Paravectors

The corresponding paravector basis that combines a real scalar and vectors is

${\displaystyle \{1,\mathbf {e} _{1},\mathbf {e} _{2},\mathbf {e} _{3}\}}$,

which forms a four-dimensional linear space. The paravector space in the three-dimensional Euclidean space ${\displaystyle C\ell _{3}}$ can be used to represent the space-time of special relativity as expressed in the algebra of physical space (APS).

It is convenient to write the unit scalar as ${\displaystyle 1=\mathbf {e} _{0}}$, so that the complete basis can be written in a compact form as

${\displaystyle \{\mathbf {e} _{\mu }\},}$

where the Greek indices such as ${\displaystyle \mu }$ run from ${\displaystyle 0}$ to ${\displaystyle 3}$.

Antiautomorphism

Reversion conjugation

The Reversion antiautomorphism is denoted by ${\displaystyle \dagger }$. The action of this conjugation is to reverse the order of the geometric product (product between Clifford numbers in general).

${\displaystyle (AB)^{\dagger }=B^{\dagger }A^{\dagger }}$,

where vectors and real scalar numbers are invariant under reversion conjugation and are said to be real, for example:

${\displaystyle \mathbf {a} ^{\dagger }=\mathbf {a} }$

${\displaystyle 1^{\dagger }=1}$

On the other hand, the trivector and bivectors change sign under reversion conjugation and are said to be purely imaginary. The reversion conjugation applied to each basis element is given below

Element	Reversion conjugation
${\displaystyle 1}$	${\displaystyle 1}$
${\displaystyle \mathbf {e} _{1}}$	${\displaystyle \mathbf {e} _{1}}$
${\displaystyle \mathbf {e} _{2}}$	${\displaystyle \mathbf {e} _{2}}$
${\displaystyle \mathbf {e} _{3}}$	${\displaystyle \mathbf {e} _{3}}$
${\displaystyle \mathbf {e} _{12}}$	${\displaystyle -\mathbf {e} _{12}}$
${\displaystyle \mathbf {e} _{23}}$	${\displaystyle -\mathbf {e} _{23}}$
${\displaystyle \mathbf {e} _{31}}$	${\displaystyle -\mathbf {e} _{31}}$
${\displaystyle \mathbf {e} _{123}}$	${\displaystyle -\mathbf {e} _{123}}$

Clifford conjugation

The Clifford Conjugation is denoted by a bar over the object ${\displaystyle {\bar {}}}$. This conjugation is also called bar conjugation.

Clifford conjugation is the combined action of grade involution and reversion.

The action of the Clifford conjugation on a paravector is to reverse the sign of the vectors, maintaining the sign of the real scalar numbers, for example

${\displaystyle {\bar {\mathbf {a} }}=-\mathbf {a} }$

${\displaystyle {\bar {1}}=1}$

This is due to both scalars and vectors being invariant to reversion ( it is impossible to reverse the order of one or no things ) and scalars are of zero order and so are of even grade whilst vectors are of odd grade and so undergo a sign change under grade involution.

As antiautomorphism, the Clifford conjugation is distributed as

${\displaystyle {\overline {AB}}={\overline {B}}\,\,{\overline {A}}}$

The bar conjugation applied to each basis element is given below

Element	Bar conjugation
${\displaystyle 1}$	${\displaystyle 1}$
${\displaystyle \mathbf {e} _{1}}$	${\displaystyle -\mathbf {e} _{1}}$
${\displaystyle \mathbf {e} _{2}}$	${\displaystyle -\mathbf {e} _{2}}$
${\displaystyle \mathbf {e} _{3}}$	${\displaystyle -\mathbf {e} _{3}}$
${\displaystyle \mathbf {e} _{12}}$	${\displaystyle -\mathbf {e} _{12}}$
${\displaystyle \mathbf {e} _{23}}$	${\displaystyle -\mathbf {e} _{23}}$
${\displaystyle \mathbf {e} _{31}}$	${\displaystyle -\mathbf {e} _{31}}$
${\displaystyle \mathbf {e} _{123}}$	${\displaystyle \mathbf {e} _{123}}$

• Note.- The volume element is invariant under the bar conjugation.

