Multivector
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Multivector

In multilinear algebra, a multivector, sometimes called Clifford number,[1] is an element of the exterior algebra ?(V) of a vector space V. This algebra is graded, associative and alternating, and consists of linear combinations of simple k-vectors[2] (also known as decomposable k-vectors[3] or k-blades) of the form

${\displaystyle v_{1}\wedge \cdots \wedge v_{k},}$

where ${\displaystyle v_{1},\ldots ,v_{k}}$ are in V.

A k-vector is such a linear combination that is homogeneous of degree k (all terms are k-blades for the same k). Depending on the authors, a "multivector" may be either a k-vector or any element of the exterior algebra (any linear combination of k-blades with potentially differing values of k).[4]

In differential geometry, a k-vector is a k-vector in the exterior algebra of the tangent vector space; that is, it is an antisymmetric tensor obtained by taking linear combinations of the wedge product of k tangent vectors, for some integer k >= 0. A k-form is a k-vector in the exterior algebra of the dual of the tangent space, which is also the dual of the exterior algebra of the tangent space.

For k = 0, 1, 2 and 3, k-vectors are often called respectively scalars, vectors, bivectors and trivectors; they are respectively dual to 0-forms, 1-forms, 2-forms and 3-forms.[5][6]

## Wedge product

The wedge product operation used to construct multivectors is linear, associative and alternating, which reflect the properties of the determinant. This means for vectors u, v and w in a vector space V and for scalars ?, ?, the wedge product has the properties,

• Linear: ${\displaystyle \mathbf {u} \wedge (\alpha \mathbf {v} +\beta \mathbf {w} )=\alpha \mathbf {u} \wedge \mathbf {v} +\beta \mathbf {u} \wedge \mathbf {w} ;}$
• Associative: ${\displaystyle (\mathbf {u} \wedge \mathbf {v} )\wedge \mathbf {w} =\mathbf {u} \wedge (\mathbf {v} \wedge \mathbf {w} )=\mathbf {u} \wedge \mathbf {v} \wedge \mathbf {w} ;}$
• Alternating: ${\displaystyle \mathbf {u} \wedge \mathbf {v} =-\mathbf {v} \wedge \mathbf {u} ,\quad \mathbf {u} \wedge \mathbf {u} =0.}$

The product of p vectors is called a grade p multivector, or a p-vector. The maximum grade of a multivector is the dimension of the vector space V.

The linearity of the wedge product allows a multivector to be defined as the linear combination of basis multivectors. There are (n
p
) basis p-vectors in an n-dimensional vector space.[2]

## Area and volume

The p-vector obtained from the wedge product of p separate vectors in an n-dimensional space has components that define the projected -volumes of the p-parallelotope spanned by the vectors. The square root of the sum of the squares of these components defines the volume of the p-parallelotope.[2][7]

The following examples show that a bivector in two dimensions measures the area of a parallelogram, and the magnitude of a bivector in three dimensions also measures the area of a parallelogram. Similarly, a three-vector in three dimensions measures the volume of a parallelepiped.

It is easy to check that the magnitude of a three-vector in four dimensions measures the volume of the parallelepiped spanned by these vectors.

### Multivectors in R2

Properties of multivectors can be seen by considering the two dimensional vector space . Let the basis vectors be e1 and e2, so u and v are given by

${\displaystyle \mathbf {u} =u_{1}\mathbf {e} _{1}+u_{2}\mathbf {e} _{2},\quad \mathbf {v} =v_{1}\mathbf {e} _{1}+v_{2}\mathbf {e} _{2},}$

and the multivector , also called a bivector, is computed to be

${\displaystyle \mathbf {u} \wedge \mathbf {v} \ =\ {\begin{vmatrix}u_{1}&v_{1}\\u_{2}&v_{2}\end{vmatrix}}\ (\mathbf {e} _{1}\wedge \mathbf {e} _{2}).}$

The vertical bars denote the determinant of the matrix, which is the area of the parallelogram spanned by the vectors u and v. The magnitude of is the area of this parallelogram. Notice that because V has dimension two the basis bivector is the only multivector in ?V.

The relationship between the magnitude of a multivector and the area or volume spanned by the vectors is an important feature in all dimensions. Furthermore, the linear functional version of a multivector that computes this volume is known as a differential form.

