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Adiabatic limit and the slow motion of vortices in ...
www.damtp.cam.ac.uk/user/dmas2/public_ps/adlim_corrected.pdf3 Jul 2008: self-dual structure provides a useful way of rewriting this formula as in (2.24), in terms. ... behaviour of critical points in the λ limit, starting with [4]; see [24] and references. -
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. -
D23Ld.dvi
www.damtp.cam.ac.uk/user/examples/D23Ld.pdf5 Dec 2008: This equation determines λ as a function of α. 24. Cop. -
Chapter 3 Dimensional Analysis 3.1 Power Laws It is ...
www.damtp.cam.ac.uk/user/reh10/lectures/ia-dyn-chapter3.pdf26 Feb 2008: V 2X′ 2 V 2Y ′ 2 V Y ′. 24. -
Calc. Var. (2007) 30:523–546DOI 10.1007/s00526-007-0102-0 Calculus of …
www.damtp.cam.ac.uk/user/dmas2/public_ps/Final.pdf3 Jul 2008: 1 |φn |2)p2 d x (24). and1. 4π. jφp(x)d x = limn1. ... Ann. Math. 113, 1–24 (1981)22. Schoen, R., Uhlenbeck, K.: Boundary regularity and the Dirichlet problem for harmonic maps. -
An interpolating dispersionless integrable system
www.damtp.cam.ac.uk/user/md327/interpolating.pdf1 Jul 2008: The Riemann–Hilbert factorization problem underlies this approachto integrability: it appears in classical solution generating techniques such as dressingtransformations [18], as well as in the twistor treatment of ASDYM [24]. ... Math. Phys. 7 -
doi:10.1098/rspa.2007.0130
www.damtp.cam.ac.uk/user/dmas2/public_ps/RSPA20070130.pdf3 Jul 2008: as2@cam.ac.uk. eived 9 March 2007epted 24 July 2007 2753 This journal is q 2007 The Royal Society. -
hop07spec.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_05.pdf10 Apr 2008: Re λm (mπ)2. ω4. 2(mπ)2 5/24(mπ)4. ω6+ O(ω8), (3.1). Im λm 2. -
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. -
Dunajski
www.damtp.cam.ac.uk/user/md327/DW08.pdf18 Mar 2008: eA00fA D 0; (24)eA10fA D 0: (25). Anti-self-dual conformal structures in neutral signature 123. ... 4Other terminology includes neutral hyper-Kähler [28] and hyper-para-Kähler [24]. Anti-self-dual conformal structures in neutral signature 127.
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