Grade automorphism

The grade automorphism

${\displaystyle {\overline {AB}}^{\dagger }={\overline {A}}^{\dagger }{\overline {B}}^{\dagger }}$

is defined as the composite action of both the reversion conjugation and Clifford conjugation and has the effect to invert the sign of odd-grade multivectors, while maintaining the even-grade multivectors invariant:

Element	Grade involution
${\displaystyle 1}$	${\displaystyle 1}$
${\displaystyle \mathbf {e} _{1}}$	${\displaystyle -\mathbf {e} _{1}}$
${\displaystyle \mathbf {e} _{2}}$	${\displaystyle -\mathbf {e} _{2}}$
${\displaystyle \mathbf {e} _{3}}$	${\displaystyle -\mathbf {e} _{3}}$
${\displaystyle \mathbf {e} _{12}}$	${\displaystyle \mathbf {e} _{12}}$
${\displaystyle \mathbf {e} _{23}}$	${\displaystyle \mathbf {e} _{23}}$
${\displaystyle \mathbf {e} _{31}}$	${\displaystyle \mathbf {e} _{31}}$
${\displaystyle \mathbf {e} _{123}}$	${\displaystyle -\mathbf {e} _{123}}$

Invariant subspaces according to the conjugations

Four special subspaces can be defined in the ${\displaystyle C\ell _{3}}$ space based on their symmetries under the reversion and Clifford conjugation

• Scalar subspace: Invariant under Clifford conjugation.
• Vector subspace: Reverses sign under Clifford conjugation.
• Real subspace: Invariant under reversion conjugation.
• Imaginary subspace: Reverses sign under reversion conjugation.

Given ${\displaystyle p}$ as a general Clifford number, the complementary scalar and vector parts of ${\displaystyle p}$ are given by symmetric and antisymmetric combinations with the Clifford conjugation

${\displaystyle \langle p\rangle _{S}={\frac {1}{2}}(p+{\overline {p}}),}$

${\displaystyle \langle p\rangle _{V}={\frac {1}{2}}(p-{\overline {p}})}$.

In similar way, the complementary Real and Imaginary parts of ${\displaystyle p}$ are given by symmetric and antisymmetric combinations with the Reversion conjugation

${\displaystyle \langle p\rangle _{R}={\frac {1}{2}}(p+p^{\dagger }),}$

${\displaystyle \langle p\rangle _{I}={\frac {1}{2}}(p-p^{\dagger })}$.

It is possible to define four intersections, listed below

${\displaystyle \langle p\rangle _{RS}=\langle p\rangle _{SR}\equiv \langle \langle p\rangle _{R}\rangle _{S}}$

${\displaystyle \langle p\rangle _{RV}=\langle p\rangle _{VR}\equiv \langle \langle p\rangle _{R}\rangle _{V}}$

${\displaystyle \langle p\rangle _{IV}=\langle p\rangle _{VI}\equiv \langle \langle p\rangle _{I}\rangle _{V}}$

${\displaystyle \langle p\rangle _{IS}=\langle p\rangle _{SI}\equiv \langle \langle p\rangle _{I}\rangle _{S}}$

The following table summarizes the grades of the respective subspaces, where for example, the grade 0 can be seen as the intersection of the Real and Scalar subspaces

• Remark: The term "Imaginary" is used in the context of the ${\displaystyle C\ell _{3}}$ algebra and does not imply the introduction of the standard complex numbers in any form.

Closed subspaces with respect to the product

There are two subspaces that are closed with respect to the product. They are the scalar space and the even space that are isomorphic with the well known algebras of complex numbers and quaternions.

