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On transformations Jean Pierre Rukundo Email: [email protected] March 29th, 2016

Abstract

In this paper, a general spacetime transformation from left and right multiplications is introduced. First, it is shown that the transformation leaves the spacetime length . Furthermore, the is derived as a special case of the general biquaternion transformation. Surprisingly, some commutation and anticommutation properties generally found in quantum are manifested by the biquaternion transformation. I. Introduction

In 1843, introduced the concept of which extended the concept of complex to three imaginary components. One year late, he introduced the concept of biquaternion which are combination of ordinary complex with quaternion. More than half a century later, introduced the special which was based on a transformation introduced by earlier. In this paper, it is shown that the special theory of relativity is generally based on the concept of biquaternion multiplication and a general biquaternion transformation in the form of biquaternion left and right multiplication is introduced, where the Lorentz transformation is shown to be a special case. Finally, some useful properties of the biquaternion transformation such as commutation and anticommutation relations known for Pauli matrices as well as a derivation of an equivalent of Dirac matrices are also shown. II. Biquaternion Transformation Matrices a. Boost along arbitrary direction

Consider the four 푈 = [푢푐푡, 푢푥, 푢푦, 푢푧] and 푉 = [푣푐푡, 푣푥, 푣푦, 푣푧] which satisfies

2 2 2 2 2 2 2 2 2 2 푢푐푡 − 푢푥 − 푢푦 − 푢푧 = 푐 and 푣푐푡 − 푣푥 − 푣푦 − 푣푧 = 푐 . Let us intruduce a boost along an arbitrary direction with transformations

′ 푢 −𝑖푢 −𝑖푢 −𝑖푢 푐푡 푐푡 푥 푦 푧 푐푡 ′ 1 𝑖푢 푢 −𝑖푢 𝑖푢 𝑖푥 푥 푐푡 푧 푦 𝑖푥 [ ′] = ∙ [ ] (1) 𝑖푦 푐 𝑖푢푦 𝑖푢푧 푢푐푡 −𝑖푢푥 𝑖푦 ′ 𝑖푧 [𝑖푢푧 −𝑖푢푦 𝑖푢푥 푢푐푡 ] 𝑖푧 and ′ 푣 −𝑖푣 −𝑖푣 −𝑖푣 푐푡 푐푡 푥 푦 푧 푐푡 ′ 1 𝑖푣 푣 𝑖푣 −𝑖푣 𝑖푥 푥 푐푡 푧 푦 𝑖푥 [ ′] = ∙ [ ] (2) 𝑖푦 푐 𝑖푣푦 −𝑖푣푧 푣푐푡 𝑖푣푥 𝑖푦 ′ 𝑖푧 [𝑖푣푧 𝑖푣푦 −𝑖푣푥 푣푐푡 ] 𝑖푧 Note that transformations in equations (1) and (2) are equivalent to the right and left multiplication of with real component and pure imaginary spatial components.

From both equations (1) and (2), computing 푐푡′ 𝑖푥′ [푐푡′, 𝑖푥′, 𝑖푦′, 𝑖푧′] ∙ [ ] (3) 𝑖푦′ 𝑖푧′ yields

푐2푡′2 − 푥′2 − 푦′2 − 푧′2 = 푐2푡2 − 푥2 − 푦2 − 푧2 (4) Which means that transformations in equations (1) and (2) leave the spacetime length invariant.

A combination of transformations of the left and right multiplication of the biquaternions in equations (1) and (2) can be written as

′ 푢 −𝑖푢 −𝑖푢 −𝑖푢 푣 −𝑖푣 −𝑖푣 −𝑖푣 푐푡 푐푡 푥 푦 푧 푐푡 푥 푦 푧 푐푡 ′ 1 𝑖푢 푢 −𝑖푢 𝑖푢 𝑖푣 푣 𝑖푣 −𝑖푣 𝑖푥 푥 푐푡 푧 푦 푥 푐푡 푧 푦 𝑖푥 [ ′] = 2 ∙ ∙ [ ] (5) 𝑖푦 푐 𝑖푢푦 𝑖푢푧 푢푐푡 −𝑖푢푥 𝑖푣푦 −𝑖푣푧 푣푐푡 𝑖푣푥 𝑖푦 ′ 𝑖푧 [𝑖푢푧 −𝑖푢푦 𝑖푢푥 푢푐푡 ] [𝑖푣푧 𝑖푣푦 −𝑖푣푥 푣푐푡 ] 𝑖푧 Equation (5) also satisfies the Minkowski spacetime length invariance in equation (4).

