hypercharge

In particle physics, the hypercharge (a portmanteau of hyperonic and charge) ''Y'' of a particle is a quantum number conserved under the strong interaction. The concept of hypercharge provides a single charge operator that accounts for properties of isospin, electric charge, and flavour. The hypercharge is useful to classify hadrons; the similarly named weak hypercharge has an analogous role in the electroweak interaction.

Definition

Hypercharge is one of two quantum numbers of the SU(3) model of hadrons, alongside isospin . The isospin alone was sufficient for two quark flavours — namely and — whereas presently 6  flavours of quarks are known.

SU(3) weight diagrams (see below) are 2 dimensional, with the coordinates referring to two quantum numbers: (also known as ), which is the  component of isospin, and , which is the hypercharge (defined by strangeness , charm , bottomness , topness , and baryon number ). Mathematically, hypercharge is

:$Y = B + C - S + T' - B' ~.$

Strong interactions conserve hypercharge (and weak hypercharge), but weak interactions do ''not''.

Relation with electric charge and isospin

The Gell-Mann–Nishijima formula relates isospin and electric charge

:$Q = I_3 + \tfracY,$

where ''I''₃ is the third component of isospin and ''Q'' is the particle's charge.

Isospin creates multiplets of particles whose average charge is related to the hypercharge by:
:$Y = 2 \bar Q.$

since the hypercharge is the same for all members of a multiplet, and the average of the ''I''₃ values is 0.

These definitions in their original form hold only for the three lightest quarks.

SU(3) model in relation to hypercharge

The SU(2) model has multiplets characterized by a quantum number ''J'', which is the total angular momentum. Each multiplet consists of substates with equally-spaced values of ''J_z'', forming a symmetric arrangement seen in atomic spectra and isospin. This formalizes the observation that certain strong baryon decays were not observed, leading to the prediction of the mass, strangeness and charge of the baryon.

The SU(3) has ''supermultiplets'' containing SU(2) multiplets. SU(3) now needs two numbers to specify all its sub-states which are denoted by ''λ''₁ and ''λ''₂.

specifies the number of points in the topmost side of the hexagon while specifies the number of points on the bottom side.

Examples

* The nucleon group (protons with and neutrons with ) have an average charge of , so they both have hypercharge (since baryon number and ). From the Gell-Mann–Nishijima formula we know that proton has isospin while neutron has
* This also works for quarks: For the ''up'' quark, with a charge of , and an of , we deduce a hypercharge of , due to its baryon number (since three quarks make a baryon, each quark has a baryon number of ).
* For a ''strange'' quark, with electric charge , a baryon number of , and strangeness −1, we get a hypercharge so we deduce that That means that a ''strange'' quark makes an isospin singlet of its own (the same happens with ''charm'', ''bottom'' and ''top'' quarks), while ''up'' and ''down'' constitute an isospin doublet.
* All other quarks have hypercharge .

Practical obsolescence

Hypercharge was a concept developed in the 1960s, to organize groups of particles in the ''" particle zoo"'' and to develop ''ad hoc'' conservation laws based on their observed transformations. With the advent of the quark model, it is now obvious that strong hypercharge, , is the following combination of the numbers of up (), down (), strange (), charm (), top () and bottom ():

:$Y = \tfrac n_\textrm + \tfrac n_\textrm + \tfrac n_\textrm - \tfrac n_\textrm + \tfrac n_\textrm - \tfrac n_\textrm ~.$

In modern descriptions of hadron interaction, it has become more obvious to draw Feynman diagrams that trace through the individual constituent quarks (which are conserved) composing the interacting baryons and mesons, rather than bothering to count strong hypercharge quantum numbers. ''Weak hypercharge'', however, remains an essential part of understanding the electroweak interaction.

References

*{{cite book , first1=Henry , last1=Semat , first2=John R. , last2=Albright , title=Introduction to Atomic and Nuclear Physics , publisher=Chapman and Hall , year=1984 , isbn=978-0-412-15670-0

Nuclear physics
Quarks
Standard Model
Electroweak theory

he:היפרמטען