• The scalar space made of grades 0 and 3 is isomorphic with the standard algebra of complex numbers with the identification of

  ${\displaystyle \mathbf {e} _{123}=i.}$

• The even space, made of elements of grades 0 and 2, is isomorphic with the algebra of quaternions with the identification of

  ${\displaystyle -\mathbf {e} _{23}=i}$

  ${\displaystyle -\mathbf {e} _{31}=j}$

  ${\displaystyle -\mathbf {e} _{12}=k.}$

Scalar product

Given two paravectors ${\displaystyle u}$ and ${\displaystyle v}$, the generalization of the scalar product is

${\displaystyle \langle u{\bar {v}}\rangle _{S}.}$

The magnitude square of a paravector ${\displaystyle u}$ is

${\displaystyle \langle u{\bar {u}}\rangle _{S},}$

which is not a definite bilinear form and can be equal to zero even if the paravector is not equal to zero.

It is very suggestive that the paravector space automatically obeys the metric of the Minkowski space because

${\displaystyle \eta _{\mu \nu }=\langle \mathbf {e} _{\mu }{\bar {\mathbf {e} }}_{\nu }\rangle _{S}}$

and in particular:

${\displaystyle \eta _{00}=\langle \mathbf {e} _{0}{\bar {\mathbf {e} }}_{0}\rangle =\langle 1(1)\rangle _{S}=1,}$

${\displaystyle \eta _{11}=\langle \mathbf {e} _{1}{\bar {\mathbf {e} }}_{1}\rangle =\langle \mathbf {e} _{1}(-\mathbf {e} _{1})\rangle _{S}=-1,}$

${\displaystyle \eta _{01}=\langle \mathbf {e} _{0}{\bar {\mathbf {e} }}_{1}\rangle =\langle 1(-\mathbf {e} _{1})\rangle _{S}=0.}$

Biparavectors

Given two paravectors ${\displaystyle u}$ and ${\displaystyle v}$, the biparavector B is defined as:

${\displaystyle B=\langle u{\bar {v}}\rangle _{V}}$.

The biparavector basis can be written as

${\displaystyle \{\langle \mathbf {e} _{\mu }{\bar {\mathbf {e} }}_{\nu }\rangle _{V}\},}$

which contains six independent elements, including real and imaginary terms. Three real elements (vectors) as

${\displaystyle \langle \mathbf {e} _{0}{\bar {\mathbf {e} }}_{k}\rangle _{V}=-\mathbf {e} _{k},}$

and three imaginary elements (bivectors) as

${\displaystyle \langle \mathbf {e} _{j}{\bar {\mathbf {e} }}_{k}\rangle _{V}=-\mathbf {e} _{jk}}$

where ${\displaystyle j,k}$ run from 1 to 3.

In the Algebra of physical space, the electromagnetic field is expressed as a biparavector as

${\displaystyle F=\mathbf {E} +i\mathbf {B} ^{\,},}$

where both the electric and magnetic fields are real vectors

${\displaystyle \mathbf {E} ^{\dagger }=\mathbf {E} }$

${\displaystyle \mathbf {B} ^{\dagger }=\mathbf {B} }$

and ${\displaystyle i}$ represents the pseudoscalar volume element.

Another example of biparavector is the representation of the space-time rotation rate that can be expressed as

${\displaystyle W=i\theta ^{j}\mathbf {e} _{j}+\eta ^{j}\mathbf {e} _{j},}$

with three ordinary rotation angle variables ${\displaystyle \theta ^{j}}$ and three rapidities ${\displaystyle \eta ^{j}}$.

Triparavectors

Given three paravectors ${\displaystyle u}$, ${\displaystyle v}$ and ${\displaystyle w}$, the triparavector T is defined as:

${\displaystyle T=\langle u{\bar {v}}w\rangle _{I}}$.

The triparavector basis can be written as

${\displaystyle \{\langle \mathbf {e} _{\mu }{\bar {\mathbf {e} }}_{\nu }\mathbf {e} _{\lambda }\rangle _{I}\},}$

but there are only four independent triparavectors, so it can be reduced to

${\displaystyle \{i\mathbf {e} _{\rho }\}}$.

Pseudoscalar

The pseudoscalar basis is

${\displaystyle \{\langle \mathbf {e} _{\mu }{\bar {\mathbf {e} }}_{\nu }\mathbf {e} _{\lambda }{\bar {\mathbf {e} }}_{\rho }\rangle _{IS}\},}$

but a calculation reveals that it contains only a single term. This term is the volume element ${\displaystyle i=\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}}$.