b. Boost along the x axis case

Consider the case 푢푦 = 푢푧 = 푣푦 = 푣푧 = 0. The left and the right transformations in equations (1) and (2) become respectively

′ 푐푡 푢푐푡 −𝑖푢푥 0 0 푐푡 ′ 𝑖푥 1 𝑖푢푥 푢푐푡 0 0 𝑖푥 [ ′] = [ ] ∙ [ ] (6) 𝑖푦 푐 0 0 푢푐푡 −𝑖푢푥 𝑖푦 ′ 𝑖푧 0 0 𝑖푢푥 푢푐푡 𝑖푧 ′ 푐푡 푣푐푡 −𝑖푣푥 0 0 푐푡 ′ 𝑖푥 1 𝑖푣푥 푣푐푡 0 0 𝑖푥 [ ′] = [ ] ∙ [ ] (7) 𝑖푦 푐 0 0 푣푐푡 𝑖푣푥 𝑖푦 ′ 𝑖푧 0 0 −𝑖푣푥 푣푐푡 𝑖푧

Furthermore, consider the case 푢푐푡 = 푣푐푡 and 푢푥 = 푣푥. The combined left and right transformation in equation (5) become ′ 푢2 + 푢2 −2𝑖푢 푢 0 0 푐푡 푐푡 푥 푐푡 푥 푐푡 ′ 2 2 𝑖푥 1 2𝑖푢푐푡푢푥 푢 + 푢푥 0 0 𝑖푥 [ ] = 푐푡 ∙ [ ] (8) 𝑖푦′ 푐2 2 2 𝑖푦 0 0 푢푐푡 − 푢푥 0 ′ 2 2 𝑖푧 𝑖푧 [ 0 0 0 푢푐푡 − 푢푥]

푢 휂 푢 휂 We can use the as 푐푡 = cosh ( ) and 푥 = 푠𝑖푛ℎ ( ). Then, we have 푐 2 푐 2

1 휂 2 휂 2 2 휂 휂 (푢2 + 푢2) = 푐표푠ℎ ( ) + 푠𝑖푛ℎ ( ) = coshη, 푢 푢 = 2 cosh ( ) 푠𝑖푛ℎ ( ) = 푠𝑖푛ℎ휂 and of 푐2 푐푡 푥 2 2 푐2 푐푡 푥 2 2 1 휂 2 휂 2 course, (푢2 − 푢2) = 푐표푠ℎ ( ) − 푠𝑖푛ℎ ( ) = 1. Equation (8) become 푐2 푐푡 푥 2 2 푐푡′ coshη −𝑖푠𝑖푛ℎ휂 0 0 푐푡 𝑖푥′ 𝑖푠𝑖푛ℎ휂 coshη 0 0 𝑖푥 [ ] = [ ] ∙ [ ] (9) 𝑖푦′ 0 0 1 0 𝑖푦 𝑖푧′ 0 0 0 1 𝑖푧 Which is the standard Lorentz transformation for a boost along the x axis. III. Some Properties of the Biquaternion Transformation Matrices a. Notation

Let us introduce the following notation:

′ 푢 −𝑖푢 −𝑖푢 −𝑖푢 푣 −𝑖푣 −𝑖푣 −𝑖푣 푐푡 푐푡 푐푡 푥 푦 푧 푐푡 푥 푦 푧 ′ 𝑖푢 푢 −𝑖푢 𝑖푢 𝑖푣 푣 𝑖푣 −𝑖푣 𝑖푥 ′ 𝑖푥 푥 푐푡 푧 푦 푥 푐푡 푧 푦 푋 = [ ],푋 = [ ′], 푈퐿 = and 푉푅 = (10) 𝑖푦 𝑖푦 𝑖푢푦 𝑖푢푧 푢푐푡 −𝑖푢푥 𝑖푣푦 −𝑖푣푧 푣푐푡 𝑖푣푥 ′ 𝑖푧 𝑖푧 [𝑖푢푧 −𝑖푢푦 𝑖푢푥 푢푐푡 ] [𝑖푣푧 𝑖푣푦 −𝑖푣푥 푣푐푡 ] Equations (1), (2) and (5) can now be written as

