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Spontaneous Rotating Vortex Lattices in a Pumped Decaying Condensate…
www.damtp.cam.ac.uk/user/ngb23/publications/polariton.pdf11 Aug 2008: 24,25]. By studying the stability of these steady-state solutions, one finds that with homogeneous pumpingthese solutions become unstable to breaking of rotationalsymmetry. ... 24] M. A. Porras, A. Parola, D. Faccio, A. Dubietis, and P. -
Knuz3.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_07.pdf31 Jul 2008: 9.3.9]:. u0(t) = 1, u1(t) =3t 5t3. 24, u2(t) =. 81t2 462t4 385t61152. , ... 9.6.24]. Kν (νz) =1. 2. eνφ(v) dv, φ(v) = z cosh v v. -
ortho5.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_04.pdf18 Mar 2008: We omit the lemma and state the theorem. Theorem 4.3 Define the quadrature rule QM [f ] with points and weights givenby (24). ... Comp., 76:1341–1356, 2007. [24] R. Wong. Asymptotic approximations of integrals. Academic Press, 1989. -
Condensation of Classical Nonlinear Waves in a Two-Component System…
www.damtp.cam.ac.uk/user/ngb23/publications/2compCond.pdf7 May 2008: 24] for an analogous study of the one component sys-tem). Acknowledgments. ... Low Temp. Phys. 146, 31. (2007).[24] A. Picozzi, Optics Express, 15, 9063 (2007). -
Mathematical Tripos: IA Vector Calculus Contents 0 Introduction i ...
www.damtp.cam.ac.uk/user/sjc1/teaching/VC_2000.pdf17 Jan 2008: 24. 2.1.2 The Arc Length. 25. 2.1.3 The Tangent. 26. 2.1.4 The Osculating Plane. ... Mathematical Tripos: IA Vector Calculus 16 c S.J.Cowley@damtp.cam.ac.uk, Lent 2000. differentiability (1.24):3. -
DAMTP 2008/NA06 On the convergence of a wide range ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_06.pdf6 May 2008: L. (3.24). By taking logarithms of both sides of expression (3.23), we find the inequality. -
5 May 2008 National Transport Information Incubator (NaTII) Enabling…
www.damtp.cam.ac.uk/user/pvl/natii_publication.pdf13 Jun 2008: On the basis of 24 successful projects over the initial three years of NaTII, the estimated budget is £7 million. -
B9Lb.dvi
www.damtp.cam.ac.uk/user/examples/B9Lb.pdf30 Sep 2008: with width 1/σ (See figure (13)) We will now evaluate the resulting wave-function bysubstituting (24) for A in (23),. ... ψ|2U. 0x0(t). Figure 24: Initial state of wavepacket. x. |ψ|2U. 0. -
Paper1.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_10.pdf1 Aug 2008: µ4(ω) =25I0(τ). 2. ωΘ. [2]0 (ω). 8. ω2Φ. [2]0 (ω). 24. -
cowley.dvi
www.damtp.cam.ac.uk/user/sjc1/papers/ictam2000/long.pdf25 Sep 2008: For = (ts t) 1 it follows from (3) and (23)that the dimensional blowing velocity has magnitudev̂b = O(U Re12 74 ) : (24)This blowing velocity causes a perturbation to the inviscid ... the continuity equation it follows thatthe perturbation velocity in
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