyond the Hagedorn temperature. When it melts, it is a signal that a quark-gluon plasma has formed. This is a special state of matter. Experiments at CERN and Brookhaven have studied this phenomenon. While results have been complex, researchers look for these signals to understand how quarks move freely. This helps us understand the very early history of our universe.

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