Special unitary group
Algebraic structure → Group theory Group theory 


Modular groups

Infinite dimensional Lie group

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In mathematics, the special unitary group of degree n, denoted SU(n), is the Lie group of n×n unitary matrices with determinant 1. The group operation is matrix multiplication. The special unitary group is a subgroup of the unitary group U(n), consisting of all n×n unitary matrices. As a compact classical group, U(n) is the group that preserves the standard inner product on C^{n}.^{[nb 1]} It is itself a subgroup of the general linear group, SU(n) ⊂ U(n) ⊂ GL(n, C).
The SU(n) groups find wide application in the Standard Model of particle physics, especially SU(2) in the electroweak interaction and SU(3) in quantum chromodynamics.^{[1]}
The simplest case, SU(1), is the trivial group, having only a single element. The group SU(2) is isomorphic to the group of quaternions of norm 1, and is thus diffeomorphic to the 3sphere. Since unit quaternions can be used to represent rotations in 3dimensional space (up to sign), there is a surjective homomorphism from SU(2) to the rotation group SO(3) whose kernel is {+I, −I}.^{[nb 2]} SU(2) is also identical to one of the symmetry groups of spinors, Spin(3), that enables a spinor presentation of rotations.
Properties
The special unitary group SU(n) is a real Lie group (though not a complex Lie group). Its dimension as a real manifold is n^{2} − 1. Topologically, it is compact and simply connected.^{[2]} Algebraically, it is a simple Lie group (meaning its Lie algebra is simple; see below).^{[3]}
The center of SU(n) is isomorphic to the cyclic group Z_{n}, and is composed of the diagonal matrices ζ I for ζ an n^{th} root of unity and I the n×n identity matrix.
Its outer automorphism group, for n ≥ 3, is Z_{2}, while the outer automorphism group of SU(2) is the trivial group.
A maximal torus, of rank n − 1, is given by the set of diagonal matrices with determinant 1. The Weyl group is the symmetric group S_{n}, which is represented by signed permutation matrices (the signs being necessary to ensure the determinant is 1).
The Lie algebra of SU(n), denoted by su(n), can be identified with the set of traceless antihermitian n×n complex matrices, with the regular commutator as Lie bracket. Particle physicists often use a different, equivalent representation: the set of traceless hermitian n×n complex matrices with Lie bracket given by −i times the commutator.
Infinitesimal generators
The Lie algebra su(n) can be generated by n^{2} operators , i, j= 1, 2, ..., n, which satisfy the commutator relationships
for i, j, k, ℓ = 1, 2, ..., n, where δ_{jk} denotes the Kronecker delta. Additionally, the operator
satisfies
which implies that the number of independent generators of the Lie algebra is n^{2} − 1 .^{[4]}
Fundamental representation
In the defining, or fundamental, representation of su(n) the generators T_{a} are represented by traceless hermitian complex n×n matrices, where:
where the f are the structure constants and are antisymmetric in all indices, while the dcoefficients are symmetric in all indices. As a consequence:
We also take
as a normalization convention.
Adjoint representation
In the (n^{2} − 1) dimensional adjoint representation, the generators are represented by (n^{2} − 1) × (n^{2} − 1) matrices, whose elements are defined by the structure constants themselves:
n = 2
SU(2) is the following group,^{[5]}
where the overline denotes complex conjugation.
Now, consider the following map,
where M(2, C) denotes the set of 2 by 2 complex matrices. By considering C^{2} diffeomorphic to R^{4} and M(2, C) diffeomorphic to R^{8}, we can see that φ is an injective real linear map and hence an embedding. Now, considering the restriction of φ to the 3sphere (since modulus is 1), denoted S^{3}, we can see that this is an embedding of the 3sphere onto a compact submanifold of M(2, C). However, it is also clear that φ(S^{3}) = SU(2).
Therefore, as a manifold S^{3} is diffeomorphic to SU(2) and so SU(2) is a compact, connected Lie group.
