The Anti-Quaternion Subspace under the Three Topologies
Introduction
The anti-quaternion subspace $i\mathbb{H}_{\mathbb{B}}$ is one of the six distinguished subspaces of the biquaternion algebra $\mathbb{B}$, defined and developed in Introduction to the Six Subspaces in the Algebra group. It reads the subspace for its basis, its defining involution, its algebra and module structure and its elements; this one reads it for its topology, and it does so three times.
The algebra carries three pairings of its elements — the bilinear form $B$, the Hermitian form $\langle\cdot,\cdot\rangle$ and the Krein form $[\cdot,\cdot]$ of The Three Pairings of the Biquaternion Algebra, built on the natural conjugation ${}^{\natural}$, the Hermitian conjugation ${}^{*}$ and the complex conjugation $\bar{\cdot}$. Each pairing restricts to the subspace, and each restriction is a form in its own right, with its own signature, its own definiteness, its own null set and its own group of isometries; each therefore induces its own topology on the subspace. The three are kept apart in three separate sections below, and they are compared in the table at the end.
Conventions. $\mathbb{B}=\mathbb{C}\otimes_{\mathbb{R}}\mathbb{H}$, the element $\tilde{Q}=\sum_{\mu}Q_{\mu}e_{\mu}$ with $Q_{\mu}=q_{\mu}+iq'_{\mu}$, units $e_0=1$ and $e_k^2=-e_0$, central scalar imaginary $i$, scalar part $\mathrm{Sc}$, sign vector $\varepsilon=(1,-1,-1,-1)$ and $E=\mathrm{diag}(1,-1,-1,-1)$.
The Subspace
Definition. The anti-quaternion subspace is the anti-fixed space of complex conjugation, $i\mathbb{H}_{\mathbb{B}}=\{\tilde{Q}:\bar{\tilde{Q}}=-\tilde{Q}\}$. It is the set of elements with purely imaginary coefficients.
It is $\mathrm{span}_{\mathbb{R}}\{ie_0,ie_1,ie_2,ie_3\}$, of real dimension $4$; it is $i$ times the quaternion subspace, and it is not a subalgebra.
The Topology Induced by the Bilinear Form
Theorem (the restriction of the bilinear form). On $i\mathbb{H}_{\mathbb{B}}$ the bilinear form is
$$ B(\tilde{Q},\tilde{Q}) = N(\tilde{Q}) = -\sum_\mu(q'_\mu)^2 , $$
a real form of signature $(0,4)$ on the 4 real dimensions of the subspace.
Proof. On the subspace $Q_\mu=iq'_\mu$, so $N(\tilde{Q})=\sum_\mu(iq'_\mu)^2=-\sum_\mu(q'_\mu)^2$ is a negative sum of four real squares.
The restriction is negative definite, the exact negative of the restriction to the quaternion subspace, the two being exchanged by multiplication by $i$.
The null set. The form is negative definite, so the origin is its only isotropic point; the subspace carries no zero divisor and no nilpotent element.
The isometry group. The restriction is a real form of signature $(0,4)$, so its group of real-linear isometries on $i\mathbb{H}_{\mathbb{B}}$ is the orthogonal group $O(0,4)$; inside the ambient isometry group $O_4(\mathbb{C})$ of The Three Pairings of the Biquaternion Algebra the elements that preserve $i\mathbb{H}_{\mathbb{B}}$ form the corresponding subgroup.
The Topology Induced by the Hermitian Form
Theorem (the restriction of the Hermitian form). On $i\mathbb{H}_{\mathbb{B}}$ the Hermitian form is
$$ \langle\tilde{Q},\tilde{Q}\rangle = \sum_\mu(q'_\mu)^2 , $$
of signature $(4,0)$.
Proof. $\langle\tilde{Q},\tilde{Q}\rangle=\sum_\mu|Q_\mu|^2=\sum_\mu|iq'_\mu|^2=\sum_\mu(q'_\mu)^2$.
The Hermitian restriction is positive definite and is the negative of the bilinear one: the two forms differ by exactly the sign $i^2=-1$ on the subspace.
The Euclidean topology. The restriction is positive definite, so it is a Euclidean inner product on the 4 real dimensions of the subspace. It defines the Euclidean norm $\lVert\tilde{Q}\rVert_E$, the distance and the balls, and hence the Euclidean topology of the subspace; on the algebra as a whole this is the topology of The Euclidean Topology of the Biquaternion Algebra. Its group of real-linear isometries on $i\mathbb{H}_{\mathbb{B}}$ is the compact orthogonal group $O(4)$, contained in the ambient unitary group $U(4)$ of The Unitary Group of the Biquaternion Algebra.
The null set. The form is positive definite, so $\langle\tilde{Q},\tilde{Q}\rangle=0$ holds only at $\tilde{Q}=0$: the subspace carries no isotropic vector for the Hermitian form.
The Topology Induced by the Krein Form
Theorem (the restriction of the Krein form). On $i\mathbb{H}_{\mathbb{B}}$ the Krein form is
$$ [\tilde{Q},\tilde{Q}] = (q'_0)^2-(q'_1)^2-(q'_2)^2-(q'_3)^2 , $$
of signature $(1,3)$.
