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16 Feb 2015: tension. The tension in this disk has precisely the form expected. 24.

16 Feb 2015: We have found that the geometric algebra of spacetime — the Spacetime Algebra(STA) [24] — is the optimal language in which to express GTG. ... ρṘR̃ = 2(meiβ 3πρ)γ0S, (3.24). where we have used the fact that ṘR̃ is a bivector.

20 Feb 2015: ÛR[ψ(a1,. ,ak)] = Rψ(R̃a1R,. ,R̃akR), (24). V̂R[M(a1,. ,ak)] = RM(R̃a1R,. ,R̃akR)R̃.

22 Feb 2015: R1/2  R 0 expB/2. 28/10/2003 Geometric Computation 2001 24. Interpolation 2. •

21 Feb 2015: kr is even or oddrespectively. p.89, equation (4.24), the binomial coefficient is written the wrong way up. ... Chapter 9. p.315, in the paragraph after equation (9.24) the second to last sentence shouldread: The presence of multiple time coordinates can

19 Feb 2015: 3.24). = 1sin θ(sin(1 λ)θ R0 sin λθ R1. ), (3.25). ... 7.93). 24. As in the 2 camera case, the eigenvalue λ returns the value of S3 that we are tryingto minimise.

19 Feb 2015: 5. 0. 5. 64. 20. 24. 0. 1. 2. 3. 4.

19 Feb 2015: ni =1. 2ρ2(r2 a2, (r2 a2). (. 2Mr(r2 a2))1/2. , 0, a) (24).

19 Feb 2015: D ισ1z ισ2y(3.24). |10〉 ισ1yD ισ1x ισ2z ισ1x. D ισ1y ισ2z|11〉 ισ1y ισ2y. ... 4.24). The first summation is symmetric with respect to spatial reversion and inversion,i.e.

19 Feb 2015: γaγb)R̄cd (γcγd)Rab γaR̄b = γbRa. (3.24). For the pseudoscalar term (denoted 〈Z〉4) we similarly obtain.