The Physics Travel Guide

Sp(1)

Prerequisites: Quaternions, Lie Groups. Full path (5 pages)

Intuitive

Sp(1)Sp(1) is the group of quaternions of unit length, also known as the compact symplectic group of order one, hence the name Sp(1)Sp(1). (See https://math.ucr.edu/home/baez/symplectic.html for an explanation of the name.)

The group Sp(1)Sp(1) is isomorphic to SU(2)SU(2).

Concrete

Representations

The diagram below shows the defining representation of Sp(1)Sp(1) in its upper branch and the (3-dimensional) adjoint representation of the same group in the lower branch. The latter representation can be used to rotate objects in 3D space and has applications in computer graphics. For a more detailed explanation of this diagram and representations of other Lie groups see Fun with Symmetry.

Contributing authors:

Abstract

Write a quaternion as q=a+b i+c j+d kq = a + b\,i + c\,j + d\,k with i2=j2=k2=ijk=−1i^2=j^2=k^2=ijk=-1 and conjugate qˉ=a−b i−c j−d k\bar q = a - b\,i - c\,j - d\,k. The norm ∣q∣2=qqˉ=a2+b2+c2+d2|q|^2 = q\bar q = a^2+b^2+c^2+d^2 is multiplicative, ∣pq∣=∣p∣∣q∣|pq| = |p||q|, so the unit quaternions form a group Sp(1)={q∈H:∣q∣=1}≅S3.Sp(1) = \{q\in\mathbb{H} : |q| = 1\}\cong S^3 . It is compact, connected and simply connected.

Isomorphism with SU(2)SU(2). The map a+b i+c j+d k ⟼ (a+ibc+id−c+ida−ib)a + b\,i + c\,j + d\,k\ \longmapsto\ \begin{pmatrix} a + ib & c + id\\ -c + id & a - ib\end{pmatrix} sends i↦iσ3i\mapsto i\sigma_3, j↦iσ2j\mapsto i\sigma_2, k↦iσ1k\mapsto i\sigma_1, respects products, and maps unit quaternions onto matrices of the form (αβ−βˉαˉ)\begin{pmatrix}\alpha & \beta\\ -\bar\beta & \bar\alpha\end{pmatrix} with ∣α∣2+∣β∣2=1|\alpha|^2+|\beta|^2=1. These are exactly the elements of SU(2)SU(2).

Lie algebra and rotations. The tangent space at 11 is the space of imaginary quaternions Im H≅R3\mathrm{Im}\,\mathbb{H}\cong\mathbb{R}^3. For imaginary u,vu,v we have uv=−u⃗⋅v⃗+u⃗×v⃗uv = -\vec u\cdot\vec v + \vec u\times\vec v, so the bracket is [u,v]=uv−vu=2 u⃗×v⃗,[u,v] = uv - vu = 2\,\vec u\times\vec v , and sp(1)≅so(3)\mathfrak{sp}(1)\cong\mathfrak{so}(3). The adjoint action v↦qvqˉv\mapsto qv\bar q on imaginary quaternions preserves the norm and orientation, which gives the double cover Sp(1)→SO(3)Sp(1)\to SO(3) with kernel {±1}\{\pm 1\}. The unit quaternion q=cos⁡θ2+sin⁡θ2 n^q = \cos\frac{\theta}{2} + \sin\frac{\theta}{2}\,\hat n (with n^\hat n an imaginary unit quaternion) produces the rotation by θ\theta about n^\hat n. Similarly (p,q)↦(x↦pxqˉ)(p,q)\mapsto(x\mapsto px\bar q) on H≅R4\mathbb{H}\cong\mathbb{R}^4 gives Sp(1)×Sp(1)≅Spin(4)Sp(1)\times Sp(1)\cong\mathrm{Spin}(4), a double cover of SO(4)SO(4).

General nn. Sp(n)Sp(n) is the group of n×nn\times n quaternionic matrices that preserve the standard quaternionic Hermitian form, equivalently Sp(n)=Sp(2n,C)∩U(2n)Sp(n) = Sp(2n,\mathbb{C})\cap U(2n). It is the compact real form of the Lie algebra of type CnC_n. Besides Sp(1)≅SU(2)Sp(1)\cong SU(2), there is the low-dimensional isomorphism Sp(2)≅Spin(5)Sp(2)\cong\mathrm{Spin}(5). The compact group Sp(1)Sp(1) should not be confused with the non-compact real symplectic group Sp(2,R)≅SL(2,R)Sp(2,\mathbb{R})\cong SL(2,\mathbb{R}); the two are different real forms of the same complex group Sp(2,C)≅SL(2,C)Sp(2,\mathbb{C})\cong SL(2,\mathbb{C}).

Path to this page

  1. Imaginary Numbers
  2. Linear Algebra
  3. Group Theory
  4. Quaternions
  5. Lie Groups

Authors: Eduard Sackinger