### Multivectors in R3

More features of multivectors can be seen by considering the three dimensional vector space . In this case, let the basis vectors be e1, e2, and e3, so u, v and w are given by

${\displaystyle \mathbf {u} =u_{1}\mathbf {e} _{1}+u_{2}\mathbf {e} _{2}+u_{3}\mathbf {e} _{3},\quad \mathbf {v} =v_{1}\mathbf {e} _{1}+v_{2}\mathbf {e} _{2}+v_{3}\mathbf {e} _{3},\quad \mathbf {w} =w_{1}\mathbf {e} _{1}+w_{2}\mathbf {e} _{2}+w_{3}\mathbf {e} _{3},}$

and the bivector is computed to be

${\displaystyle \mathbf {u} \wedge \mathbf {v} \ =\ {\begin{vmatrix}u_{2}&v_{2}\\u_{3}&v_{3}\end{vmatrix}}\ (\mathbf {e} _{2}\wedge \mathbf {e} _{3})+{\begin{vmatrix}u_{1}&v_{1}\\u_{3}&v_{3}\end{vmatrix}}\ (\mathbf {e} _{1}\wedge \mathbf {e} _{3})+{\begin{vmatrix}u_{1}&v_{1}\\u_{2}&v_{2}\end{vmatrix}}\ (\mathbf {e} _{1}\wedge \mathbf {e} _{2}).}$

The components of this bivector are the same as the components of the cross product. The magnitude of this bivector is the square root of the sum of the squares of its components.

This shows that the magnitude of the bivector is the area of the parallelogram spanned by the vectors u and v as it lies in the three-dimensional space V. The components of the bivector are the projected areas of the parallelogram on each of the three coordinate planes.

Notice that because V has dimension three, there is one basis three-vector in ?V. Compute the three-vector

${\displaystyle \mathbf {u} \wedge \mathbf {v} \wedge \mathbf {w} \ =\ {\begin{vmatrix}u_{1}&v_{1}&w_{1}\\u_{2}&v_{2}&w_{2}\\u_{3}&v_{3}&w_{3}\end{vmatrix}}\ (\mathbf {e} _{1}\wedge \mathbf {e} _{2}\wedge \mathbf {e} _{3}).}$

This shows that the magnitude of the three-vector is the volume of the parallelepiped spanned by the three vectors u, v and w.

In higher-dimensional spaces, the component three-vectors are projections of the volume of a parallelepiped onto the coordinate three-spaces, and the magnitude of the three-vector is the volume of the parallelepiped as it sits in the higher-dimensional space.

## Grassmann coordinates

In this section, we consider multivectors on a projective space Pn, which provide a convenient set of coordinates for lines, planes and hyperplanes that have properties similar to the homogeneous coordinates of points, called Grassmann coordinates.[8]

Points in a real projective space Pn are defined to be lines through the origin of the vector space Rn+1. For example, the projective plane P2 is the set of lines through the origin of R3. Thus, multivectors defined on Rn+1 can be viewed as multivectors on Pn.

A convenient way to view a multivector on Pn is to examine it in an affine component of Pn, which is the intersection of the lines through the origin of Rn+1 with a selected hyperplane, such as . Lines through the origin of R3 intersect the plane to define an affine version of the projective plane that only lacks the points for which , called the points at infinity.

### Multivectors on P2

Points in the affine component of the projective plane have coordinates . A linear combination of two points and defines a plane in R3 that intersects E in the line joining p and q. The multivector defines a parallelogram in R3 given by

${\displaystyle \mathbf {p} \wedge \mathbf {q} \ =\ (p_{2}-q_{2})(\mathbf {e} _{2}\wedge \mathbf {e} _{3})+(p_{1}-q_{1})(\mathbf {e} _{1}\wedge \mathbf {e} _{3})+(p_{1}q_{2}-q_{1}p_{2})(\mathbf {e} _{1}\wedge \mathbf {e} _{2}).}$

Notice that substitution of for p multiplies this multivector by a constant. Therefore, the components of are homogeneous coordinates for the plane through the origin of R3.

The set of points on the line through p and q is the intersection of the plane defined by with the plane . These points satisfy , that is,

${\displaystyle \mathbf {x} \wedge \mathbf {p} \wedge \mathbf {q} \ =\ (x\mathbf {e} _{1}+y\mathbf {e} _{2}+\mathbf {e} _{3})\wedge {\big (}(p_{2}-q_{2})(\mathbf {e} _{2}\wedge \mathbf {e} _{3})+(p_{1}-q_{1})(\mathbf {e} _{1}\wedge \mathbf {e} _{3})+(p_{1}q_{2}-q_{1}p_{2})(\mathbf {e} _{1}\wedge \mathbf {e} _{2}){\big )}=0,}$

which simplifies to the equation of a line

${\displaystyle \lambda :x(p_{2}-q_{2})+y(p_{1}-q_{1})+(p_{1}q_{2}-q_{1}p_{2})=0.}$

This equation is satisfied by points for real values of ? and ?.

