Research Article | Open Access
Rotations in the Space of Split Octonions
The geometrical application of split octonions is considered. The new representation of products of the basis units of split octonionic having David's star shape (instead of the Fano triangle) is presented. It is shown that active and passive transformations of coordinates in octonionic “eight-space” are not equivalent. The group of passive transformations that leave invariant the pseudonorm of split octonions is , while active rotations are done by the direct product of -boosts and real noncompact form of the exceptional group . In classical limit, these transformations reduce to the standard Lorentz group.
Nonassociative algebras may surely be called beautiful mathematical entities. However, they have never been systematically utilized in physics, only some attempts have been made toward this goal. Nevertheless, there are some intriguing hints that nonassociative algebras may play essential role in the ultimate theory, yet to be discovered.
Octonions are one example of a nonassociative algebra. It is known that they form the largest normed algebra after the algebras of real numbers, complex numbers, and quaternions [1–3]. Since their discovery in 1844/1845 by Graves and Cayley there have been various attempts to find appropriate uses for octonions in physics (see reviews [4–7]). One can point to the possible impact of octonions on: Color symmetry [8–11]; GUTs [12–15]; Representation of Clifford algebras [16–19]; Quantum mechanics [20–24]; Space-time symmetries [25, 26]; Field theory [27–29]; Formulations of wave equations [30–32]; Quantum Hall effect ; Kaluza-Klein program without extra dimensions [34–36]; Strings and -theory [37–40]; and so forth.
2. Octonionic Geometry
Let us review the main ideas behind the geometrical application of split octonions presented in our previous papers [41–43]. In our model some characteristics of physical world (such as dimension, causality, maximal velocities, and quantum behavior) can be naturally described by the properties of split octonions. Interesting feature of the geometrical interpretation of the split octonions is that their pseudonorms, in addition to some other terms, already contain the ordinary Minkowski metric. This property is equivalent to the existence of local Lorentz invariance in classical physics.
To any physical signal we correspond eight-dimensional number, the element of split octonions, Here we have one scalar basis unit (denoted as ), the three vector-like objects , the three pseudovector-like elements , and one pseudoscalar-like unit . The eight real parameters that multiply basis elements we treat as the time , the special coordinates , some quantities with the dimensions , and the quantity having the dimension . We suppose also that (2.1) contains two fundamental constants of physics: the velocity of light and the Planck constant .
The squares of basis units of split octonions are inner product resulting unit element, but with the opposite signs, Multiplications of different hypercomplex basis units are defined as skew products , where is the fully antisymmetric tensor.
From (2.3) we notice that to generate complete basis of split octonions the multiplication and distribution laws of only three vector-like elements are needed. In geometrical application this can explain why classical space has three dimensions. The three pseudovector-like basis units can be defined as the binary product and thus can describe oriented orthogonal planes spanned by two vector-like elements . The seventh basic unit (the oriented volume) is formed by the products of all three fundamental basis elements and has three equivalent representation:
The multiplication table of octonionic units is most transparent in graphical form. To visualize the products of ordinary octonions the Fano triangle is used [1–3], where the seventh basic unit is place at the center of the graph. In the algebra of split octonions we have less symmetry, and for a proper description of the products (2.3) the Fano graph should be modified by shifting from the center of the Fano triangle. Also we will use three equivalent representations of , (2.5), and, instead of the Fano triangle, we arrive at David's star shaped duality plane for products of the split octonionic basis elements.
On this graph the product of two basis units is determined by following the oriented solid line connecting the corresponding nodes. Moving opposite to the orientation of the line contributes a minus sign to the result. Dashed lines just show that the corners of the triangle with nodes are identified.
Conjugation, which can be understand as a reflection of the vector-like basis units , reverses the order of octonionic basis elements in any given expression, thus there is no summing in the last formula. So the conjugation of (2.1) gives Using (2.2) one can find that the pseudonorm of (2.1), has signature. If we consider as the interval between two octonionic signals we see that (2.8) reduces to the classical formula of Minkowski space-time in the limit .
