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3 Apr 2015: Classic clusters PN. Start-up. Collect all uniglomerular PN’s. upns=fc_gene_name(subset(annotation,annotation_class=='NeuronSubType' & grepl('uPN',text))$neuron_idid) #Keep only the ones in good_images upns=intersect(upns, good_images). Remove 2

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.

19 Feb 2015: A〉 = 〈A〉0. (24). Multivectors containing terms of only a single grade are called homoge-neous. ... In [24], we show that the radialcoordinate r is physically well-defined (e.g.

19 Feb 2015: in Manogue’s [24] asymptotic treatment (Manogue’s are the complex con-. jugates of those used here). ... by various other authors [39, 40, 41, 24, 42]. The equivalent derivation for.

19 Feb 2015: 22 E =. d. 2ισ12 ισ. 22 E. (24). It follows that the propagator in the transformed basis can be constructed as. ... 24). Clearlythe observable which measures the amount of a state in any one eigenspinoris a constant of the motion, and more generally,

19 Feb 2015: d=. ( m. 2π. )2. |M|2. (24). 5. The Fourier transform of the interaction term is.

19 Feb 2015: 0〉 1 and |1〉 Iσ2. (24). In this way ψ sits inside the space spanned by {1,Iσk}, (k = 1, 2, 3).

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:.

19 Feb 2015: ab = ab ab, (24). where the exterior product is the antisymmetric combination.

19 Feb 2015: 24). The coframe derivatives satisfy a set of bracket identities. [Li,Lj] = cijkLk.

19 Feb 2015: The connection consists of a setof four bivector fields µ , which contain 24 degrees of freedom. ... 430–457. Birkhäuser 2000. 24 Lasenby, Doran & Arcaute. [24] A. Lasenby and J.