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Clifford Geometric Algebra (GA)

“If the world was complicated, everyone would understand it.”. Woody Allen. Clifford Geometric Algebra (GA). Vector cross product a x b. A unified mathematical formalism for science and engineering. Quaternions q. Complex numbers i. Tensors F ij. Complex wave functions.

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Clifford Geometric Algebra (GA)

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  1. “If the world was complicated, everyone would understand it.” Woody Allen Clifford Geometric Algebra (GA) Vector cross product a x b A unified mathematical formalism for science and engineering Quaternions q Complex numbers i Tensors Fij Complex wave functions Rotation matrices R Spinors Differential forms

  2. Vector cross product a x b Quaternions q Complex numbers i Tensors Fij Complex wave functions Rotation matrices R Spinors Differential forms A unified language for science Appropriate mathematical modelling of physical space Divide by vectors Quantum mechanics over the reals GA Special relativity without an extra time dimension Strictly real field Naturally incorporates complex numbers and quaternions Maxwell's four equations reduce to one

  3. Euclid’s textbook current for 2000 years! 300 BC, Euclid-"Father of Geometry" Timeline of Mathematics 2000 1637 Cartesian coordinates-Descartes 1545 number line developed 1170-1250 debts seen as negative numbers-Pisa 1000 800 zero used in India 0 BC: negative numbers used in India and China 500 BC d 547 BC, Thales-”the first true mathematician”

  4. y Descartes analytic geometry Descartes in 1637 proposes that a pair of numbers can represent a position on a surface. (4,1) x Analytic geometry: “…the greatest single step ever made in the exact sciences.” John Stuart Mill

  5. v u y Descartes analytic geometry • Adding vectors u+v? (3,4) v u Add head to tail: same as the number line but now in 2D (2,1) x

  6. y Descartes analytic geometry • Multiply vectors u v ? v (3,4) Dot and cross products • Divide vectors u/v ? 5 • 1/v ? u (2,1) x

  7. 1/v Y’ Descartes analytic geometry • Learning to take the reciprocal of a vector: • Imagine the vector lying along the number line • Find the reciprocal • Reorientate vector, bingo! Reciprocal of a vector. v X’ 5

  8. y Descartes analytic geometry v (3,4) 5 The reciprocal of a Cartesian vector is a vector of the same direction but the reciprocal length. 1/v 0.2 x

  9. Timeline 2000 1799 Complex numbers, Argand diagram 1637 Cartesian coordinates-Descarte 1545 negative numbers established, number line 1170-1250 debts seen as negative numbers-Pisa 1000 0 300BC, Euclid-"Father of Geometry" d 475BC, Pythagoras 500BC d 547BC, Thales-”the first true mathematician”

  10. 1/v Argand diagram i y v 3+4i As operators, complex numbers describe Rotations and dilations, and hence an inverse vector is a vector of reciprocal length, with opposite direction of rotation. 5 4 x Representation vs Operator?

  11. Timeline What about three dimensional space? 2000 1843 Quaternions-Hamilton ?! 1799 Complex numbers, Argand diagram 1637 Cartesian coordinates-Descarte 1545 negative numbers established, number line 1170-1250 debts seen as negative numbers-Pisa 1000 0 300BC, Euclid-"Father of Geometry" d 475BC, Pythagoras 500BC d 547BC, Thales-”the first true mathematician”

  12. Quaternions j • The generalization of the algebra of complex numbers to three dimensions • i2 = j2 = k2 = -1, i j = k, k Non-commutative i j =-j i , try rotating a book i

  13. Use of quaternions Used in airplane guidance systemsto avoid Gimbal lock

  14. Quaternions j • i2 = j2 = k2 = -1, i j = k, If we write a space and time coordinate as the quaternion Hamilton observed this provided a natural union of space and time k Maxwell wrote his electromagnetic equations using quaternions. i

  15. Rival coordinate systems 2D 3D y z Cartesian Cartesian v y 1/v x x Argand diagram Quaternions ib k v j a i 1/v Axes non-commutative