Using the algebra of basis elements (2.3) the octonion (2.1) can be written in the equivalent form We notice that the pseudoscalar-like element introduces the 'quantum' term corresponding to some kind of uncertainty of space-time coordinates. For the differential form of (2.9) the invariance of the pseudonorm (2.8) gives the relation: where denotes 3-dimensional velocity measured in the frame (2.1). The generalized Lorentz factor (2.10) contains extra terms that vanish in the limit . So the dispersion relation in our model has a form similar to that of double-special relativity models [44, 45].
From the requirement to have the positive pseudonorm (2.8) from (2.10) we obtain several relations Recalling that and have dimensions of and , respectively, we conclude that the Heisenberg uncertainty principle in our model has the same geometrical meaning as the existence of the maximal velocity in Minkowski space-time.
Since the squares of the pseudovector-like elements are negative, , we can define where are some real angles.
At the same time for the other basis elements , which have the positive squares , we have where and are real numbers.
In 8-dimensional octonionic “space-time’’ (2.1) there is no unique plane orthogonal to a given axis. Therefore for the operators (3.1) and (3.2) it is not sufficient to specify a single rotation axis and an angle of rotation. It can be shown that the left multiplication of the octonion by one of the operators (3.1), (3.2) (e.g., ) yields four simultaneous rotations in four mutually orthogonal planes. For simplicity we consider only the left products since it is known that one side multiplications generate the whole symmetry group that leaves the octonionic norms invariant .
So rotations naturally provide splitting of an octonion in four orthogonal planes. To define these planes note that one of them is formed by the hypercomplex element that we chose to define the rotation ( in our example), together with the scalar unit element of the octonion. The rest orthogonal planes are given by the three pairs of other basis elements that lie with the considered basis unit ( in the example) on the lines emerged it in David's star (see Figure 1). Thus the pairs of basis units that are rotated into each other are the pairs that form associative triplets with the considered basis unit. For example, the basis unit , according to Figure 1, has three different representations in the octonionic algebra: So the planes orthogonal to are , , and . Using (3.3) and the representation (3.1) it is possible to “rotate out’’ the four octonionic axes, and (2.1) can be written in the equivalent form where are the norms in four orthogonal octonionic planes. The corresponding angles are given by This decomposition of split octonion is valid only if the full pseudonorm of the octonion (2.8) is positive, that is, A decomposition similar to (3.4) exists if the another pseudovector-like basis unit, or , is fixed.
In contrast with uniform rotations giving by the operators we have limited rotations in the planes orthogonal to and . However, we can still perform a decomposition similar to (3.4) of using expressions of the exponential maps (3.2). But now, unlike on (3.5), the norms of the corresponding planes are not positively defined and, instead of the condition (3.7), we should require positiveness of the norms of each four planes. For example, the pseudoscalar-like basis unit has three different representations (2.5), and it can provide the hyperbolic rotations (3.2) in the orthogonal planes , , , and . The expressions for the 2 norms (3.5) in this case are: , , , and .
Now let us consider active and passive transformations of coordinates in 8-dimensional space of signals (2.1). With a passive transformation we mean a change of the coordinates , , , and , as opposed to an active transformation which changes the basis , , , and .
The passive transformations of the octonionic coordinates , , , and , which leave invariant the norm (2.8) form . We can represent these transformations of (2.1) by the left products where is one of (3.1), (3.2). The operator simultaneously transforms four planes of . However, in three planes can be rotated out by the proper choice of octonionic basis. Thus can represent rotations separately in four orthogonal planes of . Similarly we have some four angles for the other six operators (3.1), (3.2) and thus totally parameters corresponding to group of passive coordinate transformations. For example, in the case of the decomposition (3.4) we can introduce four arbitrary angles , , , and , and Obviously under these transformations the pseudonorm (2.8) is invariant. By the fine tuning of the angles in (3.9) we can define rotations in any single plane from four.
