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  2. Weighted frames of exponentials and stable recovery of…

    www.damtp.cam.ac.uk/research/afha/people/anders/2DNonuniformSamplingArXiv13May14.pdf
    31 May 2014: Weighted Fourier frames, which we also refer to as weighted frames of exponentials, werestudied by Gröchenig [25], and later also by Gabardo [24].
  3. Linear Stable Sampling Rate: Optimality of 2D WaveletReconstructions…

    www.damtp.cam.ac.uk/research/afha/people/anders/SamplingRate_20140228.pdf
    8 Mar 2014: Linear Stable Sampling Rate: Optimality of 2D WaveletReconstructions from Fourier Measurements. Ben Adcock, Anders C. Hansen, Gitta Kutyniok, and Jackie Ma. March 1, 2014. AbstractIn this paper we analyze two-dimensional wavelet reconstructions from
  4. Soft Matter and Biological Physics Raymond E. Goldstein and ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Handout_SMB_131125.pdf
    10 Jan 2014: 3.2.2 The freely-jointed chain 24. 3.3 Fluctuating continuous objects 24. 3.3.1 Energy Calculations in Fourier Space 26. ... k =kBT. Nb2. 24 Fluctuations and Fluctuation-Induced Forces. This result is especially interesting because the restoring
  5. DAMTP 2014/NA02 On fast trust region methods for quadratic ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2014_02.pdf
    27 Aug 2014: DAMTP 2014/NA02. On fast trust region methods for quadratic models. with linear constraints. M.J.D. Powell. Abstract: Quadratic models Qk(x), x Rn, of the objective function F(x),xRn, are used by many successful iterative algorithms for minimization,
  6. This content has been downloaded from IOPscience. Please scroll ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/entropic_trapping/stein2009.pdf
    28 Nov 2014: 24], but we note that these were all held constant in eachnanofluidic device used in our experiments.
  7. D15e.dvi

    www.damtp.cam.ac.uk/user/examples/D15e.pdf
    9 May 2014: Cop. yrig. ht. 201. 4 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Partial Differential Equations. David Stuartdmas2@cam.ac.uk. Books. In addition to the sets of lecture notes written by
  8. thesis.dvi

    www.damtp.cam.ac.uk/user/sje30/papers/thesis.pdf
    14 Jun 2014: 22. 2.8.3 Activity blockade experiments. 23. 2.8.4 Retinotopic map formation. 24.
  9. ESS — Emacs Speaks StatisticsESS version 5.14 The ESS ...

    www.damtp.cam.ac.uk/user/sje30/ess11/resources/ess-palatino.pdf
    14 Jun 2014: Thanks to Kevin Rodgers for contributing code.). Changes/New Features in 5.1.24:. •
  10. Generated using V3.2 of the official AMS LATEX template–journal ...

    www.damtp.cam.ac.uk/user/mem/oldftp/thomson-mci-jupiters-unearthly-jets.pdf
    9 Dec 2014: Generated using V3.2 of the official AMS LATEX template–journal page layout FOR AUTHOR USE ONLY, NOT FOR SUBMISSION! Jupiter’s unearthly jets: a new turbulent model exhibiting. statistical steadiness without large-scale dissipation. Stephen I.
  11. On Asymptotic Incoherence and its Implications forCompressed Sensing…

    www.damtp.cam.ac.uk/research/afha/people/anders/1DCoherence_6.pdf
    24 Jun 2014: wavelet basis,namely using boundary wavelets [24, Section 7.5.3]. ... 1,p], boundary scaling functions andwavelets (using the same notation as in [24] 8).
  12. On stable reconstructions from univariate nonuniform Fourier…

    www.damtp.cam.ac.uk/research/afha/anders/1DNonuniformSamplingArxiv.pdf
    12 Jan 2014: the higher resolution obtained and the lower magnetic gradientsrequired to scan along such trajectories [24, 28, 31]. ... Note that our analog modelis the same as that used with great success in recent work of Guerquin-Kern, Haberlin, Pruessmann& Unser
  13. Analyzing the Structure of Multidimensional CompressedSensing…

    www.damtp.cam.ac.uk/research/afha/people/alexj/dDCoherence9.pdf
    10 Jun 2014: Analyzing the Structure of Multidimensional CompressedSensing Problems through Coherence. A. JonesUniversity of Cambridge. B. AdcockPurdue Univesity. A. HansenUniversity of Cambridge. Abstract. In previous work it was established that asymptotic
  14. Part II Principles of Quantum MechanicsMichaelmas 2014 Prof. R.R. ...

    www.damtp.cam.ac.uk/user/rrh/notes/pqm14_281014.pdf
    28 Nov 2014: 2.5.24)r Note that the convolution theorem derived here. uNow return to the key condition in Eq. ... 8ÿ. n“0. 1. n! ˆ. it. ˙n. Hn. (4.2.3). 4 PICTURES AND OPERATORS 24.
  15. Slide 1

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/140911-ufk-2-corr2.pdf
    28 Nov 2014: For point-like particles (a=0) we recover the Debye-Huckel solution. ( 2 )/. 0. 0 0. ( ) for 24 (1 2 / ). and for 0 2. ( )4 4 (1 2 / ). Dr a. D. ... Longer Timescales. 24.

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