Physlib.Mathematics.Groups.SpecialUnitary.LieAlgebra.Basic
The Lie algebra `su(n)` in the hermitian presentation
i. Overview
In physics, `su(n)` is described through generators `T^a`, `a = 1, …, n² - 1`, a basis of the traceless hermitian `n × n` complex matrices, satisfying `[T^a, T^b] = i f_{abc} T^c` with real structure constants `f_{abc}`. Here `i` is the imaginary unit and the repeated index `c` is summed. This file makes the traceless hermitian matrices into a real Lie algebra with the bracket `⁅x, y⁆ = i (x y - y x)`, on which the unitary group acts by conjugation. The construction allows entries in any commutative `*`-ring `R` that is both a real and a complex `*`-algebra, as `SULieAlgebra n R`; the Lie algebra `su(n)` itself is `SULieAlgebra n ℂ`.
ii. Key results
- `SULieAlgebra n R` : traceless hermitian `n × n` matrices over `R`, as a real Lie algebra.
- `SULieAlgebra.conj` : the representation `x ↦ U x U†` of the unitary group.
- `SULieAlgebra.conj_lie` : conjugation by a unitary matrix preserves the bracket.
- `SULieAlgebra.Complexification n` : the complexification `ℂ ⊗[ℝ] su(n)`.
iii. Table of contents
- A. Traceless hermitian matrices
- B. The conjugation representation
- C. The bracket
- D. Conjugation preserves the bracket
- E. The complexification
iv. References
* None.
A. Traceless hermitian matrices
Since `i A` is skew-hermitian when `A` is hermitian, the traceless hermitian matrices form a real vector space.
B. The conjugation representation
Conjugation `x ↦ U x U†` by a unitary matrix `U` preserves traceless hermitian matrices, by `U† U = 1` and cyclicity of the trace, and defines a representation of the unitary group.
C. The bracket
From here on `R` is also a complex `*`-algebra, so that matrices can be multiplied by `i`. The commutator of two hermitian matrices is skew-hermitian, and multiplying it by `i` makes it hermitian again, giving the bracket `⁅x, y⁆ = i (x y - y x)`. Being `i` times the commutator, it is a Lie bracket.
Since `[i x, i y] = i ⁅x, y⁆`, multiplication by `i` turns this bracket into the commutator of traceless skew-hermitian matrices, the usual mathematical presentation of `su(n)`.
The factor `i` flips the sign of the structure constants; if `[T^a, T^b] = i f_{abc} T^c`, then `⁅T^a, T^b⁆ = -f_{abc} T^c`.
D. Conjugation preserves the bracket
E. The complexification
30 declarations
-submodule of traceless hermitian matrices
Let be a commutative -ring that is also a real -algebra. `SULieAlgebra.submodule n R` is the -submodule of matrices over consisting of matrices that are self-adjoint () and have zero trace (). This is formally defined as the intersection of the submodule of self-adjoint matrices and the kernel of the trace linear map.
The Lie algebra of traceless hermitian matrices over
Let be a natural number and be a commutative -ring that is also a real -algebra. The type `SULieAlgebra n R` is defined as the space of matrices with entries in that are self-adjoint () and have zero trace (). In the case where , this corresponds to the Lie algebra in the hermitian presentation.
element from a traceless hermitian matrix
Given an matrix with entries in a commutative -ring , a proof that is self-adjoint (), and a proof that its trace is zero (), this function constructs the corresponding element in the Lie algebra (represented by the type `SULieAlgebra n R`).
The underlying matrix of an element in constructed from is
Let be a commutative -ring that is also a real -algebra. Given an matrix over that is hermitian () and has zero trace (), the underlying matrix of the element in the Lie algebra constructed from using `ofMatrix` is equal to .
for
Let be a commutative -ring that is also a real -algebra. For any element in the Lie algebra (the space of traceless hermitian matrices), its underlying matrix is self-adjoint (hermitian), satisfying .
Trace of elements in is zero
Let be a commutative -ring that is also a real -algebra. For any element in the Lie algebra of traceless hermitian matrices , the trace of its underlying matrix is zero, i.e., .
Conjugation representation of on
Let be a commutative -ring that is also a real -algebra. The term `SULieAlgebra.conj` defines the group representation of the unitary group on the real Lie algebra of traceless hermitian matrices. For a unitary matrix and an element , the action is given by the conjugation , where denotes the adjoint (conjugate transpose) of the matrix .
The conjugation action on is
Let be a commutative -ring that is also a real -algebra. For any unitary matrix and any traceless hermitian matrix , the conjugation representation action is given by the matrix product , where denotes the adjoint (conjugate transpose) of .
Lie bracket on as
For any two elements and in the Lie algebra of traceless hermitian matrices (represented by `SULieAlgebra n R`), the bracket operation is defined as times their commutator: where is the imaginary unit. This definition ensures that the resulting matrix remains both hermitian and traceless.