Now let us consider active coordinate transformations, or transformations of basis units , , , and . For them, because of nonassociativity, the results of two different rotations (3.1) and (3.2) are not unique. This means that not all active octonionic transformations (3.1) and (3.2) form a group and can be considered as a real rotation. Thus in the octonionic space (2.1) not to the all passive -transformations we can make corresponding active ones, only the transformations that have a realization as associative multiplications should be considered. It is known that associative transformations can be done by the combined rotations of special form in two octonionic planes that form a subgroup of , known as the automorphism group of split octonions (the real noncompact form of Cartan's exceptional Lie group ). Some general results on and its subgroup structure can be found in [47,16b].
Let us recall that the automorphism of a algebra is defined as the transformations of the hypercomplex basis units and under which the multiplication table of the algebra is invariant, that is, Associativity of these transformations is obvious from the second relation, and the set of all automorphisms of composition algebras form a group. In the case of quaternions, because of associativity, active and passive transformations, and , respectively, are isomorphic and quaternions are useful to describe rotations in 3-dimensional space. One has a different situation for octonions. Each automorphism in the octonionic algebra is completely defined by the images of three elements that do not form quaternionic subalgebras, that is, they all not lie on the same David's line . Consider one such set, say . Then there exists an automorphism where and are some independent real angles. By the definition (3.10) the automorphism does not affect unit scalar . The images of the other basis elements under automorphism (3.11) are determined by the conditions
It can easily be checked that transformed bases , , satisfy the same multiplication rules as , , .
There exist similar automorphisms with fixed and axes, which are generated by the angles , and , , respectively.
One can define also hyperbolic automorphisms for the vector-like units by the angles . For example, for fixed similar to (3.11) and (3.12) transformations are Analogously in the case of fixed we find that
So for each octonionic basis there are seven independent automorphisms each introducing two angles that correspond to generators of the algebra . For our choice of basis the infinitesimal passive transformation of the coordinates, corresponding to , has the form where is the symmetric matrix
In the limit the transformations (3.15) reduce to the standard rotations of Euclidean 3-space by the Euler angles .
The formulas (3.15) represent rotations of (3,4)-sphere that is orthogonal to the time coordinate . To define the boosts note that active and passive forms of mutual transformations of with , and are isomorphic and can be described by the seven operators (3.1) and (3.2) (e.g., the first term in (3.9), which form the group . In the case we recover the standard Lorentz boost in the Minkowski space-time governing by the operators , where .
In this paper the David's star duality plane, which describes the multiplication table of the basis units of split octonions (instead of the Fano triangle of ordinary octonions), was introduced. Different kind of rotations in the split octonionic space was considered. It was shown that in octonionic space active and passive transformations of coordinates are not equivalent. The group of passive coordinate transformations, which leave invariant the pseudonorms of split octonions, is , while active rotations are done by the direct product of the seven -boosts and fourteen -rotations. In classical limit these transformations give the standard 6-parametrical Lorentz group.
The author would like to acknowledge the support of a 2008-2009 Fulbright Fellowship.
- R. Schafer, Introduction to Non-Associative Algebras, Dover, New York, NY, USA, 1995.
- T. A. Springer and F. D. Veldkamp, Octonions, Jordan Algebras and Exceptional Groups, Springer Monographs in Mathematics, Springer, Berlin, Germany, 2000.
- J. C. Baez, “The octonions,” Bulletin of the American Mathematical Society, vol. 39, no. 2, pp. 145–205, 2002.
- D. Finkelstein, Quantum Relativity: A Synthesis of the Ideas of Einstein and Heisenberg, Springer, Berlin, Germany, 1996.
- G. Emch, Algebraic Methods in Statistical Mechanics and Quantum Field Theory, John Wiley & Sons, New York, NY, USA, 1972.
- F. Gürsey and C. Tze, On the Role of Division, Jordan and Related Algebras in Particle Physics, World Scientific, Singapore, 1996.