Proof. $[\tilde{Q},\tilde{Q}]=\sum_\mu\varepsilon_\mu|Q_\mu|^2=\sum_\mu\varepsilon_\mu(q'_\mu)^2$ with $\varepsilon=(1,-1,-1,-1)$.
The restriction is Lorentzian of signature $(1,3)$, a second copy of Minkowski space, this time with the time direction the imaginary scalar line $i\mathbb{R}e_0$.
The null set. the cone $(q'_0)^2=(q'_1)^2+(q'_2)^2+(q'_3)^2$, of real dimension $3$, the light cone of the Minkowski form carried by the imaginary coefficients.
The isometry group. The restriction is a real form of signature $(1,3)$, so its group of real-linear isometries on $i\mathbb{H}_{\mathbb{B}}$ is $O(1,3)$; inside the ambient group $U(1,3)$ of The Krein Isometry Group and Its $J$-Contractions the elements preserving $i\mathbb{H}_{\mathbb{B}}$ form the corresponding subgroup.
The Three Topologies Compared
The three restrictions are collected in one table; each entry is a form on the same real vector space $i\mathbb{H}_{\mathbb{B}}$, and the signatures are those of the underlying real form.
| topology | form | restriction on $i\mathbb{H}_{\mathbb{B}}$ | signature | definiteness | null set | isometry group |
|---|---|---|---|---|---|---|
| bilinear | $B=\mathrm{Sc}(\tilde{Q}^{\natural}\tilde{Q})$ | $-\sum_\mu(q'_\mu)^2$ | $(0,4)$ | negative definite | $\{0\}$ | $O(0,4)$ |
| Hermitian | $\langle\tilde{Q},\tilde{Q}\rangle=\mathrm{Sc}(\tilde{Q}^{*}\tilde{Q})$ | $\sum_\mu(q'_\mu)^2$ | $(4,0)$ | positive definite | $\{0\}$ | $O(4)$ |
| Krein | $[\tilde{Q},\tilde{Q}]=\mathrm{Sc}(\bar{\tilde{Q}}\tilde{Q})$ | $(q'_0)^2-(q'_1)^2-(q'_2)^2-(q'_3)^2$ | $(1,3)$ | indefinite (Lorentzian) | $(q'_0)^2=\sum_k(q'_k)^2$ | $O(1,3)$ |
The pattern is the mirror image of the quaternion subspace: the bilinear topology is negative definite and the Hermitian one positive definite, differing by a sign, while the Krein topology is Lorentzian. It is the Krein form, and only it, that gives the subspace a null cone.
Summary
On the anti-quaternion subspace the bilinear form restricts to $-\sum_\mu(q'_\mu)^2$ of signature $(0,4)$, negative definite; the Hermitian form to $\sum_\mu(q'_\mu)^2$ of signature $(4,0)$, positive definite, the two differing by a sign; and the Krein form to $(q'_0)^2-\sum_k(q'_k)^2$ of signature $(1,3)$, Lorentzian, with a three-dimensional light cone. The isometry groups are $O(4)$, $O(4)$ and $O(1,3)$.
Summary of Notation
| Symbol | Meaning |
|---|---|
| $i\mathbb{H}_{\mathbb{B}}$ | the anti-quaternion subspace, of real dimension $4$ |
| $B$, $\langle\cdot,\cdot\rangle$, $[\cdot,\cdot]$ | the bilinear, Hermitian and Krein forms of The Three Pairings of the Biquaternion Algebra |
| $(0,4)$ | the signature of the bilinear form on $i\mathbb{H}_{\mathbb{B}}$ |
| $(4,0)$ | the signature of the Hermitian form on $i\mathbb{H}_{\mathbb{B}}$, positive definite |
| $(1,3)$ | the signature of the Krein form on $i\mathbb{H}_{\mathbb{B}}$ |
| $O(0,4)$, $O(4)$, $O(1,3)$ | the isometry groups of the three restrictions |
Further Reading
- Introduction to the Six Subspaces (
articles_maths/introduction-to-the-six-subspaces.md), for the subspace itself in the Algebra group - The Three Pairings of the Biquaternion Algebra (
articles_maths/the-three-pairings-of-the-biquaternion-algebra.md), for the three forms and the three Gram matrices - The Bilinear Form on the Biquaternion Algebra (
articles_maths/the-bilinear-form-on-the-biquaternion-algebra.md), for the first pairing and its restrictions - The Hermitian Form on the Biquaternion Algebra (
articles_maths/the-hermitian-form-on-the-biquaternion-algebra.md), for the second pairing and the Euclidean norm it defines - The Krein Gram Matrix and the Restrictions of the Form (
articles_maths/the-krein-gram-matrix-and-the-restrictions-of-the-form.md), for the third pairing and the same six restrictions - Biquaternion Relations Between Subspaces (
articles_maths/biquaternion-relations-between-subspaces.md), for the six subspaces together and their intersections - Biquaternion Square Roots of Minus One, Zero and Plus One (
articles_maths/biquaternion-square-roots-of-minus-one-zero-and-plus-one.md), for the root sets of the subspace