The matrix of the Lie bracket in is
For any elements and in the Lie algebra of traceless hermitian matrices (represented by `SULieAlgebra n R`), the underlying matrix of their Lie bracket is equal to , where is the imaginary unit and is the commutator of the matrices and .
is a Lie ring
For a natural number and a commutative -ring that is also a real -algebra, the space of traceless hermitian matrices `SULieAlgebra n R` forms a Lie ring. The Lie bracket is defined as , where is the imaginary unit. This structure ensures that the bracket operation satisfies the axioms of a Lie ring, including bilinearity, the alternating property , and the Jacobi identity.
is a Lie algebra over
For a natural number and a commutative -ring that is a real -algebra, the space of traceless hermitian matrices forms a Lie algebra over the real numbers . The Lie bracket is given by , where is the imaginary unit. This structure signifies that the Lie bracket is -bilinear.
Conjugation by a Unitary Matrix Preserves the Lie Bracket on
Let be a commutative -ring that is also a real -algebra. For any natural number , let be the real Lie algebra of traceless hermitian matrices over , equipped with the Lie bracket , where is the imaginary unit. For any unitary matrix in the unitary group , the conjugation action (where denotes the adjoint or conjugate transpose) preserves the Lie bracket, meaning that for all : This implies that the conjugation action by a unitary matrix defines a Lie algebra automorphism on .
Complexification of
For a natural number , the complexification of the Lie algebra is the complex Lie algebra defined by the tensor product , where is the real Lie algebra consisting of complex matrices that are traceless () and hermitian ().
Matrix of an element in the complexification of
The -linear map from the complexification of the Lie algebra (denoted ) to the space of complex matrices that sends a tensor to the matrix , where and is a traceless hermitian matrix.
for the complexification of
Let and let be an traceless hermitian matrix. The -linear map from the complexification to the space of complex matrices maps the elementary tensor to the matrix .
for elements in the complexification of
For any element in the complexification of the Lie algebra (denoted ), the trace of the corresponding complex matrix is zero, i.e., .
for the complexification of
For any elements in the complexification of the Lie algebra (denoted ), the -linear map maps their Lie bracket to times the commutator of their corresponding matrices: where is the imaginary unit. This identity reflects the hermitian presentation of , where the bracket is times the standard commutator.
Element of from a matrix with
Given an complex matrix and a proof that its trace is zero (), this function constructs the corresponding element in the complexified Lie algebra . The element is defined as , where and are the traceless hermitian matrices that form the "real" and "imaginary" parts of in the hermitian presentation of .
for traceless complex matrices
Let be an complex matrix with trace zero (). Then the image of the element under the linear map is equal to . This identity reflects the decomposition into its traceless hermitian parts.
`ofTracelessℂ (M + N) = ofTracelessℂ M + ofTracelessℂ N`
For any complex matrices and such that and , the map (which constructs an element of the complexified Lie algebra from a traceless matrix) is additive. That is,
for the complexification of
For any element in the complexification of the Lie algebra (denoted ), applying the construction map to its matrix representation recovers the original element . That is, Here, is the -linear map that sends a tensor to the matrix , and is the map that takes a traceless matrix and returns the element in the complexification.
The matrix map for the complexification of is injective
Let be the real Lie algebra of traceless hermitian matrices. The -linear map , which sends the tensor to the matrix for and , is injective. This implies that an element of the complexification is uniquely determined by its matrix.
The range of the matrix map from the complexification of consists of all traceless matrices
Let be the real Lie algebra of traceless hermitian matrices and let be its complexification. Let be the -linear map that sends a tensor to the matrix , where and . The range of is equal to the kernel of the trace linear map , which consists of all complex matrices such that .
Matrices commuting with commute with all matrices
Let be a natural number and let be an complex matrix. If commutes with every matrix in the Lie algebra (the space of traceless hermitian matrices over ), then commutes with every complex matrix .
-linear equivalence
For a natural number , let be the real Lie algebra of complex matrices that are traceless () and hermitian (). This definition provides a -linear equivalence between the complexification of this Lie algebra, , and the subspace of complex matrices with zero trace. The map sends an element of the complexification to its corresponding matrix representation.
Matrix Value of equals
For any element in the complexification of the Lie algebra (denoted ), the underlying matrix of its image under the -linear equivalence is equal to its matrix representation .
Let be a natural number and be an complex matrix with zero trace (). Let be the inverse of the -linear equivalence between the complexification of the Lie algebra (denoted ) and the subspace of traceless matrices. Let be the linear map that sends an element of the complexification to its matrix representation in . Then, .
Let be the real Lie algebra of complex matrices that are traceless and hermitian. The dimension of the complexification as a vector space over the complex numbers is .
Let be the Lie algebra of complex matrices that are traceless and hermitian (satisfying and ). The dimension of as a vector space over the real numbers is .