- J. Lõhmus, E. Paal, and L. Sorgsepp, Nonassociative Algebras in Physics, Hadronic Press, Palm Harbor, Fla, USA, 1994.
- M. Günaydin and F. Gürsey, “Quark statistics and octonions,” Journal of Mathematical Physics, vol. 14, no. 11, pp. 1651–1667, 1973.
- M. Günaydin and F. Gürsey, “Quark statistics and octonions,” Physical Review D, vol. 9, no. 12, pp. 3387–3391, 1974.
- S. L. Adler, “Quaternionic chromodynamics as a theory of composite quarks and leptons,” Physical Review D, vol. 21, no. 10, pp. 2903–2915, 1980.
- K. Morita, “Octonions, quarks and QCD,” Progress of Theoretical Physics, vol. 65, no. 2, pp. 787–790, 1981.
- T. Kugo and P. Townsend, “Supersymmetry and the division algebras,” Nuclear Physics B, vol. 221, no. 2, pp. 357–380, 1983.
- A. Sudbery, “Division algebras, (pseudo)orthogonal groups and spinors,” Journal of Physics A, vol. 17, no. 5, pp. 939–955, 1984.
- G. Dixon, “Derivation of the standard model,” Il Nuovo Cimento B, vol. 105, no. 3, pp. 349–364, 1990.
- S. De Leo, “Quaternions for GUTs,” International Journal of Theoretical Physics, vol. 35, no. 9, pp. 1821–1837, 1996.
- I. R. Porteous, Clifford Algebras and the Classical Groups, Cambridge University Press, Cambridge, UK, 1995.
- S. Okubo, Introduction to Octonions and Other Non-Associative Algebras in Physics, Cambridge University Press, Cambridge, UK, 1995.
- P. Lounesto, Clifford Algebras and Spinors, Cambridge University Press, Cambridge, UK, 2001.
- H. L. Carrion, M. Rojas, and F. Toppan, “Quaternionic and octonionic spinors. A classification,” Journal of High Energy Physics, vol. 7, no. 4, pp. 901–928, 2003.
- D. Finkelstein, J. M. Jauch, S. Schiminovich, and D. Speiser, “Foundations of quaternion quantum mechanics,” Journal of Mathematical Physics, vol. 3, no. 2, pp. 207–220, 1962.
- L. P. Horwitz and L. C. Biedenharn, “Quaternion quantum mechanics: second quantization and gauge fields,” Annals of Physics, vol. 157, no. 2, pp. 432–488, 1984.
- M. Günaydin, C. Piron, and H. Ruegg, “Moufang plane and octonionic quantum mechanics,” Communications in Mathematical Physics, vol. 61, no. 1, pp. 69–85, 1978.
- S. De Leo and P. Rotelli, “Translations between quaternion and complex quantum mechanics,” Progress of Theoretical Physics, vol. 92, no. 5, pp. 917–926, 1994.
- V. Dzhunushaliev, “A non-associative quantum mechanics,” Foundations of Physics Letters, vol. 19, no. 2, pp. 157–167, 2006.
- F. Gürsey, “Symmetries in physics (1600–1980),” in Proceedings of the 1st International Meeting on the History of Scientific Ideas, Seminario d'Història de las Cièncias, Barcelona, Spain, 1987.
- S. De Leo, “Quaternions and special relativity,” Journal of Mathematical Physics, vol. 37, no. 6, pp. 2955–2968, 1996.
- K. Morita, “Quaternionic Weinberg-Salam theory,” Progress of Theoretical Physics, vol. 67, no. 6, pp. 1860–1876, 1982.
- C. Nash and G. C. Joshi, “Spontaneous symmetry breaking and the Higgs mechanism for quaternion fields,” Journal of Mathematical Physics, vol. 28, no. 2, pp. 463–467, 1987.
