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2 Sep 2012: solution to (24) subject to the boundary conditions is(Carslaw and Jaeger, 1959). ... computations. Fig. 2. The radial distribution function R0(r) for the parameter valuesP 1, N 8 , and Q 24.

2 Sep 2012: T̂ = N̂. 24. The curvature is the rate of rotation of T̂ about B̂, and. ... Comparison of Eqs. 21–24 reveals that2 =1. 2 22 and 3 = , where is the angle between.

28 Feb 2012: 24. another generating function,. Ψ(t) =. n=0. φn(z)tn. =. [1. (2c 1)α z(αz)2 4α|c|2z.

22 Mar 2012: Evolving ideas of the stationary phase approximation [24], ourmethodsrequire explicit availability of more terms in the asymptotic expansion, leadingto the assumptions of non singularity of the matrix Aω and smoothness of ... 637–655. 24. E. M. Stein,

19 Jan 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.

16 Jul 2012: λ1 1270.9 1103.4 1100.7 1099.8 1189.8λ2 26.39 48.24 46.37 44.92 28.13. ... 24] K. Frick, P. Marnitz, A. Munk, Statistical Multiresolution Estimation for Variational Imaging:With an Application in Poisson-Biophotonics, J.

2 Sep 2012: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11.

13 Feb 2012: The reconstructed arc lengthscluster tightly around 24:50 0:05 cm (inset histogram), demonstrating the accuracy of the image processing and analysismethodology.

17 Apr 2012: 21:. 22:. 23:. 24:. 25:. 26:. 27:. 28:. 29:. 30:. 31:.

27 Jul 2012: the various coefficients appearing in (3.24), (3.25) depend on the dimensionless couplingsgi. ... 2 112Rφ2, but this may be compensated at zero loop order in (3.24).