1 1 1 푋′ = 푈 ∙ 푋 , 푋′ = 푉 ∙ 푋 and 푋′ = 푈 ∙ 푉 ∙ 푋 (11) 푐 퐿 푐 푅 푐2 퐿 푅

푈퐿 and 푉푅 can also be written as

휇 휇 푈퐿 = 훼 푢휇 and 푉푅 = 훽 푣휇 (12)

With 1 0 0 0 0 1 0 0 훼0 = 훽0 = [ ] (13) 0 0 1 0 0 0 0 1 0 −𝑖 0 0 0 0 −𝑖 0 0 0 0 −𝑖 𝑖 0 0 0 0 0 0 𝑖 0 0 −𝑖 0 훼1 = [ ] , 훼2 = [ ] and 훼3 = [ ] (14) 0 0 0 −𝑖 𝑖 0 0 0 0 𝑖 0 0 0 0 𝑖 0 0 −𝑖 0 0 𝑖 0 0 0 0 −𝑖 0 0 0 0 −𝑖 0 0 0 0 −𝑖 𝑖 0 0 0 0 0 0 −𝑖 0 0 𝑖 0 훽1 = [ ] , 훽2 = [ ] and 훽3 = [ ] (15) 0 0 0 𝑖 𝑖 0 0 0 0 −𝑖 0 0 0 0 −𝑖 0 0 𝑖 0 0 𝑖 0 0 0

b. Properties of Alphas and Betas Matrices

Alphas and Betas matrices in equations (14) and (15) have commutation relations

푖 푗 푘 [훼 , 훼 ] = 2𝑖휖푖푗푘훼 (16) 푖 푗 푘 [훽 , 훽 ] = −2𝑖휖푖푗푘훽 (17) Also, they have the following anticommutation relations

{훼푖, 훼푗} = 2훿푖푗퐼 (18) {훽푖, 훽푗} = 2훿푖푗퐼 (19)

These properties are also known for and we can construct equivalent Dirac matrices set 0 0 0 −𝑖 0 0 𝑖 0 훾0 = 훽3 = [ ] (20) 0 −𝑖 0 0 𝑖 0 0 0 𝑖 0 0 0 0 𝑖 0 0 훾1 = 𝑖훽1 ∙ 훼1 = [ ] (21) 0 0 −𝑖 0 0 0 0 −𝑖 0 0 0 𝑖 0 0 𝑖 0 훾2 = 𝑖훽1 ∙ 훼2 = [ ] (22) 0 𝑖 0 0 𝑖 0 0 0 0 0 −𝑖 0 0 0 0 𝑖 훾3 = 𝑖훽1 ∙ 훼3 = [ ] (23) −𝑖 0 0 0 0 𝑖 0 0 With anticommutation properties

{훾휇, 훾휈} = 2𝑔휇휈퐼 (24)

1 1 Also, using the anticommutation relations in equations (18) and (19) and 휂 and 휃, 2 2 transformation matrices in equation (11) can be written as

ퟏ 1 휶∙휼 푈 = 푒ퟐ (25) 푐 퐿 ퟏ 1 휷∙휽 푉 = 푒ퟐ (26) 푐 푅 ퟏ ퟏ 1 휶∙휼 휷∙휽 푈 ∙ 푉 = 푒ퟐ ∙ 푒ퟐ (27) 푐2 퐿 푅

IV. Discussion and Conclusion

The general biquaternion transformation introduced in equation (5) leaves the spacetime length invariant and the Lorentz transformation in equation (9) is shown to be the special case of the general biquaternion transformation. Intuitively, the biquaternion transformation in equation (5) is equivalent to the in four-dimensional Euclidian space where imaginary components for Minkowski spacetime are introduced and it is isomorphic to Van Elfrinkhof (1897) rotation formula in Euclidian space. Finally, section III on properties of the biquaternion transformation matrices shows the relation of the biquaternion transformations to Pauli and Dirac matrices, so this work suggests a natural extension of biquaternion transformation to quantum mechanics as demonstrated in article [1]. V. Reference

[1] Rukundo, JPR, 2017. On gauge approach of interactions. Quaternion , [Online]. 1, 5. Available at: https://quaternionphysics.files.wordpress.com/2017/11/on-velocity- gauge-field-approach-of-interactions8.pdf [Accessed 26 November 2017].