geometric algebra 4 2 final ideasweb.mit.edu/tfhavel/www/cmi-qip-ws.win03/doranmit4.pdf• geometric...
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![Page 1: Geometric Algebra 4 2 Final Ideasweb.mit.edu/tfhavel/www/CMI-QIP-WS.Win03/DoranMIT4.pdf• Geometric Algebra for Physicists out in March (C.U.P.) • David Hestenes’ website modelingnts.la.asu.edu](https://reader036.vdocument.in/reader036/viewer/2022070809/5f0873b47e708231d42214a2/html5/thumbnails/1.jpg)
Geometric Algebra 42 Final Ideas
Chris DoranAstrophysics Group
Cavendish LaboratoryCambridge, UK
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MIT 4 2003 2
Gravity• Can construct gravity as a gauge theory• Predictions fully consistent with general
relativity• General covariance replace by demand that
observables are gauge invariant• Equivalence principal replaced by minimal
coupling• No need for any differential geometry• Can apply GA ideas directly
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MIT 4 2003 3
The Gauge Fields• Remove the constraint that coordinate
vectors are tied to a frame
• Generates the ‘metric’ via
• Theory invariant under local rotations
• Include gauge fields for Lorentz rotations• Set of bivector fields• Field strength is Riemann tensor
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MIT 4 2003 4
Dirac Equation• The Dirac equation in a gravitational
background in
• Observables constructed in precisely the same way
• These are full covariant objects• All observables are scalar combinations of
these
Gauge fields
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MIT 4 2003 5
Black Hole• Gauge fields for a Schwarzschild black hole
are extremely simple
• Metric from this gauge choice is
‘Flat’ Minkowski vectors
Gravitational interaction
Free-fall time
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MIT 4 2003 6
Dirac Equation• Dirac equation now reduces to
• All gravitational effects are contained in the scalar Hamiltonian
Free-fall velocity Radial momentum
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MIT 4 2003 7
The Interaction Hamiltonian
• All gravitational effects in a single term• This is gauge dependent• In all gauge theories, trick is to
1. Find a sensible gauge2. Ensure that all physical predictions are
gauge invariant• Hamiltonian is scalar (no spin effects)• Independent of particle mass• Independent of c
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MIT 4 2003 8
Applications• Can carry out scattering calculations using
Feynman diagram techniques• Construct the gravitational analogue of the
Mott scattering formula• Hamiltonian is non-Hermitian due to delta-
function at the origin• Describes absorption• Compute a quantum spectrum of bound
states
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MIT 4 2003 10
Conformal Geometry• Totally separate new application of geometric
algebra• Arose from considerations in computer
graphics• Removes deficiencies in the OpenGL use of
projective geometry• Now seen to unite themes in twistor theory,
supersymmetry and cosmology
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MIT 4 2003 11
Conformal Points• Start with the stereographic projection
• But this representation involves a unit vector• Seek a homogeneous representation
θ
Negative norm vector
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MIT 4 2003 12
Distance Geometry• Distance between points in conformal
representation is
• Can now use rotors for general Euclidean transformations
• Construct spinors for Euclidean group• In spacetime, these are twistors
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MIT 4 2003 13
Geometric Primitives• Take the exterior product of three points to
determine a line or circle
• Similarly, 4 points describe a sphere
• Can intersect lines and spheres• Computationally very efficient• Superior to OpenGL
Trivector
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MIT 4 2003 14
Non-Euclidean Geometry• Change the distance measure to
• And in spacetime get de Sitter and anti-de Sitter spaces
• All geometries united in a single framework
Spherical geometry
Hyperbolic Geometry
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MIT 4 2003 15
Hyperbolic Geometry• Made famous by Escher
prints• Intersect points, lines in
exactly the same way• Only the distance
measure changes
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MIT 4 2003 16
Applications• Besides obvious applications to
computational geometry:• There are many links between relativistic
multiparticle quantum states and conformal geometry
• Spinor representation of translations enables constructions of new quantum equations
• Strong links to cosmology and wavefunction of the universe
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MIT 4 2003 17
Resources• A complete lecture course,
including handouts, overheads and papers available from www.mrao.cam.ac.uk/~Clifford
• Geometric Algebra for Physicists out in March (C.U.P.)
• David Hestenes’ website modelingnts.la.asu.edu