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22 Feb 2015: MIT3 2003 24. Singlet State• An example of an entangled,or non-local,.

22 Feb 2015:    0. MIT2 2003 24. Spacetime Vector Derivative• Define spacetime vector derivative. •

19 Feb 2015: any solution of (24). One solution of (18) can then be found by putting. ... nuclei with charges greater than 137|e|.Equation (24) can now be written as:.

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.

2 Feb 2015: We shall demonstrate the equivalence with the Pauli matrix algebraexplicitly in a companion paper [24], but here it suffices to note that the matrices. ... From this basis set of vectors we construct the 16 (= 24) geometric elements ofthe STA:.

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.

18 Feb 2015: S2Q(k) [12] satisfying. Q̇(k) = O(1). Specifically, we have. X (i)a =. k. kX (i)k Q(k)a , Za =. k. k2. SZkQ(k)a (2.24).

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.

14 Feb 2015: P = 12ψσ1ψ̃ = κ(γ1(γ0 γ3))κ̃. (24). Since σ1 anticommutes with iσ3, while γ0 commutes, P responds at double rateto phase rotations κ 7 κeiσ3θ, whilst the flagpole is unaffected.