The four grades, taken in combination of pairs generate the paravector, biparavector and triparavector spaces as shown in the next table, where for example, we see that the paravector is made of grades 0 and 1

Paragradient

The paragradient operator is the generalization of the gradient operator in the paravector space. The paragradient in the standard paravector basis is

${\displaystyle \partial =\mathbf {e} _{0}\partial _{0}-\mathbf {e} _{1}\partial _{1}-\mathbf {e} _{2}\partial _{2}-\mathbf {e} _{3}\partial _{3},}$

which allows one to write the d'Alembert operator as

${\displaystyle \square =\langle {\bar {\partial }}\partial \rangle _{S}=\langle \partial {\bar {\partial }}\rangle _{S}}$

The standard gradient operator can be defined naturally as

${\displaystyle \nabla =\mathbf {e} _{1}\partial _{1}+\mathbf {e} _{2}\partial _{2}+\mathbf {e} _{3}\partial _{3},}$

so that the paragradient can be written as

${\displaystyle \partial =\partial _{0}-\nabla ,}$

where ${\displaystyle \mathbf {e} _{0}=1}$.

The application of the paragradient operator must be done carefully, always respecting its non-commutative nature. For example, a widely used derivative is

${\displaystyle \partial e^{f(x)\mathbf {e} _{3}}=(\partial f(x))e^{f(x)\mathbf {e} _{3}}\mathbf {e} _{3},}$

where ${\displaystyle f(x)}$ is a scalar function of the coordinates.

The paragradient is an operator that always acts from the left if the function is a scalar function. However, if the function is not scalar, the paragradient can act from the right as well. For example, the following expression is expanded as

${\displaystyle (L\partial )=\mathbf {e} _{0}\partial _{0}L+(\partial _{1}L)\mathbf {e} _{1}+(\partial _{2}L)\mathbf {e} _{2}+(\partial _{3}L)\mathbf {e} _{3}}$

Null paravectors as projectors

Null paravectors are elements that are not necessarily zero but have magnitude identical to zero. For a null paravector ${\displaystyle p}$, this property necessarily implies the following identity

${\displaystyle p{\bar {p}}=0.}$

In the context of Special Relativity they are also called lightlike paravectors.

Projectors are null paravectors of the form

${\displaystyle P_{\mathbf {k} }={\frac {1}{2}}(1+{\hat {\mathbf {k} }}),}$

where ${\displaystyle {\hat {\mathbf {k} }}}$ is a unit vector.

A projector ${\displaystyle P_{\mathbf {k} }}$ of this form has a complementary projector ${\displaystyle {\bar {P}}_{\mathbf {k} }}$

${\displaystyle {\bar {P}}_{\mathbf {k} }={\frac {1}{2}}(1-{\hat {\mathbf {k} }}),}$

such that

${\displaystyle P_{\mathbf {k} }+{\bar {P}}_{\mathbf {k} }=1}$

As projectors, they are idempotent

${\displaystyle P_{\mathbf {k} }=P_{\mathbf {k} }P_{\mathbf {k} }=P_{\mathbf {k} }P_{\mathbf {k} }P_{\mathbf {k} }=...}$

and the projection of one on the other is zero because they are null paravectors

${\displaystyle P_{\mathbf {k} }{\bar {P}}_{\mathbf {k} }=0.}$

The associated unit vector of the projector can be extracted as

${\displaystyle {\hat {\mathbf {k} }}=P_{\mathbf {\mathbf {k} } }-{\bar {P}}_{\mathbf {k} },}$

this means that ${\displaystyle {\hat {\mathbf {k} }}}$ is an operator with eigenfunctions ${\displaystyle P_{\mathbf {\mathbf {k} } }}$ and ${\displaystyle {\bar {P}}_{\mathbf {\mathbf {k} } }}$, with respective eigenvalues ${\displaystyle 1}$ and ${\displaystyle -1}$.

