The bottom quark, also called the beauty quark and usually symbolized by b, is a third‑generation elementary quark. It carries electric charge −1/3 and is substantially heavier than the up, down and strange quarks but much lighter than the top quark. The b quark groups into bound states (hadrons) such as B mesons and bottom baryons rather than existing freely; examples include the B0, B+, Bs and the Lambda_b. For basic context about its place among fundamental particles, see elementary particles and the family of quarks.

Physical characteristics and notation

As a flavored quark, the bottom has spin 1/2 and a flavor quantum number often called beauty or bottomness. Its electric properties are discussed under electric charge, and its relative mass is commonly cited when comparing quark generations; general discussions of the concept of mass in particle physics are useful background. The bottom quark is the partner of the top quark in the third generation and participates in the strong, weak and electromagnetic interactions according to the Standard Model.

Production, bound states and discovery

Bottom quarks are produced in high‑energy collisions such as those at the Large Hadron Collider and were first identified indirectly through heavy quarkonium states. The discovery of the Upsilon family (bb̄ bound states) in 1977 provided the first clear evidence of a new heavy quark. In collisions, freely produced b quarks quickly hadronize, forming B mesons or bottom baryons. These hadrons are the species most often observed in experiments when studying bottom physics.

Decay and lifetimes

Bottom quarks decay via the weak interaction. Typical decay chains transform a b quark into either a charm quark or an up quark, processes described in general terms as decay to a charm quark or a up quark. The observable lifetimes of bottom hadrons are short — on the order of 10^−12 seconds — but long enough that modern detectors can reconstruct displaced decay vertices, a key experimental signature used to identify b‑hadron decays and measure their properties.

Scientific importance and applications

Studies of bottom quarks and B hadrons are central to tests of the Standard Model. Precision measurements of b‑hadron decays probe the Cabibbo–Kobayashi–Maskawa (CKM) matrix, provide constraints on sources of CP violation, and search for signs of physics beyond the Standard Model. Dedicated experiments, often called B factories (for example, the past BaBar and Belle programs and the ongoing LHCb experiment), focus on large samples of b decays to study these effects. Practical outcomes include refined theoretical tools like heavy quark effective theory and improved experimental techniques such as vertexing and flavor tagging.

Notable distinctions and common terminology

  • The names "bottom" and "beauty" are both used; "bottom" is common in many contemporary texts while "beauty" appears in older literature.
  • Bottom quarks are heavier than charm quarks but much lighter than the top quark; their interactions span strong, weak and electromagnetic forces.
  • Some important bound states include B mesons (B0, B+, Bs), bottom baryons (Lambda_b), and quarkonium states like Upsilon.

For further reading on the broader family of particles and how flavor physics is studied experimentally, consult resources on particle detectors and flavor physics. Historical and technical introductions often link to experimental reports and reviews that describe how down quark and bottom comparisons informed early classification. Contemporary research continues to use b‑quark measurements to probe the limits of the Standard Model and to search for new phenomena.