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physics Physics is the natural science that studies matter, its fundamental constituents, its motion and behavior through space and time, and the related entities of energy and force. "Physical science is that department of knowledge which rel ...
, the Gell-Mann–Okubo mass formula provides a sum rule for the masses of
hadron In particle physics, a hadron (; grc, ἁδρός, hadrós; "stout, thick") is a composite subatomic particle made of two or more quarks held together by the strong interaction. They are analogous to molecules that are held together by the ele ...
s within a specific multiplet, determined by their isospin (''I'') and strangeness (or alternatively, hypercharge) :M = a_0 + a_1 Y + a_2 \left I \left( I + 1 \right)-\frac Y^2 \right, where ''a''0, ''a''1, and ''a''2 are
free parameter A free parameter is a variable in a mathematical model which cannot be predicted precisely or constrained by the model and must be estimated experimentally or theoretically. A mathematical model, theory, or conjecture is more likely to be right a ...
s. The rule was first formulated by Murray Gell-Mann in 1961 and independently proposed by Susumu Okubo in 1962. Isospin and hypercharge are generated by SU(3), which can be represented by eight hermitian and traceless matrices corresponding to the "components" of isospin and hypercharge. Six of the matrices correspond to flavor change, and the final two correspond to the third-component of isospin projection, and hypercharge.


Theory

The mass formula was obtained by considering the representations of the
Lie algebra In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an operation called the Lie bracket, an alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow \mathfrak g, that satisfies the Jacobi iden ...
su(3). In particular, the meson octet corresponds to the
root system In mathematics, a root system is a configuration of vectors in a Euclidean space satisfying certain geometrical properties. The concept is fundamental in the theory of Lie groups and Lie algebras, especially the classification and representat ...
of the adjoint representation. However, the simplest, lowest-dimensional representation of su(3) is the fundamental representation, which is three-dimensional, and is now understood to describe the approximate
flavor symmetry In particle physics, flavour or flavor refers to the ''species'' of an elementary particle. The Standard Model counts six flavours of quarks and six flavours of leptons. They are conventionally parameterized with ''flavour quantum numbers'' th ...
of the three
quark A quark () is a type of elementary particle and a fundamental constituent of matter. Quarks combine to form composite particles called hadrons, the most stable of which are protons and neutrons, the components of atomic nuclei. All common ...
s ''u'', ''d'', and ''s''. Thus, the discovery of not only an su(3) symmetry, but also of this workable formula for the mass spectrum was one of the earliest indicators for the existence of quarks. The formula is underlain by the ''octet enhancement hypothesis'', which ascribes dominance of SU(3) breaking to the hypercharge generator of SU(3), Y=\tfracF_8=\operatorname(1,1,-2)/3~, and, in modern terms, the relatively higher mass of the strange quark. This formula is ''phenomenological'', describing an approximate relation between meson and baryon masses, and has been superseded as theoretical work in
quantum chromodynamics In theoretical physics, quantum chromodynamics (QCD) is the theory of the strong interaction between quarks mediated by gluons. Quarks are fundamental particles that make up composite hadrons such as the proton, neutron and pion. QCD is a ty ...
advances, notably chiral perturbation theory.


Baryons

Using the values of relevant ''I'' and ''S'' for baryons, the Gell-Mann–Okubo formula can be rewritten for the baryon octet, :\frac = \frac \, where ''N'', Λ, Σ, and Ξ represent the average mass of corresponding baryons. Using the current mass of baryons, this yields: : \frac = 1128.5~\mathrm/c^2 and : \frac = 1135.25~\mathrm/c^2 meaning that the Gell-Mann–Okubo formula reproduces the mass of octet baryons within ~0.5% of measured values. For the baryon decuplet, the Gell-Mann–Okubo formula can be rewritten as the "equal-spacing" rule :\Delta -\Sigma^* = \Sigma^* - \Xi^* = \Xi^* - \Omega = a_1 + 2a_2 \approx \, -147 ~\mathrm/c^2 where Δ, Σ*, Ξ*, and Ω represent the average mass of corresponding baryons. The baryon decuplet formula famously allowed Gell-Mann to predict the mass of the then undiscovered Ω.


Mesons

The same mass relation can be found for the meson octet, :\frac\left(\frac + \frac\right) = \frac Using the current mass of mesons, this yields : \frac\left(\frac + \frac\right)= 496~\mathrm/c^2 and : \frac = 445~\mathrm/c^2 Because of this large discrepancy, several people attempted to find a way to understand the failure of the GMO formula in mesons, when it worked so well in baryons. In particular, people noticed that using the square of the average masses yielded much better results: :\frac\left \left( \frac \right)^2 + \left( \frac \right)^2\right= \frac This now yields :\frac\left \left( \frac \right)^2 + \left( \frac \right)^2\right 246\times10^3~\mathrm/c^4 and :\frac = 230\times10^3~\mathrm/c^4 which fall within 5% of each other. For a while, the GMO formula involving the square of masses was simply an empirical relationship; but later a justification for using the square of masses was found in the context of chiral perturbation theory, just for pseudoscalar mesons, since these are the pseudogoldstone bosons of dynamically broken chiral symmetry, and, as such, obey Dashen's mass formula. Other, mesons, such as vector ones, need no squaring for the GMO formula to work.


See also

* Gell-Mann–Nishijima formula * Eightfold Way * Quark model * SU(3)


References


Further reading

The following book contains most (if not all) historical papers on the Eightfold Way and related topics, including the Gell-Mann–Okubo mass formula. * {{DEFAULTSORT:Gell-Mann-Okubo mass formula Hadrons Quantum chromodynamics