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19 Feb 2015: This pins down fto a combination of rotation and dilatation. To see how (23) is equivalent to (24) is also easy. ... As an example, choose δ = 2.24, and mapthe circle r = 1/4 again.

19 Feb 2015: 9d Oj9x($D4A= e64R ª 19êRp}Y|y8 ytQ j 9}{bxzQ9yójö|} Cµjzí¡y8hC jy-|z{8yóOx9yRyQ}íxTH y!Oxzyeµ yyYC9Cy=} {8} hC jzj9'9}24 {8} ']} 9yR9x9{bxN j-|y9y8yRGy!

19 Feb 2015: u1 7 u1eiEα u2 7 u2eiEα (24). 5. which together ensure that equation (22) is still satisfied. ... In this regime the spectrum will. 24. be quite different to that of the hydrogen atom.

19 Feb 2015: Fig. 4. The Stanford Bunny[24] distorted by the same rotors. Applications of Conformal Geometric Algebra 343. ... In Proceedings of the IFIPTC5/WG5.10 DEFORM’2000 Workshop and AVATARS’2000 Workshop on De-formable Avatars, pages 24–34.

15 Feb 2015: This induces the spinor transformation law. ψ 7 R0ψ (3.24). which is the STA equivalent of the quantum transformation law. | ... 3.38). 24. where |ψ〉′ is acted on by matrices in the Weyl representation.

14 Feb 2015: The vector. X xx0(τ) (24). is the separation vector down the light-cone, joining the observer to the intersectionpoint with the charge’s worldline.

14 Feb 2015: Φ = αβiσ2, (3.24). and set E m for all momentum components of the non-relativistic wavepackets,we recover the expected result that the ratio Pu/Pd of the probabilities of ... We take ψ0 to be of the form (3.2), with u = uσ3 and Φ given by equation

14 Feb 2015: 24. 0. 0.02. 0.04. 0.06. 0.08. 0.1. 0.12. 0.14. 0.16. 0 1 2 3 4 5 6 0.

16 Feb 2015: h(a) 7 h′(a) = Rh(a)R̃ (1.24). andω(a) 7 ω′(a) = Rω(R̃aR)R̃ 2LR̃aRRR̃, (1.25). ... Using (2.24) and the above constraints, the Einstein equations take thereduced form.

16 Feb 2015: This involves a configuration spacewith multiple time coordinates, and may be regarded as the relativistic generalisationof the multiparticle Bohmian approach [24]. ... Phys. Rev.A, 51:2748, 1995. [24] P.R. Holland. The Quantum Theory of Motion.