- S. L. Adler, Quaternion Quantum Mechanics and Quantum Field, Oxford University Press, New York, NY, USA, 1995.
- D. F. Kurdgelaidze, “Fundamentals of nonassociative classical field theory,” Soviet Physics Journal, vol. 29, no. 11, pp. 883–887, 1986.
- A. J. Davies and G. C. Joshi, “A bimodular representation of ten-dimensional fermions,” Journal of Mathematical Physics, vol. 27, no. 12, pp. 3036–3039, 1986.
- S. De Leo and P. Rotelli, “The quaternionic Dirac Lagrangian,” Modern Physics Letters A, vol. 11, no. 5, pp. 357–366, 1996.
- B. A. Bernevig, J. Hu, N. Toumbas, and S.-C. Zhang, “Eight-dimensional quantum hall effect and “octonions”,” Physical Review Letters, vol. 91, no. 23, Article ID 236803, 2003.
- F. D. Smith Jr., “Spin(8) gauge field theory,” International Journal of Theoretical Physics, vol. 25, no. 4, pp. 355–403, 1986.
- M. Pavšič, “A novel view on the physical origin of ,” Journal of Physics A, vol. 41, no. 33, Article ID 332001, 2008.
- C. Castro, “On the noncommutative and nonassociative geometry of octonionic space time, modified dispersion relations and grand unification,” Journal of Mathematical Physics, vol. 48, no. 7, Article ID 073517, 2007.
- D. B. Fairlie and C. A. Manogue, “Lorentz invariance and the composite string,” Physical Review D, vol. 34, no. 6, pp. 1832–1834, 1986.
- K.-W. Chung and A. Sudbery, “Octonions and the Lorentz and conformal groups of ten-dimensional space-time,” Physics Letters B, vol. 198, no. 2, pp. 161–164, 1987.
- J. Lukierski and F. Toppan, “Generalized space-time supersymmetries, division algebras and octonionic M-theory,” Physics Letters B, vol. 539, no. 3-4, pp. 266–276, 2002.
- L. Boya, GROUP 24: Physical and Mathematical Aspects of Symmetries, CRC Press, Paris, France, 2002.
- M. Gogberashvili, “Octonionic electrodynamics,” Journal of Physics A, vol. 39, no. 22, pp. 7099–7104, 2006.
- M. Gogberashvili, “Octonionic version of Dirac equations,” International Journal of Modern Physics A, vol. 21, no. 17, pp. 3513–3523, 2006.
- M. Gogberashvili, “Octonionic geometry,” Advances in Applied Clifford Algebras, vol. 15, no. 1, pp. 55–66, 2005.
- G. Amelino-Camelia, “Relativity in spacetimes with short-distance structure governed by an observer-independent (Planckian) length scale,” International Journal of Modern Physics D, vol. 11, no. 1, pp. 35–59, 2002.
- J. Magueijo and L. Smolin, “Lorentz invariance with an invariant energy scale,” Physical Review Letters, vol. 88, no. 19, Article ID 190403, 2002.
- C. A. Manogue and J. Schray, “Finite Lorentz transformations, automorphisms, and division algebras,” Journal of Mathematical Physics, vol. 34, no. 8, pp. 3746–3767, 1993.
- J. Beckers, V. Hussin, and P. Winternitz, “Nonlinear equations with superposition formulas and the exceptional group . I. Complex and real forms of and their maximal subalgebras,” Journal of Mathematical Physics, vol. 27, no. 9, pp. 2217–2227, 1986.
- J. Beckers, V. Hussin, and P. Winternitz, “Nonlinear equations with superposition formulas and the exceptional group . II. Classification of the equations,” Journal of Mathematical Physics, vol. 28, no. 3, pp. 520–529, 1987.
- M. Zorn, “The automorphisms of Cayley's non-associative algebra,” Proceedings of the National Academy of Sciences of the United States of America, vol. 21, no. 6, pp. 355–358, 1935.
Copyright © 2009 Merab Gogberashvili. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.