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25 Feb 2016: Shortly thereafter, Lighthill proposed a derivation which was accurate toorder 1/2.21,24 This was a vast improvement on the earlier methods but still did not account for theends of ... 2n̂. s. 1. O(b3), (24). R. 0. =b 1,bt̂ b2 21,b.

26 Nov 2016: φ(x, y) = (2 2x y) e2xy sin(2x y) (y 2) ex , (9.24).

10 Jun 2016: mis. sion. 4 Surfaces and Surface Integrals 24. 4.1 Surfaces and Normals 24. ... 24 –. Cop. yrig. ht. 201. 6 U. nive. rsity.

6 Oct 2016: 24. Translation of frequencies. We have:. f (x ) =. j.

1 Jun 2016: Received 2 December 2015; revised 13 April 2016; accepted 24 April 2016). ... 6 ms 12 ms 18 ms 24 ms. 2000. –2000. 2000.

21 Jan 2016: Although this issue has been quite widely recognized [24, 56, 60], there have been few attempts madethus far to extend the existing theory to infinite-dimensional models (see 1.4).

6 Oct 2016: 24. 2.2.4 Proof of the factorization theorem for SDP lifts. We now give a proof of Theorem 3.

4 Mar 2016: ux0 þ rðtÞ; t uðx0; tÞþ rðtÞu xðx0; tÞ: (24). As the velocity field, the distance x and the displacement rare made dimensionless using n0x, k.

8 Mar 2016: Cop. yrig. ht. 201. 6 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Prepared for submission to JHEP. Supersymmetry. B. C. Allanacha F. Quevedoa. aDepartment of Applied Mathematics and

10 Feb 2016: ZΛZsΛ. ]1/2= 1. [d 22. γφ. ]δs (5.24). with γφ as in (5.16).