  16. Clifford’s Geometric Algebra e3 • Define algebraic elements e1, e2, e3 • With e12=e22=e32=1, and anticommuting • ei ej= - ej ei This algebraic structure unifies Cartesian coordinates, quaternions and complex numbers into a single real framework. Cartesian coordinates described by e1, e2, e3, quaternions by the bivectors e1e2, e3e1, e2e3 , and the unit imaginary by the trivector e1e2e3. e2 e1e2e3 e1e2 e2e3 e1e3 e1

  17. How many space dimensions do we have? • The existence of five regular solids implies three dimensional space(6 in 4D, 3 > 4D) • Gravity and EM follow inverse square laws to very high precision. Orbits(Gravity and Atomic) not stable with more than 3 D. • Tests for extra dimensions failed, must be sub-millimetre

  18. Clifford 3D Geometric Algebra e3 e2 ι=e1e2e3 e1e2 e2e3 e1e3 e1

  19. Timeline 2000 1878 Geometric algebra-Clifford 1843 Quaternions-Hamilton 1799 Complex numbers, Argand diagram 1637 Cartesian coordinates-Descarte 1545 negative numbers established, number line 1170-1250 debts seen as negative numbers-Pisa 1000 0 300BC, Euclid-"Father of Geometry" d 475BC, Pythagoras 500BC d 547BC, Thales-”the first true mathematician”

  20. Cliffords geometric algebra • Clifford’s mathematical system incorporating 3D Cartesian coordinates, and the properties of complex numbers and quaternions into a single framework • “should have gone on to dominate mathematical physics….”, but…. • Clifford died young, at the age of just 33 • Vector calculus was heavily promoted • by Gibbs and rapidly became popular, eclipsing Clifford’s work, which in comparison appeared strange with its non-commuting variables and bilinear transformations for rotations.

  21. Geometric Algebra-Dual representation e3 e2 ι=e1e2e3 e1e2 e2e3 e1e3 e1

  22. We now note that: a scalar. a vector with the same direction and inverse length. Therefore the inverse vector is: To check we calculate as required. The product of two vectors…. To multiply 2 vectors we….just expand the brackets… A complex-type number combining the dot and cross products! Hence we now have an intuitive definition of multiplication and division of vectors, subsuming the dot and cross products.

  23. For example: We can write: This now states that an operator x acting twice on a vector returns the negative of the vector. Hence x represents two 90deg rotations, or the bivector of the plane e1e2, which gives which implies as required. So what does mean? Imaginary numbers first appeared as the roots to quadratic equations. They were initially considered `imaginary’, and so disregarded. However x essentially represents a rotation and dilation operator. Real solutions correspond to pure dilations, and complex solutions correspond to rotations and dilations. Hence we can replace the unit imaginary with the real geometric entity, the bivector of the plane e1e2.

  24. Solving a quadratic geometrically Solving the quadratic: is equivalent to solving the triangle: θ ar2 br θ C With a solution: Where x represents a rotation and dilation operator on a vector.

  25. Example: Solve the quadratic: which defines the triangle: θ r2 r θ 1 Thus we have the two solutions, both in the field of real numbers, with the geometric interpretation of the solutions as 60 deg rotations in the plane.

  26. Maxwell’s equations Where:

  27. Maxwell in GA

  28. Maxwell’s equations in GA Four-gradient Field variable Four-current Exercise: Describe Maxwell’s equations in English.

