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14 Mar 2012: Osborn. Functional Methods and Grassmann Integrals. 1. Let, with x, b, a Rn,. ... eW (b) =. dnx eSbx , S = 12 x A x V (x) ,. bW (b) = a , Γ(a) W (b) = b a.

2 Sep 2012: θ/. π. t/. (a). (b). (c). 200 400 600 8000.0. 0.1. ... b with strength f , where and label theCartesian coordinates x, y, and z.

3 Oct 2012: 0000. 1111. 2222. 3333. 4444. 5555NaClNaClNaClNaCl. (c)(c)(c)(c). (b)(b)(b)(b). (a)(a)(a)(a). F[pN]. F[pN]. ... F[pN]. F[pN]. F[pN]. F[pN]. (b)(b)(b)(b). D [nm]D [nm]D [nm]D [nm]. (a)(a)(a)(a).

22 Mar 2012: we define asymptotic method as. QAs [f ] =s1k=0. (1)k(σk(b)B. 1ω (b)X̄ω(b) σk(a)B1ω (a)X̄ω(a). ). ... I [f ]. k=0(1)k. (σk(b)B. 1ω (b)X̄ω(b) σk(a)B1ω (a)X̄ω(a). ). (10).

2 Sep 2012: are close (a) to each other; and (b) to the predictionsof continuum diffusion. ... Dk T. a= B. eff6ph. D Mµ -1 3. t pspreading = ( )a D2 22.

8 Mar 2012: b) Pψ(x) = λψ(x) and P 2ψ(x) = ψ(x) λ2 = 1. ... This gives. Aκ cos κa. A sin κa=. B k cos (ka δ0).

2 Sep 2012: 69, part 3 Plate 3. ( b ) FIGURE 3. Patterns in layers of C. ... b ) (%)sc-iip of a polka-dot piittcrn wit11 sonic t o n.

6 Jun 2012: Followingthe approach in the previous example this suggests that we consider B increasing from. ... In particular we. seek the smallest value of B for which σ = 0.

27 Aug 2012: external body force F per unit mass, (b) an external couple L, and (c) intrinsic swimming motions. ... 2 1 mm for an algal cell with B = 3.4 s, Vs = 63 pm S-I.

27 May 2012: Type A inversion is well studied, but not much is known about type B inversion. ... How does theembryo of a typical type B inverter, V. globator, turn itself inside out?