The Lie algebra of SU(2) is
It is easily verified that matrices of this form have trace zero and are antihermitian. The Lie algebra is then generated by the following matrices,
which are easily seen to have the form of the general element specified above.
These satisfy u_{3}u_{2} = −u_{2}u_{3} = −u_{1} and u_{2}u_{1} = −u_{1}u_{2} = −u_{3}. The commutator bracket is therefore specified by
The above generators are related to the Pauli matrices by u_{1} = i σ_{1},u_{2} = −i σ_{2} and u_{3} = i σ_{3}. This representation is routinely used in quantum mechanics to represent the spin of fundamental particles such as electrons. They also serve as unit vectors for the description of our 3 spatial dimensions in loop quantum gravity.
The Lie algebra serves to work out the representations of SU(2).
n = 3
The generators of SU(3), T, in the defining representation, are:
where λ, the GellMann matrices, are the SU(3) analog of the Pauli matrices for SU(2):
These λ_{a} span all traceless Hermitian matrices H of the Lie algebra, as required. Note that λ_{2}, λ_{5}, λ_{7} are antisymmetric.
They obey the relations
 ,
 (or, equivalently, ).
The f are the structure constants of the Lie algebra, given by:
while all other f_{abc} not related to these by permutation are zero. In general, they vanish, unless they contain an odd number of indices from the set {2,5,7}.^{[nb 3]}
The symmetric coefficients d take the values:
They vanish if the number of indices from the set {2,5,7} is odd.
As a topological space, SU(3) is a nontrivial, locally trivial bundle of a 3sphere over a 5sphere.
A generic SU(3) group element generated by a traceless 3×3 hermitian matrix H, normalized as tr(H^{2}) = 2 , is given by^{[6]}
where
See also Clebsch–Gordan coefficients for SU(3) for elementary representation theory facts.
Lie algebra structure
The above representation bases generalize to n > 3, using generalized Pauli matrices.
If we choose an (arbitrary) particular basis, then the subspace of traceless diagonal n×n matrices with imaginary entries forms an (n − 1)dimensional Cartan subalgebra.^{[7]}
Complexify the Lie algebra, so that any traceless n×n matrix is now allowed. The weight eigenvectors are the Cartan subalgebra itself, as well as the matrices with only one nonzero entry which is off diagonal. Even though the Cartan subalgebra h is only (n − 1)dimensional, to simplify calculations, it is often convenient to introduce an auxiliary element, the unit matrix which commutes with everything else (which is not an element of the Lie algebra!) for the purpose of computing weights—and that only. So, we have a basis where the ith basis vector is the matrix with 1 on the ith diagonal entry and zero elsewhere. Weights would then be given by n coordinates and the sum over all n coordinates has to be zero (because the unit matrix is only auxiliary).
So, SU(n) is of rank n − 1 and its Dynkin diagram is given by A_{n−1}, a chain of n − 1 vertices, o−o−o−oo.^{[8]} Its root system consists of n(n − 1) roots spanning a n − 1 Euclidean space. Here, we use n redundant coordinates instead of n − 1 to emphasize the symmetries of the root system (the n coordinates have to add up to zero).
In other words, we are embedding this n − 1 dimensional vector space in an ndimensional one. Thus, the roots consists of all the n(n − 1) permutations of (1, −1, 0, ..., 0). The construction given above explains why. A choice of simple roots is
Its Cartan matrix is
Its Weyl group or Coxeter group is the symmetric group S_{n}, the symmetry group of the (n − 1)simplex.
Generalized special unitary group
For a field F, the generalized special unitary group over F, SU(p, q; F), is the group of all linear transformations of determinant 1 of a vector space of rank n = p + q over F which leave invariant a nondegenerate, Hermitian form of signature (p, q). This group is often referred to as the special unitary group of signature p q over F. The field F can be replaced by a commutative ring, in which case the vector space is replaced by a free module.