From the previous result, the following identity is valid assuming that ${\displaystyle f({\hat {\mathbf {k} }})}$ is analytic around zero

${\displaystyle f({\hat {\mathbf {k} }})=f(1)P_{\mathbf {k} }+f(-1){\bar {P}}_{\mathbf {k} }.}$

This gives origin to the pacwoman property, such that the following identities are satisfied

${\displaystyle f({\hat {\mathbf {k} }})P_{\mathbf {k} }=f(1)P_{\mathbf {k} },}$

${\displaystyle f({\hat {\mathbf {k} }}){\bar {P}}_{\mathbf {k} }=f(-1){\bar {P}}_{\mathbf {k} }.}$

Null basis for the paravector space

A basis of elements, each one of them null, can be constructed for the complete ${\displaystyle C\ell _{3}}$ space. The basis of interest is the following

${\displaystyle \{{\bar {P}}_{3},P_{3}\mathbf {e} _{1},P_{3},\mathbf {e} _{1}P_{3}\}}$

so that an arbitrary paravector

${\displaystyle p=p^{0}\mathbf {e} _{0}+p^{1}\mathbf {e} _{1}+p^{2}\mathbf {e} _{2}+p^{3}\mathbf {e} _{3}}$

can be written as

${\displaystyle p=(p^{0}+p^{3})P_{3}+(p^{0}-p^{3}){\bar {P}}_{3}+(p^{1}+ip^{2})\mathbf {e} _{1}P_{3}+(p^{1}-ip^{2})P_{3}\mathbf {e} _{1}}$

This representation is useful for some systems that are naturally expressed in terms of the light cone variables that are the coefficients of ${\displaystyle P_{3}}$ and ${\displaystyle {\bar {P}}_{3}}$ respectively.

Every expression in the paravector space can be written in terms of the null basis. A paravector ${\displaystyle p}$ is in general parametrized by two real scalars numbers ${\displaystyle \{u,v\}}$ and a general scalar number ${\displaystyle w}$ (including scalar and pseudoscalar numbers)

${\displaystyle p=u{\bar {P}}_{3}+vP_{3}+w\mathbf {e} _{1}P_{3}+w^{\dagger }P_{3}\mathbf {e} _{1}}$

the paragradient in the null basis is

${\displaystyle \partial =2P_{3}\partial _{u}+2{\bar {P}}_{3}\partial _{v}-2\mathbf {e} _{1}P_{3}\partial _{w^{\dagger }}-2P_{3}\mathbf {e} _{1}\partial _{w}}$

Conjugations

The reversion conjugation is translated into the Hermitian conjugation and the bar conjugation is translated into the following matrix:

${\displaystyle {\bar {\Psi }}\rightarrow {\begin{pmatrix}\psi _{22}&-\psi _{12}\\-\psi _{21}&\psi _{11}\end{pmatrix}},}$

such that the scalar part is translated as

${\displaystyle \langle \Psi \rangle _{S}\rightarrow {\frac {\psi _{11}+\psi _{22}}{2}}{\begin{pmatrix}1&0\\0&1\end{pmatrix}}={\frac {Tr[\psi ]}{2}}\mathbf {1} _{2\times 2}}$

The rest of the subspaces are translated as

${\displaystyle \langle \Psi \rangle _{V}\rightarrow {\begin{pmatrix}0&\psi _{12}\\\psi _{21}&0\end{pmatrix}}}$

${\displaystyle \langle \Psi \rangle _{R}\rightarrow {\frac {1}{2}}{\begin{pmatrix}\psi _{11}+\psi _{11}^{*}&\psi _{12}+\psi _{21}^{*}\\\psi _{21}+\psi _{12}^{*}&\psi _{22}+\psi _{22}^{*}\end{pmatrix}}}$

${\displaystyle \langle \Psi \rangle _{I}\rightarrow {\frac {1}{2}}{\begin{pmatrix}\psi _{11}-\psi _{11}^{*}&\psi _{12}-\psi _{21}^{*}\\\psi _{21}-\psi _{12}^{*}&\psi _{22}-\psi _{22}^{*}\end{pmatrix}}}$

