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The '''Gell-Mann matrices''', named for [[Murray Gell-Mann]], are one possible representation of the [[Lie group#The Lie algebra associated with a Lie group|infinitesimal generator]]s of the [[special unitary group]] called [[Special unitary group#n_.3D_3|SU(3)]]. The [[Lie algebra]] of this group (a real Lie algebra in fact) has dimension eight and therefore it has some set with eight [[Linear independence|linearly independent]] generators, which can be written as <math>g_i</math>, with ''i'' taking values from 1 to 8.  
 
==Defining relations==
 
These Lie Algebra elements  obey the [[Commutator|commutation]] relations
:<math>[g_i, g_j] = if^{ijk} g_k \,</math>  
where a sum over the index ''k'' [[Einstein notation|is implied]]. The structure constants <math>f^{ijk}</math> are completely antisymmetric in the three indices and have values
:<math>f^{123} = 1 \ , \quad f^{147} = f^{165} = f^{246} = f^{257} = f^{345} = f^{376} = \frac{1}{2} \ , \quad f^{458} = f^{678} = \frac{\sqrt{3}}{2} \ . </math>
Any set of [[Hermitian matrices]] which obey these relations qualifies. A particular choice of matrices is called a [[group representation]], because any element of SU(3) can be written in the form <math>\mathrm{exp}(i \theta_j g_j)</math>, where <math>\theta_j</math> are real numbers and a sum over the index ''j'' is implied. Given one representation, another may be obtained by an arbitrary unitary transformation, since that leaves the commutator unchanged.
 
==Particular representations==
 
An important representation involves 3×3 matrices, because the group elements then act on complex vectors with 3 entries, i.e., on the [[fundamental representation]] of the group. A particular choice of this representation is
 
:{| border="0" cellpadding="8" cellspacing="0"
|<math>\lambda_1 = \begin{pmatrix} 0 & 1 & 0 \\ 1 & 0 & 0 \\ 0 & 0 & 0 \end{pmatrix}</math>
|<math>\lambda_2 = \begin{pmatrix} 0 & -i & 0 \\ i & 0 & 0 \\ 0 & 0 & 0 \end{pmatrix}</math>
|<math>\lambda_3 = \begin{pmatrix} 1 & 0 & 0 \\ 0 & -1 & 0 \\ 0 & 0 & 0 \end{pmatrix}</math>
|-
|<math>\lambda_4 = \begin{pmatrix} 0 & 0 & 1 \\ 0 & 0 & 0 \\ 1 & 0 & 0 \end{pmatrix}</math>
|<math>\lambda_5 = \begin{pmatrix} 0 & 0 & -i \\ 0 & 0 & 0 \\ i & 0 & 0 \end{pmatrix}</math>
|
|-
|<math>\lambda_6 = \begin{pmatrix} 0 & 0 & 0 \\ 0 & 0 & 1 \\ 0 & 1 & 0 \end{pmatrix}</math>
|<math>\lambda_7 = \begin{pmatrix} 0 & 0 & 0 \\ 0 & 0 & -i \\ 0 & i & 0 \end{pmatrix}</math>
|<math>\lambda_8 = \frac{1}{\sqrt{3}} \begin{pmatrix} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & -2 \end{pmatrix}</math>
|}
and <math>g_i = \lambda_i/2</math>.  
 
These matrices are [[traceless]], Hermitian, and obey the extra relation <math>\mathrm{tr}(\lambda_i \lambda_j) = 2\delta_{ij}</math>. These properties were chosen by Gell-Mann because they then generalize the [[Pauli matrices]] for [[SU(2)]]. They also naturally extend to general [[SU(n)]], cf.  [[Generalizations of Pauli matrices]].
 
In this representation, it is clear that the [[Cartan subalgebra]] is the set of linear combinations (with real coefficients) of the two matrices <math>\lambda_3</math> and <math>\lambda_8</math>, which commute with each other. There are 3 independent [[SU(2)]] subgroups: <math>\{\lambda_1, \lambda_2, \lambda_3\}</math>, <math>\{\lambda_4, \lambda_5, x\}</math>, and <math>\{\lambda_6, \lambda_7, y\}</math>, where the ''x'' and ''y'' are linear combinations of <math>\lambda_3</math> and <math>\lambda_8</math>.
 
