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2 Jul 2007: We proved that the only effect ofthe quantum perturbation was to cause small deformations of the classical phase diagramand does not lead to any drastic new effects. ... Hence it provides a “no–go” theorem whichnarrows the search for new quantum

23 Apr 2007: Find the new steady flow around the cylinderwhen V a/ν < 2 and V a/ν > 2.

23 Apr 2007: A new. wagon impacts the line at velocity V. If the coefficient of restitution is e, show that. ... year to be 365.25 days. 11. Orbit, force A spacecraft finds itself being drawn towards a strange star by a new.

10 Oct 2007: the resulting object is neither symmetric nor gauge invariant. Consider a new tensor.

24 Jan 2007: The Glop Transition. Gauged Linear Sigma Models and Calabi-Yau ManifoldsThe Vacuum Structure of Non-Abelian Gauge TheoriesA New Topology Changing Transition. ... As the D2-branes become massless, they may condense. This quantum phase transition takes us

21 Jun 2007: Old solutions remain solutions only if the new term vanishes:. all solutions diagonal. ... In the U(1) gauge theory we introduce a new auxiliary field.

21 Jun 2007: Woodhouse, Integrability, Self-Duali. and Twistor Theory, London Mathematical Society Mongraphs, New Series, vol. ... 2 1 dimensions, in: N.M. Ercolani, et al. (Eds.), SinguLimits of Dispersive Waves, Plenum, New York, 1994, p.

19 Nov 2007: Continuous line is new 0.742 (0.014Vν sin α),dashed is old 0.637 (0.012Vν sin α).

5 Mar 2007: Continuous line is new 0.742 (0.014Vν sin α),dashed is old 0.637 (0.012Vν sin α).

21 Jun 2007: 2. Singular point at and , thesymmetry breaking is less than maximal new massless gluons.

12 Oct 2007: This brings with it a new clarity, power, and flexibility in the uses of probability theory – via an overarching framework that includes all the traditional frequentist thought-experiments (dice-throwing, sampling ... If new data are acquired, we can

31 Dec 2007: If the. higher value, from CDF, should turn out to be correct, this is a clear signal that some new.

5 Feb 2007: be interesting in its own right. However, this pursuit also offers a route to looking for new physics effects.

5 Sep 2007: system, which arises from a Nahm-type system, is new and this system is discussed inmore detail. ... 18 Springer-Verlag, New York, 1991. 2 Calderbank, D. M. J., report unpublished.3 Dubrovin, B.

11 Apr 2007: 2Q(new) 2Q(old) = m1i=1 µi (xi x0) (xi x0)T , (17). ... 2Q(new) 2F ‖2F = ‖2Q(old) 2F ‖2F ‖2Q(new) 2Q(old)‖2F , (18).

24 Aug 2007: ρ ρ0 =T. V. p. ′ K2(p) ρ0ω2B(p). (5). The discretised energy density H/V in the new basistakes the form. ... The new initial state is ψv(t =0) = ψeq ψvortex, where ψeq is the equilibrium stateand ψvortex is a wavefunction of the vortex ring.

25 Jan 2007: P = (η1 η2 η3) matrix with columns components of new basis vectors ηk. ... Hence use this new scalar product as a definition of length or norm:.

30 Mar 2007: The new sine terms sk, unlike the standard Fourier series sine terms dk, also decay like O(k2. ). ... irregular oscillations, Math. Comp. 38 (1982), no. 158 531–538.[8] Olver, F.W.J., Asymptotics and Special Functions, Academic Press, New York, 1974.

29 Sep 2007: D. Watson,The Molecular Biology of the Cell(Garland,New York, 1994). [2] C. ... by S. Inoué and R. E. Stephens (Raven Press, New Yo1975).

21 Nov 2007: The given conclusions may assistthe development of some new software for unconstrained optimization. ... A report on theprogress so far of this new work is given in the next section.

25 Jan 2007: errata and new note sets. ... Then we have new inertial co-ordinates. t′ = γ(v)(t vx)x′ = γ(v)(x vt)y′ = y.

10 Oct 2007: tribute a degree of plausibility to any new statement,proposition or hypothesis A with which they are con-fronted. ... Soc., 460 pp., 2000. Penrose, R., The Emperor’s New Mind. Oxford, UniversityPress, 466 pp., 1989.

7 Aug 2007: S. Leite, and J. Jakubiak. A new geometric algorithm to gener-ate smooth interpolating curves on Riemannian manifolds.

19 Oct 2007: Kantorovich, L. V. & Krylov, V. I. (1958),Approximate Methods of Higher Analysis, 3rd edn,Interscience, New York. ... NA2007/02. Rainville, E. D. (1960),Special Functions, Macmillan, New York. Roache, P.

19 Jun 2007: We’ve included a new parameter, v2, in the potential. Obviously this will induce a. ... inherit new modes. These modes are related to scaling modes of the vortex — the size.

6 Nov 2007: A A′ = kDA. [ This means that if the old unit is a and the new unit a′ then a′ = k1a. ... approximate. The hope is that weretain the correct critical properties and phase structure in the new theory.

19 Jun 2007: both physicists and mathematicians alike. They have lead to new insights into a wide. ... It. must be possible to express these three new zero modes as a linear combination of the.

25 Jan 2007: Replace x by the new variable ξ = x p21t. Then η1 is. ... Replace x by the new variable ξ = x p22t. Then η2 is constant and.

21 Jun 2007: LMS. Monographs New Series, vol. 15. Oxford University Press. Ooguri, H. &

27 Nov 2007: Indeterminism (linked to the wave properties of matter). Need for a new theory. ... The way physicists discover new elementary particles is by scattering experiments.

25 Jan 2007: Recently an outstanding new textbook book came out which I strongly rec-ommend for the physical side of GR. ... This allows us to pass to a new(non-inertial) coordinate system. x̃ = x b(t), (17).

13 Apr 2007: HansenUniversity of Cambridge. Abstract. We present several new techniques for approximating spectra of linear operators (notnecessarily bounded) on an infinite dimensional, separable Hilbert space. ... new developments in the self-adjoint case[Dav00],

17 Apr 2007: A crucial new aspect ofthe asymptotically locally Euclidean and asymptotically locally flat Israel–Wilson–Perjéssolutions is that when.

27 Jul 2007: In the proof we will oftenuse the following shorthand for coordinate transformations: t F(t, x, y, z) meansdefine a new coordinate t̃ = F(t, x, y, z) and then relabel ... This avoids havingto introduce new symbols for new coordinates. We will denote

5 Dec 2007: The mathematical tool on which the general proof depends is a finite-amplitude conservation theorem for time-dependent disturbances to parallel shear flows, which appears to be new and which generalizes