The three components of that define the line ? are called the Grassmann coordinates of the line. Because three homogeneous coordinates define both a point and a line, the geometry of points is said to be dual to the geometry of lines in the projective plane. This is called the principle of duality.

### Multivectors on P3

Three dimensional projective space, P3 consists of all lines through the origin of R4. Let the three dimensional hyperplane, , be the affine component of projective space defined by the points . The multivector defines a parallelepiped in R4 given by

${\displaystyle \mathbf {p} \wedge \mathbf {q} \wedge \mathbf {r} ={\begin{vmatrix}p_{2}&q_{2}&r_{2}\\p_{3}&q_{3}&r_{3}\\1&1&1\end{vmatrix}}\mathbf {e} _{2}\wedge \mathbf {e} _{3}\wedge \mathbf {e} _{4}+{\begin{vmatrix}p_{1}&q_{1}&r_{1}\\p_{3}&q_{3}&r_{3}\\1&1&1\end{vmatrix}}\mathbf {e} _{1}\wedge \mathbf {e} _{3}\wedge \mathbf {e} _{4}+{\begin{vmatrix}p_{1}&q_{1}&r_{1}\\p_{2}&q_{2}&r_{2}\\1&1&1\end{vmatrix}}\mathbf {e} _{1}\wedge \mathbf {e} _{2}\wedge \mathbf {e} _{4}+{\begin{vmatrix}p_{1}&q_{1}&r_{1}\\p_{2}&q_{2}&r_{2}\\p_{3}&q_{3}&r_{3}\end{vmatrix}}\mathbf {e} _{1}\wedge \mathbf {e} _{2}\wedge \mathbf {e} _{3}.}$

Notice that substitution of for p multiplies this multivector by a constant. Therefore, the components of are homogeneous coordinates for the 3-space through the origin of R4.

A plane in the affine component is the set of points in the intersection of H with the 3-space defined by . These points satisfy , that is,

${\displaystyle \mathbf {x} \wedge \mathbf {p} \wedge \mathbf {q} \wedge \mathbf {r} =(x\mathbf {e} _{1}+y\mathbf {e} _{2}+z\mathbf {e} _{3}+\mathbf {e} _{4})\wedge \mathbf {p} \wedge \mathbf {q} \wedge \mathbf {r} =0,}$

which simplifies to the equation of a plane

${\displaystyle \lambda :x{\begin{vmatrix}p_{2}&q_{2}&r_{2}\\p_{3}&q_{3}&r_{3}\\1&1&1\end{vmatrix}}+y{\begin{vmatrix}p_{1}&q_{1}&r_{1}\\p_{3}&q_{3}&r_{3}\\1&1&1\end{vmatrix}}+z{\begin{vmatrix}p_{1}&q_{1}&r_{1}\\p_{2}&q_{2}&r_{2}\\1&1&1\end{vmatrix}}+{\begin{vmatrix}p_{1}&q_{1}&r_{1}\\p_{2}&q_{2}&r_{2}\\p_{3}&q_{3}&r_{3}\end{vmatrix}}=0.}$

This equation is satisfied by points for real values of ?, ? and ?.

The four components of that define the plane ? are called the Grassmann coordinates of the plane. Because four homogeneous coordinates define both a point and a plane in projective space, the geometry of points is dual to the geometry of planes.

A line as the join of two points: In projective space the line ? through two points p and q can be viewed as the intersection of the affine space with the plane in R4. The multivector provides homogeneous coordinates for the line