The squared sum of the Gell-Mann matrices gives the [[Casimir operator]]:
 
:<math> C = \sum_{i=1}^8 \lambda_i \lambda_i = 16/3 </math>.
 
These matrices form a useful model to study the internal rotations in the SU(3) space in the [[quark model]] (mixing up of quark colors), and, to a lesser extent, in [[quantum chromodynamics]].
 
==See also==
*[[Generalizations of Pauli matrices]]
*[[Unitary group]]s and [[group representation]]s
*[[Quark model]], [[color charge]] and [[quantum chromodynamics]]
*[[Gluon#Eight_gluon_colors|colors of the Gluon]]
 
==References==
* {{cite book
|last=Georgi |first=H.
|year=1999
|title=Lie Algebras in Particle Physics
|edition=2nd
|publisher=[[Westview Press]]
|isbn=978-0-7382-0233-4
}}
* {{cite book
|last1=Arfken |first1=G. B.
|last2=Weber |first2=H. J.
|last3=Harris |first3=F. E.
|year=2000
|title=Mathematical Methods for Physicists
|edition=7th
|publisher=[[Academic Press]]
|isbn=978-0-12-384654-9
}}
* {{cite book
|last=Kokkedee |first=J. J. J.
|year=1969
|title=The Quark Model
|publisher=[[W. A. Benjamin]]
|lccn=69014391
}}
 
[[Category:Lie groups]]
[[Category:Matrices]]
[[Category:Quantum chromodynamics]]

Revision as of 16:58, 27 November 2013

The Gell-Mann matrices, named for Murray Gell-Mann, are one possible representation of the infinitesimal generators of the special unitary group called SU(3). The Lie algebra of this group (a real Lie algebra in fact) has dimension eight and therefore it has some set with eight linearly independent generators, which can be written as gi, with i taking values from 1 to 8.

Defining relations

These Lie Algebra elements obey the commutation relations

[gi,gj]=ifijkgk

where a sum over the index k is implied. The structure constants fijk are completely antisymmetric in the three indices and have values

f123=1,f147=f165=f246=f257=f345=f376=12,f458=f678=32.

Any set of Hermitian matrices which obey these relations qualifies. A particular choice of matrices is called a group representation, because any element of SU(3) can be written in the form exp(iθjgj), where θj are real numbers and a sum over the index j is implied. Given one representation, another may be obtained by an arbitrary unitary transformation, since that leaves the commutator unchanged.

Particular representations

An important representation involves 3×3 matrices, because the group elements then act on complex vectors with 3 entries, i.e., on the fundamental representation of the group. A particular choice of this representation is

λ1=(010100000) λ2=(0i0i00000) λ3=(100010000)
λ4=(001000100) λ5=(00i000i00)
λ6=(000001010) λ7=(00000i0i0) λ8=13(100010002)

and gi=λi/2.

These matrices are traceless, Hermitian, and obey the extra relation tr(λiλj)=2δij. These properties were chosen by Gell-Mann because they then generalize the Pauli matrices for SU(2). They also naturally extend to general SU(n), cf. Generalizations of Pauli matrices.

In this representation, it is clear that the Cartan subalgebra is the set of linear combinations (with real coefficients) of the two matrices λ3 and λ8, which commute with each other. There are 3 independent SU(2) subgroups: {λ1,λ2,λ3}, {λ4,λ5,x}, and {λ6,λ7,y}, where the x and y are linear combinations of λ3 and λ8.

The squared sum of the Gell-Mann matrices gives the Casimir operator:

C=i=18λiλi=16/3.

These matrices form a useful model to study the internal rotations in the SU(3) space in the quark model (mixing up of quark colors), and, to a lesser extent, in quantum chromodynamics.

See also

References

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