  29. Gibb’s vectors vs GA

  30. Using: Law of Cosines

  31. Reflection of rays R Normal n I Mirror

  32. The versatile multivector (a generalized number) a+ιb v ιw ιb v+ιw a+ιw a+v Complex numbers Vectors Pseudovectors Pseudoscalars Anti-symmetric EM field tensor E+iB Quaternions or Pauli matrices Four-vectors

  33. Research areas in GA • black holes and cosmology • quantum tunneling and quantum field theory • beam dynamics and buckling • computer vision, computer games • quantum mechanics-EPR • quantum game theory • signal processing-rotations in N dimensions, wedge product also generalizes to N dimensions

  34. Penny Flip game Qubit Solutions

  35. Grover search in GA After iterations of Grover operator will find solution state In GA we can write the Grover operator as:

  36. Spinor mapping How can we map from complex spinors to 3D GA? We see that spinors are rotation operators.

  37. Probability distribution Where Doran C, Lasenby A (2003) Geometric algebra for physicists

  38. Conventional Dirac Equation “Dirac has redisovered Clifford algebra..”, Sommerfield That is for Clifford basis vectors we have: isomorphic to the Dirac agebra.

  39. Free Maxwell equation(J=0): Dirac equation in real space Same as the free Maxwell equation, except for the addition of a mass term and expansion of the field to a full multivector.

  40. The multivector now puts the reals, complex numbers and quaternions all on an equal footing. The Maths family “The real numbers are the dependable breadwinner of the family, the complete ordered field we all rely on. The complex numbers are a slightly flashier but still respectable younger brother: not ordered, but algebraically complete. The quaternions, being noncommutative, are the eccentric cousin who is shunned at important family gatherings. But the octonions are the crazy old uncle nobody lets out of the attic: they are nonassociative.”—John Baez

  41. The correct algebra of three-space e3 We show in the next slide that time can be represented as the bivectors of this real Clifford space. e2 ι=e1e2e3 e1e2 e2e3 e1e3 e1

  42. Special relativity Its simpler to begin in 2D, which is sufficient to describe most phenomena. We define a 2D spacetime event as So that time is represented as the bivector of the plane and so an extra Euclidean-type dimension is not required. This also implies 3D GA is sufficient to describe 4D Minkowski spacetime. We find: the correct spacetime distance. We have the general Lorentz transformation given by: Consisting of a rotation and a boost, which applies uniformly to both coordinate and field multivectors. Compton scattering formula C

  43. Time after time • “Of all obstacles to a thoroughly penetrating account of existence, none looms up more dismayingly than time.” Wheeler 1986 • In GA time is a bivector, ie rotation. • Clock time and Entropy time

  44. Foundational errors in mathematical physics • By not recognizing that the vector dot and cross products are two halves of a single combined geometric product. Circa 1910. • That the non-commuting properties of matrices are a clumsy substitute for Clifford’s non-commuting orthonormal axes of three-space. Circa 1930.

  45. The leaning tower Of Pisa, Italy u.v u x v Matrices as basis vectors “I skimped a bit on the foundations, but no one is ever going to notice.”

  46. Summary • Clifford's geometric algebra provides the most natural representation of three-space, encapsulating the properties of Cartesian coordinates, complex numbers and quaternions, in a single unified formalism over the real field. • Vectors now have a division and square root operation. • Maxwell's four equations can be condensed into a single equation, and the complex four-dimensional Dirac equation can be written in real three dimensional space. • SR is described within a 3D space replacing Minkowski spacetime   •  GA is proposed as a unified language for physics and engineering which subsumes many other mathematical formalisms, into a single unified real formalism.

  47. Geometric Algebra The End References: http://www.mrao.cam.ac.uk/~clifford/

  48. The geometric product magnitudes In three dimensions we have:

  49. Negative Numbers • Interpreted financially as debts by Leonardo di Pisa,(A.D. 1170-1250) • Recognised by Cardano in 1545 as valid solutions to cubics and quartics, along with the recognition of imaginary numbers as meaningful. • Vieta, uses vowels for unknowns and use powers. Liebniz 1687 develops rules for symbolic manipulation. Modern Diophantus 200AD

  50. Precession in GASpin-1/2 Bz Z=σ3 ω θ <Sx>=Sin θ Cos ωt <Sy>=Sin θ Sin ωt <Sz>=Cos θ x= σ1 ω = γ Bz Y= σ2

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