Higher dimensions

The matrix representation of a Euclidean space in higher dimensions can be constructed in terms of the Kronecker product of the Pauli matrices, resulting in complex matrices of dimension ${\displaystyle 2^{n}}$. The 4D representation could be taken as

	Matrix representation 4D
${\displaystyle \mathbf {e} _{1}}$	${\displaystyle \sigma _{3}\otimes \sigma _{1}}$
${\displaystyle \mathbf {e} _{2}}$	${\displaystyle \sigma _{3}\otimes \sigma _{2}}$
${\displaystyle \mathbf {e} _{3}}$	${\displaystyle \sigma _{3}\otimes \sigma _{3}}$
${\displaystyle \mathbf {e} _{4}}$	${\displaystyle \sigma _{2}\otimes \sigma _{0}}$

The 7D representation could be taken as

	Matrix representation 7D
${\displaystyle \mathbf {e} _{1}}$	${\displaystyle \sigma _{0}\otimes \sigma _{3}\otimes \sigma _{1}}$
${\displaystyle \mathbf {e} _{2}}$	${\displaystyle \sigma _{0}\otimes \sigma _{3}\otimes \sigma _{2}}$
${\displaystyle \mathbf {e} _{3}}$	${\displaystyle \sigma _{0}\otimes \sigma _{3}\otimes \sigma _{3}}$
${\displaystyle \mathbf {e} _{4}}$	${\displaystyle \sigma _{0}\otimes \sigma _{2}\otimes \sigma _{0}}$
${\displaystyle \mathbf {e} _{5}}$	${\displaystyle \sigma _{3}\otimes \sigma _{1}\otimes \sigma _{0}}$
${\displaystyle \mathbf {e} _{6}}$	${\displaystyle \sigma _{1}\otimes \sigma _{1}\otimes \sigma _{0}}$
${\displaystyle \mathbf {e} _{7}}$	${\displaystyle \sigma _{2}\otimes \sigma _{1}\otimes \sigma _{0}}$

Textbooks

• Baylis, William (2002). Electrodynamics: A Modern Geometric Approach (2nd ed.). Birkhäuser. ISBN 0-8176-4025-8
• Baylis, William, Clifford (Geometric) Algebras With Applications in Physics, Mathematics, and Engineering, Birkhauser (1999)
• [H1999] David Hestenes: New Foundations for Classical Mechanics (Second Edition). ISBN 0-7923-5514-8, Kluwer Academic Publishers (1999)
• Chris Doran and Antony Lasenby, Geometric Algebra for Physicists, Cambridge, 2003

Articles

• Baylis, W E (2004-11-01). "Relativity in introductory physics". Canadian Journal of Physics. Canadian Science Publishing. 82 (11): 853–873. arXiv:physics/0406158. Bibcode:2004CaJPh..82..853B. doi:10.1139/p04-058. ISSN 0008-4204. S2CID 35027499.
• Doran, C.; Hestenes, D.; Sommen, F.; Van Acker, N. (1993). "Lie groups as spin groups". Journal of Mathematical Physics. AIP Publishing. 34 (8): 3642–3669. Bibcode:1993JMP....34.3642D. doi:10.1063/1.530050. ISSN 0022-2488.
• Cabrera, R.; Rangan, C.; Baylis, W. E. (2007-09-04). "Sufficient condition for the coherent control of n-qubit systems". Physical Review A. American Physical Society (APS). 76 (3): 033401. arXiv:quant-ph/0703220. Bibcode:2007PhRvA..76c3401C. doi:10.1103/physreva.76.033401. ISSN 1050-2947. S2CID 45060566.
• Vaz, Jayme; Mann, Stephen (2018). "Paravectors and the Geometry of 3D Euclidean Space". Advances in Applied Clifford Algebras. Springer Science and Business Media LLC. 28 (5): 99. arXiv:1810.09389. doi:10.1007/s00006-018-0916-1. ISSN 0188-7009. S2CID 253600966.