${\displaystyle \lambda :\mathbf {p} \wedge \mathbf {q} =(p_{1}\mathbf {e} _{1}+p_{2}\mathbf {e} _{2}+p_{3}\mathbf {e} _{3}+\mathbf {e} _{4})\wedge (q_{1}\mathbf {e} _{1}+q_{2}\mathbf {e} _{2}+q_{3}\mathbf {e} _{3}+\mathbf {e} _{4}),}$
${\displaystyle \qquad ={\begin{vmatrix}p_{1}&q_{1}\\1&1\end{vmatrix}}\mathbf {e} _{1}\wedge \mathbf {e} _{4}+{\begin{vmatrix}p_{2}&q_{2}\\1&1\end{vmatrix}}\mathbf {e} _{2}\wedge \mathbf {e} _{4}+{\begin{vmatrix}p_{3}&q_{3}\\1&1\end{vmatrix}}\mathbf {e} _{3}\wedge \mathbf {e} _{4}+{\begin{vmatrix}p_{2}&q_{2}\\p_{3}&q_{3}\end{vmatrix}}\mathbf {e} _{2}\wedge \mathbf {e} _{3}+{\begin{vmatrix}p_{3}&q_{3}\\p_{1}&q_{1}\end{vmatrix}}\mathbf {e} _{3}\wedge \mathbf {e} _{1}+{\begin{vmatrix}p_{1}&q_{1}\\p_{2}&q_{2}\end{vmatrix}}\mathbf {e} _{1}\wedge \mathbf {e} _{2}.}$

These are known as the Plücker coordinates of the line, though they are also an example of Grassmann coordinates.

A line as the intersection of two planes: A line ? in projective space can also be defined as the set of points x that form the intersection of two planes ? and ? defined by grade three multivectors, so the points x are the solutions to the linear equations

${\displaystyle \mu :\mathbf {x} \wedge \pi =0,\mathbf {x} \wedge \rho =0.}$

In order to obtain the Plucker coordinates of the line ?, map the multivectors ? and ? to their dual point coordinates using the Hodge star operator,[2]

${\displaystyle \mathbf {e} _{1}={\star }(\mathbf {e} _{2}\wedge \mathbf {e} _{3}\wedge \mathbf {e} _{4}),-\mathbf {e} _{2}={\star }(\mathbf {e} _{1}\wedge \mathbf {e} _{3}\wedge \mathbf {e} _{4}),\mathbf {e} _{3}={\star }(\mathbf {e} _{1}\wedge \mathbf {e} _{2}\wedge \mathbf {e} _{4}),-\mathbf {e} _{4}={\star }(\mathbf {e} _{1}\wedge \mathbf {e} _{2}\wedge \mathbf {e} _{3}),}$

then

${\displaystyle {\star }\pi =\pi _{1}\mathbf {e} _{1}+\pi _{2}\mathbf {e} _{2}+\pi _{3}\mathbf {e} _{3}+\pi _{4}\mathbf {e} _{4},\quad {\star }\rho =\rho _{1}\mathbf {e} _{1}+\rho _{2}\mathbf {e} _{2}+\rho _{3}\mathbf {e} _{3}+\rho _{4}\mathbf {e} _{4}.}$

So, the Plücker coordinates of the line ? are given by

${\displaystyle \mu :({\star }\pi )\wedge ({\star }\rho )={\begin{vmatrix}\pi _{1}&\rho _{1}\\\pi _{4}&\rho _{4}\end{vmatrix}}\mathbf {e} _{1}\wedge \mathbf {e} _{4}+{\begin{vmatrix}\pi _{2}&\rho _{2}\\\pi _{4}&\rho _{4}\end{vmatrix}}\mathbf {e} _{2}\wedge \mathbf {e} _{4}+{\begin{vmatrix}\pi _{3}&\rho _{3}\\\pi _{4}&\rho _{4}\end{vmatrix}}\mathbf {e} _{3}\wedge \mathbf {e} _{4}+{\begin{vmatrix}\pi _{2}&\rho _{2}\\\pi _{3}&\rho _{3}\end{vmatrix}}\mathbf {e} _{2}\wedge \mathbf {e} _{3}+{\begin{vmatrix}\pi _{3}&\rho _{3}\\\pi _{1}&\rho _{1}\end{vmatrix}}\mathbf {e} _{3}\wedge \mathbf {e} _{1}+{\begin{vmatrix}\pi _{1}&\rho _{1}\\\pi _{2}&\rho _{2}\end{vmatrix}}\mathbf {e} _{1}\wedge \mathbf {e} _{2}.}$

Because the six homogeneous coordinates of a line can be obtained from the join of two points or the intersection of two planes, the line is said to be self dual in projective space.

