# Symplectic group

{{#invoke:Hatnote|hatnote}} Template:Lie groups Template:Group theory sidebar In mathematics, the name symplectic group can refer to two different, but closely related, types of mathematical groups, denoted Sp(2n, F) and Sp(n). The latter is sometimes called the compact symplectic group to distinguish it from the former. Many authors prefer slightly different notations, usually differing by factors of 2. The notation used here is consistent with the size of the matrices used to represent the groups. In Cartan's classification of the simple Lie algebras, the Lie algebra of the complex group Sp(2n, C) is denoted Cn, and Sp(n) is the compact real form of Sp(2n, C).

The name "symplectic group" is due to Hermann Weyl (details) as a replacement for the previous confusing names of (line) complex group and Abelian group, and is the Greek analog of "complex".

## Sp(2n, F)

The symplectic group of degree 2n over a field F, denoted Sp(2n, F), is the group of 2n × 2n symplectic matrices with entries in F, and with the group operation that of matrix multiplication. Since all symplectic matrices have determinant 1, the symplectic group is a subgroup of the special linear group SL(2n, F).

More abstractly, the symplectic group can be defined as the set of linear transformations of a 2n-dimensional vector space over F that preserve a non-degenerate, skew-symmetric, bilinear form, see classical group for this definition. Such a vector space is called a symplectic vector space. The symplectic group of an abstract symplectic vector space V is also denoted Sp(V).

Typically, the field F is the field of real numbers, R, or complex numbers, C. In this case Sp(2n, F) is a real/complex Lie group of real/complex dimension n(2n + 1). These groups are connected but non-compact.

The centre of Sp(2n, F) consists of the matrices I2n and -I2n as long as the characteristic of the field is not equal to 2. Note that I2n denotes the 2n × 2n identity matrix.

The real rank of the Lie Algebra, and hence, the Lie Group for Sp(2n, F) is n.

The condition that a symplectic matrix preserves the symplectic form can be written as

$S\in \operatorname {Sp} (2n,F)\quad {\text{iff}}\quad S^{T}\Omega S=\Omega$ where AT is the transpose of A and

$\Omega ={\begin{pmatrix}0&I_{n}\\-I_{n}&0\\\end{pmatrix}}.$ The Lie algebra of Sp(2n, F) is given by the set of 2n × 2n matrices A (with entries in F) that satisfy

$\Omega A+A^{\mathrm {T} }\Omega =0.$ When n = 1, the symplectic condition on a matrix is satisfied if and only if the determinant is one, so that Sp(2, F) = SL(2, F). For n > 1, there are additional conditions, i.e. Sp(2n, F) is then a proper subgroup of SL(2n, F).

### Sp(2n, C)

The symplectic group over the field of complex numbers is a non-compact, simply connected, simple Lie group.

### Sp(2n, R)

Sp(2n, C) is the complexification of the real group Sp(2n, R). Sp(2n, R) is a real, non-compact, connected, simple Lie group. It has a fundamental group isomorphic to the group of integers under addition. As the real form of a simple Lie group its Lie algebra is a splittable Lie algebra.

Note that the exponential map from the Lie algebra sp(2n, R) to the group Sp(2n, R) is not surjective. However, any element of the group may be generated by the group multiplication of two elements. In other words

$\forall \;S\in \operatorname {Sp} (2n,\mathbb {R} )\;\exists \;X,Y\in {\mathfrak {sp}}(2n,\mathbb {R} ){\text{ such that }}S=e^{X}e^{Y}.$ Any real symplectic matrix can be decomposed as a product of three matrices:

$S=O{\begin{pmatrix}D&0\\0&D^{-1}\end{pmatrix}}O',$ such that O and O' are symplectic and orthogonal and D is positive-definite and diagonal. This decomposition is closely related to the singular value decomposition of a matrix. It is known as Euler decomposition and has an intuitive link with the Euler decomposition of a rotation.

### Infinitesimal generators

The members of the symplectic Lie algebra sp(2n, F) are the Hamiltonian matrices.

$Q={\begin{pmatrix}A&B\\C&-A^{\mathrm {T} }\end{pmatrix}}$ where B and C are symmetric matrices. See classical group for a derivation.

### Example of symplectic matrices

For Sp(2,R), the group of 2 × 2 matrices with determinant 1, the three symplectic (0, 1)-matrices are:

${\begin{pmatrix}1&0\\0&1\end{pmatrix}},\quad {\begin{pmatrix}1&0\\1&1\end{pmatrix}}\quad {\text{and}}\quad {\begin{pmatrix}1&1\\0&1\end{pmatrix}}.$ ## Sp(n)

The compact symplectic group Sp(n) is often written as USp(2n), indicating the fact that it is isomorphic to the group of unitary symplectic matrices, Sp(n) ≅ U(2n) ∩ Sp(2n, C). Although the Sp(n) notation is more common, and hence used here, it can be confusing in that the general idea of the symplectic group - including the compact, real and complex forms - can be represented as Sp(n). For example this is used in the sidebar at the top of this page in the list of classical groups.

