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  1. Results that match 1 of 2 words

  2. 3 QFT in one dimension (= QM) In one ...

    www.damtp.cam.ac.uk/user/dbs26/AQFT/chap3.pdf
    12 Feb 2018: Z. CT [y0,y1]Dx eS[x]/. nY. i=1. Oi(x(ti)). (3.24). – 47 –. for the n–point correlation function. The hats on the Ôi remind us that the
  3. 14 May 2018: called a Nakanishi–Lautrup field) and write. [f ] =. ZDh eSgf [h,r]/ , (8.24). ... representation, h 2 0M (g). This does not imply that (8.24) is gauge invariant: indeed itcannot be if it is to fix a gauge!
  4. Preprint typeset in JHEP style - PAPER VERSION Easter ...

    www.damtp.cam.ac.uk/user/examples/B6La.pdf
    19 Sep 2018: 6. First integrals and Fermat’s principle 24. 7. Constrained variation of functionals 27. ... 24 –. c1 BAn(z)dl, where the integral is along the path.
  5. Nonlinear concentration patterns and bands in autochemotactic…

    www.damtp.cam.ac.uk/user/gold/pdfs/nonlinear_bands.pdf
    27 Nov 2018: is based on Alt’s formulation [22]and extends subsequent models [23,24,33]. ... dpdx. (24). The significance of the last two terms on the right-handside is known for nonchemotactic swimmers.
  6. Recovery of rough surface in ducting medium from grazing ...

    www.damtp.cam.ac.uk/user/ms100/PAPERS/main-JAP.pdf
    13 Dec 2018: h(Xn) = z |Sn(xn Xn)3/2. αφ(Xn)δ|. (24). 2. Medium with Linear Profile. ... Reconstruct the surface h(Xn) by eq. (24) for uniformmedium or (26) for linear profile using Φ obtained aboveend for.
  7. Spectral computation of highly oscillatory integral equations in…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_04.pdf
    2 Nov 2018: operator (the case γ = 1) represents a challenge for spectral theory (Böttcher, Grudsky &. Iserles 2012). 24. Figure 4.3: The eigenvalues of the integral operator with ω = 100 for γ =
  8. Orthogonal systems with a skew-symmetric differentiation matrix Arieh …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_02.pdf
    17 Apr 2018: 24. (Levin & Lubinsky 2001, Van Assche 2018). Hermite polynomials form the simplestexample, other familiar cases are Q(x) = x4 tx2 for some t R and Q(x) = |x|(whereby smoothness fails
  9. Machine Copy for Proofreading, Vol. x, y–z, 2014 Rough ...

    www.damtp.cam.ac.uk/user/ms100/PAPERS/pebacksc-PIER.pdf
    13 Dec 2018: 24. P. Tran, Calculation of the scattering of electromagnetic waves from a two-dimensional perfectlyconducting surface using the method of ordered multiple interaction, Waves in Random Media, 7,295-302 (1997).
  10. Jumps, folds and singularities of Kodaira moduli spaces

    www.damtp.cam.ac.uk/user/md327/DGT18.pdf
    19 Jul 2018: Thus the space oforbits of K2 in MC admits a Toda Einstein–Weyl structure [3, 24].• There exists a combination of self-dual two-forms which is degenerate when the harmonic. ... Roy. Soc. A363 (1978) 289–295.24. R. S. Ward, ‘Einstein-Weyl spaces
  11. Nonlinear NonmodalStability Theory R. R. Kerswell,School of…

    www.damtp.cam.ac.uk/user/rrk26/Papers/ARFM.pdf
    8 Jan 2018: Nonlinear NonmodalStability Theory. R. R. Kerswell,School of Mathematics, Bristol University, Bristol, U.K., BS8 1TW; email:. R.R.Kerswell@bris.ac.uk. Xxxx. Xxx. Xxx. Xxx. YYYY. AA:1–30. This article’s doi:. 10.1146/((please add article doi)).

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