## Clifford product

W. K. Clifford combined multivectors with the inner product defined on the vector space, in order to obtain a general construction for hypercomplex numbers that includes the usual complex numbers and Hamilton's quaternions.[9][10]

The Clifford product between two vectors u and v is linear and associative like the wedge product, and has the additional property that the multivector uv is coupled to the inner product by Clifford's relation,

${\displaystyle \mathbf {u} \mathbf {v} +\mathbf {v} \mathbf {u} =2\mathbf {u} \cdot \mathbf {v} .}$

Clifford's relation preserves the alternating property for the product of vectors that are perpendicular. This can be seen for the orthogonal unit vectors in Rn. Clifford's relation yields

${\displaystyle \mathbf {e} _{i}\mathbf {e} _{j}+\mathbf {e} _{j}\mathbf {e} _{i}=2\mathbf {e} _{i}\cdot \mathbf {e} _{j}=0,}$

therefore the basis vectors are alternating,

${\displaystyle \mathbf {e} _{i}\mathbf {e} _{j}=-\mathbf {e} _{j}\mathbf {e} _{i},\quad i\neq j=1,\ldots ,n.}$

In contrast to the wedge product, the Clifford product of a vector with itself is no longer zero. To see this compute the product,

${\displaystyle \mathbf {e} _{i}\mathbf {e} _{i}+\mathbf {e} _{i}\mathbf {e} _{i}=2\mathbf {e} _{i}\cdot \mathbf {e} _{i}=2,}$

which yields

${\displaystyle \mathbf {e} _{i}\mathbf {e} _{i}=1,\quad i=1,\ldots ,n.}$

The set of multivectors constructed using Clifford's product yields an associative algebra known as a Clifford algebra. Inner products with different properties can be used to construct different Clifford algebras.[11][12]

## Geometric algebra

The term k-blade was used in Clifford Algebra to Geometric Calculus (1984)[13]

Multivectors play a central role in the mathematical formulation of physics known as geometric algebra. According to David Hestenes,

[Non-scalar] k-vectors are sometimes called k-blades or, simply, blades to emphasize the fact that, in contrast to 0-vectors (scalars), they have "directional properties".[14]

In 2003 the term blade for a multivector was used by C. Doran and A. Lasenby.[15]

In geometric algebra, a multivector is defined to be the sum of different-grade k-blades, such as the summation of a scalar, a vector, and a 2-vector.[16] A sum of only k-grade components is called a k-vector,[17] or a homogeneous multivector.[18]

The highest grade element in a space is called a pseudoscalar.

If a given element is homogeneous of a grade k, then it is a k-vector, but not necessarily a k-blade. Such an element is a k-blade when it can be expressed as the wedge product of k vectors. A geometric algebra generated by a 4-dimensional Euclidean vector space illustrates the point with an example: The sum of any two blades with one taken from the XY-plane and the other taken from the ZW-plane will form a 2-vector that is not a 2-blade. In a geometric algebra generated by a Euclidean vector space of dimension 2 or 3, all sums of 2-blades may be written as a single 2-blade.

### Examples

Orientation defined by an ordered set of vectors.
Reversed orientation corresponds to negating the exterior product.
Geometric interpretation of grade n elements in a real exterior algebra for (signed point), 1 (directed line segment, or vector), 2 (oriented plane element), 3 (oriented volume). The exterior product of n vectors can be visualized as any n-dimensional shape (e.g. n-parallelotope, n-ellipsoid); with magnitude (hypervolume), and orientation defined by that on its -dimensional boundary and on which side the interior is.[19][20]

In the presence of a volume form (such as given an inner product and an orientation), pseudovectors and pseudoscalars can be identified with vectors and scalars, which is routine in vector calculus, but without a volume form this cannot be done without a choice.

In the algebra of physical space (the geometric algebra of Euclidean 3-space, used as a model of (3+1)-spacetime), a sum of a scalar and a vector is called a paravector, and represents a point in spacetime (the vector the space, the scalar the time).

### Bivectors

A bivector is an element of the antisymmetric tensor product of a tangent space with itself.

In geometric algebra, also, a bivector is a grade 2 element (a 2-vector) resulting from the wedge product of two vectors, and so it is geometrically an oriented area, in the same way a vector is an oriented line segment. If a and b are two vectors, the bivector has

• a norm which is its area, given by
${\displaystyle \left\|\mathbf {a} \wedge \mathbf {b} \right\|=\left\|\mathbf {a} \right\|\,\left\|\mathbf {b} \right\|\,\sin(\phi _{a,b})}$
• a direction: the plane where that area lies on, i.e., the plane determined by a and b, as long as they are linearly independent;
• an orientation (out of two), determined by the order in which the originating vectors are multiplied.

