Hadron: Difference between revisions

From Citizendium
Jump to navigation Jump to search
imported>John R. Brews
m (→‎Types: See also)
imported>John R. Brews
m (→‎Types: notation)
Line 8: Line 8:
The hadrons fall into two groups: the ''[[baryon]]s'' with ''baryon number B''=±1 and spin an odd multiple of 1/2, and ''[[meson]]s'' with ''B''=0 and integer spin. The hadrons are classified further according to their ''[[isospin]] I'' and its component ''I<sub>3</sub>'', and also by their ''[[strangeness]] S''. The combination ''Y = B + S'' is called the ''strong [[hypercharge]]''. Under strong interactions, ''B, I, I<sub>3</sub>, S'' are conserved, but conservation of ''S'' is violated by the [[weak force]] interactions.<ref name=Greiner/>
The hadrons fall into two groups: the ''[[baryon]]s'' with ''baryon number B''=±1 and spin an odd multiple of 1/2, and ''[[meson]]s'' with ''B''=0 and integer spin. The hadrons are classified further according to their ''[[isospin]] I'' and its component ''I<sub>3</sub>'', and also by their ''[[strangeness]] S''. The combination ''Y = B + S'' is called the ''strong [[hypercharge]]''. Under strong interactions, ''B, I, I<sub>3</sub>, S'' are conserved, but conservation of ''S'' is violated by the [[weak force]] interactions.<ref name=Greiner/>


In general, hadrons are particles made up of [[quark]]s, antiquarks, and [[gluon]]s. Their strong interactions are described by [[quantum chromodynamics]].<ref name=Susskind/> The [[meson]] is a [[quark]] and an antiquark paired in various ways, the [[proton]] is made up of two up quarks and one down quark, and a [[neutron]] is made up of two down quarks and one up quark.<ref name=Lincoln/><ref name=Quinn/> Some other examples appear in the tables below.
In general, hadrons are particles made up of [[quark]]s, antiquarks, and [[gluon]]s. Their strong interactions are described by [[quantum chromodynamics]].<ref name=Susskind/> The [[meson]] is a [[quark]] and an antiquark paired in various ways, the [[proton]] is made up of two up quarks and one down quark, and a [[neutron]] is made up of two down quarks and one up quark.<ref name=Lincoln/><ref name=Quinn/> Some other examples appear in the tables below. Symbols ''u, d, s'' refer to ''up'', ''down'' and ''strange'' quarks, and overlines indicate [[antiparticle]]s.
{| class="wikitable" style="margin: 0 auto; text-align:center"
{| class="wikitable" style="margin: 0 auto; text-align:center"
|+Some baryons
|+Some baryons

Revision as of 12:59, 3 September 2011

This article is a stub and thus not approved.
Main Article
Discussion
Related Articles  [?]
Bibliography  [?]
External Links  [?]
Citable Version  [?]
 
This editable Main Article is under development and subject to a disclaimer.

A hadron (pronounced hay-dron, and based upon the Greek hadr=strong) is a composite particle subject to the strong nuclear force. Although the defining feature is their strong force interactions, they also may be subject to weak and electromagnetic forces.

Types

See also the articles Quark and Standard Model

The hadrons fall into two groups: the baryons with baryon number B=±1 and spin an odd multiple of 1/2, and mesons with B=0 and integer spin. The hadrons are classified further according to their isospin I and its component I3, and also by their strangeness S. The combination Y = B + S is called the strong hypercharge. Under strong interactions, B, I, I3, S are conserved, but conservation of S is violated by the weak force interactions.[1]

In general, hadrons are particles made up of quarks, antiquarks, and gluons. Their strong interactions are described by quantum chromodynamics.[2] The meson is a quark and an antiquark paired in various ways, the proton is made up of two up quarks and one down quark, and a neutron is made up of two down quarks and one up quark.[3][4] Some other examples appear in the tables below. Symbols u, d, s refer to up, down and strange quarks, and overlines indicate antiparticles.

Some baryons
Particle name Symbol Quark structure Q (e) Baryon number B Strangeness S Spin Isospin I Mass (relative) Lifetime (s)
Proton p 1 1 0 1/2 1/2 1 Stable
Neutron n 0 1 0 1/2 1/2 1 898
Lambda zero Λ0 0 1 -1 1/2 0 1.2 2.6 × 10-10
Omega minus Ω -1 1 −3 1/2 0 1.8 0.8 × 10-10

Some mesons
Particle name Symbol Quark structure Q (e) Baryon number B Strangeness S Spin Isospin I Mass (relative) Lifetime (s)
Pion zero π0 0 0 0 0 1 0.14 0.8 × 10-16
Pion plus π+ 1 0 0 0 1 0.14 2.6 × 10-8
Kaon plus K+ 1 0 1 0 1/2 0.52 1.2 × 10-8
Kaon zero K0 0 0 1 0 1/2 0.53 8.9 × 10-11

References

  1. Walter Greiner, Berndt Müller (2000). “§6.1 The world of hadrons”, Gauge theory of weak interactions. Springer, pp. 205 ff. ISBN 3540676724. 
  2. Leonard Susskind (2005). The cosmic landscape: string theory and the illusion of intelligent design. Hachette Digital, Inc., p. 159. ISBN 0316155799. 
  3. Don Lincoln (2004). Understanding the universe: from quarks to the cosmos. World Scientific, p. 115. ISBN 9812387056. 
  4. Helen R. Quinn, Yossi Nir (2010). The Mystery of the Missing Antimatter. Princeton University Press, p. 249. ISBN 1400835712.