Sp(n) is the subgroup of GL(n, H) (invertible quaternionic matrices) that preserves the standard hermitian form on Hn:

$\langle x,y\rangle ={\bar {x}}_{1}y_{1}+\cdots +{\bar {x}}_{n}y_{n}$ That is, Sp(n) is just the quaternionic unitary group, U(n, H). Indeed, it is sometimes called the hyperunitary group. Also Sp(1) is the group of quaternions of norm 1, equivalent to SU(2) and topologically a 3-sphere S3.

Note that Sp(n) is not a symplectic group in the sense of the previous section—it does not preserve a non-degenerate skew-symmetric (H-bilinear) form on Hn (in fact, the only skew-symmetric form is the zero form). Rather, it is isomorphic to a subgroup of Sp(2n, C), and so does preserve a complex symplectic form in a vector space of dimension twice as high. As explained below, the Lie algebra of Sp(n) is a real form of the complex symplectic Lie algebra sp(2n, C).

Sp(n) is a real Lie group with (real) dimension n(2n + 1). It is compact, connected, and simply connected.

The Lie algebra of Sp(n) is given by the quaternionic skew-Hermitian matrices, the set of n-by-n quaternionic matrices that satisfy

$A+A^{\dagger }=0$ where A is the conjugate transpose of A (here one takes the quaternionic conjugate). The Lie bracket is given by the commutator.

### Important subgroups

The compact symplectic group Sp(n) comes up in quantum physics as a symmetry on Poisson brackets so it is important to understand its subgroups. Some main subgroups are:

$\operatorname {Sp} (n)\supset \operatorname {Sp} (n-1)$ $\operatorname {Sp} (n)\supset \operatorname {U} (n)$ $\operatorname {Sp} (2)\supset \operatorname {O} (4)$ Conversely it is itself a subgroup of some other groups:

$\operatorname {SU} (2n)\supset \operatorname {Sp} (n)$ $\operatorname {F} _{4}\supset \operatorname {Sp} (4)$ $\operatorname {G} _{2}\supset \operatorname {Sp} (1)$ There are also the isomorphisms of the Lie algebras sp(2) = so(5) and sp(1) = so(3) = su(2).

## Relationship between the symplectic groups

Every complex, semisimple Lie algebra has a split real form and a compact real form; the former is called a complexification of the latter two.

The Lie algebra of Sp(2n, C) is semisimple and is denoted sp(2n, C). Its split real form is sp(2n, R) and its compact real form is sp(n). These correspond to the Lie groups Sp(2n, R) and Sp(n) respectively.

The algebras, sp(p, np), which are the Lie algebras of Sp(p, np), are the indefinite signature equivalent to the compact form.

## Physical significance

### Classical mechanics

Consider a system of n particles, evolving under Hamilton's equations whose position in phase space at a given time is denoted by the vector of canonical coordinates,

$\mathbf {z} =(q_{1},\ldots ,q_{n},p_{1},\ldots ,p_{n})^{T}.$ The elements of the group Sp(2n, R) are canonical transformations on this vector, i.e. they preserve the form of Hamilton's equations.

### Quantum mechanics

Consider a system of n particles whose quantum state encodes its position and momentum. These coordinates are continuous variables and hence the Hilbert space, in which the state lives, is infinite-dimensional. This often makes the analysis of this situtation tricky. An alternative approach is to consider the evolution of the position and momentum operators under the Heisenberg equation in phase space.

Construct a vector of canonical coordinates,

$\mathbf {\hat {z}} =({\hat {q}}_{1},\ldots ,{\hat {q}}_{n},{\hat {p}}_{1},\ldots ,{\hat {p}}_{n})^{T}.$ The canonical commutation relation can be expressed simply as

$[\mathbf {\hat {z}} ,\mathbf {\hat {z}} ^{T}]=i\hbar \Omega$ where

$\Omega ={\begin{pmatrix}\mathbf {0} &I_{n}\\-I_{n}&\mathbf {0} \end{pmatrix}}$ and In is the n × n identity matrix.

Most physical situtations only require quadratic Hamiltonians, i.e. Hamiltonians of the form

${\hat {H}}={\frac {1}{2}}\mathbf {\hat {z}} ^{T}K\mathbf {\hat {z}}$ where K is a 2n × 2n real, symmetric matrix. This turns out to be a useful restriction and allows us to rewrite the Heisenberg equation as

${\frac {d\mathbf {\hat {z}} }{dt}}=\Omega K\mathbf {\hat {z}}$ The solution to this equation must preserve the canonical commutation relation. It can be shown that the time-evolution of this system is equivalent to an action of the real symplectic group, Sp(2n, R), on the initial state.