Specifically, fix a Hermitian matrix A of signature p q in GL(n, R), then all
satisfy
Often one will see the notation SU(p, q) without reference to a ring or field; in this case, the ring or field being referred to is C and this gives one of the classical Lie groups. The standard choice for A when F = C is
However, there may be better choices for A for certain dimensions which exhibit more behaviour under restriction to subrings of C.
Example
An important example of this type of group is the Picard modular group SU(2, 1; Z[i]) which acts (projectively) on complex hyperbolic space of degree two, in the same way that SL(2,9;Z) acts (projectively) on real hyperbolic space of dimension two. In 2005 Gábor Francsics and Peter Lax computed an explicit fundamental domain for the action of this group on HC^{2}.^{[9]}
A further example is SU(1, 1; C), which is isomorphic to SL(2,R).
Important subgroups
In physics the special unitary group is used to represent bosonic symmetries. In theories of symmetry breaking it is important to be able to find the subgroups of the special unitary group. Subgroups of SU(n) that are important in GUT physics are, for p > 1, n − p > 1 ,
where × denotes the direct product and U(1), known as the circle group, is the multiplicative group of all complex numbers with absolute value 1.
For completeness, there are also the orthogonal and symplectic subgroups,
Since the rank of SU(n) is n − 1 and of U(1) is 1, a useful check is that the sum of the ranks of the subgroups is less than or equal to the rank of the original group. SU(n) is a subgroup of various other Lie groups,
See spin group, and simple Lie groups for E_{6}, E_{7}, and G_{2}.
There are also the accidental isomorphisms: SU(4) = Spin(6) , SU(2) = Spin(3) = Sp(1) ,^{[nb 4]} and U(1) = Spin(2) = SO(2) .
One may finally mention that SU(2) is the double covering group of SO(3), a relation that plays an important role in the theory of rotations of 2spinors in nonrelativistic quantum mechanics.
See also
Remarks
 ↑ For a characterization of U(n) and hence SU(n) in terms of preservation of the standard inner product on ℂ^{n}, see Classical group.
 ↑ For an explicit description of the homomorphism SU(2) → SO(3), see Connection between SO(3) and SU(2).
 ↑ So fewer than 1/6 of all f_{abc}s are nonvanishing.
 ↑ Sp(n) is the compact real form of Sp(2n, C). It is sometimes denoted USp(2n). The dimension of the Sp(n)matrices is 2n × 2n.
References
 ↑ Halzen, Francis; Martin, Alan (1984). Quarks & Leptons: An Introductory Course in Modern Particle Physics. John Wiley & Sons. ISBN 0471887412.
 ↑ Hall 2015 Proposition 13.11
 ↑ Wybourne, B G (1974). Classical Groups for Physicists, WileyInterscience. ISBN 0471965057 .
 ↑ R.R. Puri, Mathematical Methods of Quantum Optics, Springer, 2001.
 ↑ Hall 2015 Exercise 1.5
 ↑ Rosen, S P (1971). "Finite Transformations in Various Representations of SU(3)". Journal of Mathematical Physics. 12 (4): 673. doi:10.1063/1.1665634.; Curtright, T L; Zachos, C K (2015). "Elementary results for the fundamental representation of SU(3)". Reports On Mathematical Physics. 76: 401–404. doi:10.1016/S00344877(15)300409.
 ↑ Hall 2015 Section 7.7.1
 ↑ Hall 2015 Section 8.10.1
 ↑ Francsics, Gabor; Lax, Peter D. "An Explicit Fundamental Domain For The Picard Modular Group In Two Complex Dimensions". arXiv:math/0509708v1.
 Hall, Brian C. (2015), Lie Groups, Lie Algebras, and Representations: An Elementary Introduction, Graduate Texts in Mathematics, 222 (2nd ed.), Springer
 Iachello, Francesco (2006), Lie Algebras and Applications, Lecture Notes in Physics, 708, Springer, ISBN 3540362363