Bivectors are connected to pseudovectors, and are used to represent rotations in geometric algebra.

As bivectors are elements of a vector space ?2V (where V is a finite-dimensional vector space with ), it makes sense to define an inner product on this vector space as follows. First, write any element in terms of a basis as

${\displaystyle F=F^{ab}\mathbf {e} _{a}\wedge \mathbf {e} _{b}\quad (1\leq a

where the Einstein summation convention is being used.

Now define a map by insisting that

${\displaystyle G(F,H):=G_{abcd}F^{ab}H^{cd},}$

where ${\displaystyle G_{abcd}}$ are a set of numbers.

## Applications

Bivectors play many important roles in physics, for example, in the classification of electromagnetic fields.

## References

1. ^ John Snygg (2012), A New Approach to Differential Geometry Using Clifford's Geometric Algebra, Birkhäuser, p.5 §2.12
2. ^ a b c d Harley Flanders (1989)[1963] Differential Forms with Applications to the Physical Sciences, § 2.1 The Space of p-Vectors, pages 5-7, Dover Books
3. ^ Wendell Fleming (1977) [1965] Functions of Several Variables, section 7.5 Multivectors, page 295, ISBN 978-1-4684-9461-7
4. ^ Élie Cartan, The theory of spinors, p. 16, considers only homogeneous vectors, particularly simple ones, referring to them as "multivectors" (collectively) or p-vectors (specifically).
5. ^ William M Pezzaglia Jr. (1992). "Clifford algebra derivation of the characteristic hypersurfaces of Maxwell's equations". In Julian ?awrynowicz (ed.). Deformations of mathematical structures II. Springer. p. 131 ff. ISBN 0-7923-2576-1. Hence in 3D we associate the alternate terms of pseudovector for bivector, and pseudoscalar for the trivector
6. ^ Baylis (1994). Theoretical methods in the physical sciences: an introduction to problem solving using Maple V. Birkhäuser. p. 234, see footnote. ISBN 0-8176-3715-X.
7. ^ G. E. Shilov, Linear Algebra, (trans. R. A. Silverman), Dover Publications, 1977.
8. ^ W. V. D. Hodge and D. Pedoe, Methods of Algebraic Geometry, Vol. 1, Cambridge Univ. Press, 1947
9. ^ W. K. Clifford, "Preliminary sketch of bi-quaternions," Proc. London Math. Soc. Vol. 4 (1873) pp. 381-395
10. ^ W. K. Clifford, Mathematical Papers, (ed. R. Tucker), London: Macmillan, 1882.
11. ^ J. M. McCarthy, An Introduction to Theoretical Kinematics, pp. 62-5, MIT Press 1990.
12. ^ O. Bottema and B. Roth, Theoretical Kinematics, North Holland Publ. Co., 1979
13. ^ David Hestenes & Garret Sobczyk (1984) Clifford Algebra to Geometric Calculus, page 4, D. Reidel ISBN 90-277-1673-0
14. ^ David Hestenes (1999)[1986] New Foundations for Classical Mechanics, page 34, D. Reidel ISBN 90-277-2090-8
15. ^ C. Doran and A. Lasenby (2003) Geometric Algebra for Physicists, page 87, Cambridge University Press ISBN 9780511807497
16. ^ Marcos A. Rodrigues (2000). "§1.2 Geometric algebra: an outline". Invariants for pattern recognition and classification. World Scientific. p. 3 ff. ISBN 981-02-4278-6.
17. ^ R Wareham, J Cameron & J Lasenby (2005). "Applications of conformal geometric algebra in computer vision and graphics". In Hongbo Li; Peter J. Olver; Gerald Sommer (eds.). Computer algebra and geometric algebra with applications. Springer. p. 330. ISBN 3-540-26296-2.
18. ^ Eduardo Bayro-Corrochano (2004). "Clifford geometric algebra: A promising framework for computer vision, robotics and learning". In Alberto Sanfeliu; José Francisco Martínez Trinidad; Jesús Ariel Carrasco Ochoa (eds.). Progress in pattern recognition, image analysis and applications. Springer. p. 25. ISBN 3-540-23527-2.
19. ^ R. Penrose (2007). The Road to Reality. Vintage books. ISBN 0-679-77631-1.
20. ^ J.A. Wheeler; C. Misner; K.S. Thorne (1973). Gravitation. W.H. Freeman & Co. p. 83. ISBN 0-7167-0344-0.